Device, accelerator, decelerator, nuclear conversion system, light source device, light exposure device, propulsion device, centrifugal force device, material pressurizing device, and high-pressure induction superconduction experimenting device

Abstract

To study a system that transmutes atomic nuclei using muons, devise a light source device and a propulsion device including a nuclear transmutation system, and examine a centrifugal force application unit which may be accelerated by the propulsion device, and devise an electric field generator or a magnetic field generator.SOLUTION: A system is devised that decelerates cosmic muons produced from cosmic rays or high-speed muons derived from mesons produced from atomic collisions with electric field and deceleration means and uses the muons for nuclear transmutation. Also, a decelerator using a laser wake field and a decelerator using an element forming an electric field are proposed. A radiation light source having the nuclear transmutation unit is disclosed. An ionization device, a centrifugal gun device, a centrifugal force and pressure applying device, a pressure generation unit, a pressure applying material, a high-pressure induction superconductivity experimenting system, a magnetic device, and a magnetic sail are disclosed.SELECTED DRAWING: Figure 18

Description

Technical Field

[0001] <Incorporation by Reference> This invention This application claims the benefit of priority to Japanese Patent Application No. 2023-174791, filed on October 6, 2023, the entire disclosure of which is incorporated herein by reference in its entirety. This application claims the benefit of priority to Japanese Patent Application No. 2023-174037, filed on October 6, 2023, the entire disclosure of which is incorporated herein by reference in its entirety. This application claims the benefit of priority to Japanese Patent Application No. 2023-174 180, filed on October 6, 2023, the entire disclosure of which is incorporated herein by reference in its entirety. This application claims the benefit of priority to Japanese Patent Application No. 2023-196029, filed on November 17, 2023, the entire disclosure of which is incorporated herein by reference in its entirety. This application claims the benefit of priority to Japanese Patent Application No. 2024-011 380, filed on January 29, 2024, the entire disclosure of which is incorporated herein by reference in its entirety. This application claims the benefit of priority to Japanese Patent Application No. 2024-065053, filed on April 14, 2024, the entire disclosure of which is incorporated herein by reference in its entirety. This application claims the benefit of priority to Japanese Patent Application No. 2024-072096, filed on April 26, 2024, the entire disclosure of which is incorporated herein by reference in its entirety. This application claims the benefit of priority to International Application No. PCT / JP2024 / 016620, filed on April 28, 2024, the entire disclosure of which is incorporated herein by reference. This application claims the benefit of priority to Japanese Patent Application No. 2024-082974, filed on May 22, 2024, the entire disclosure of which is incorporated herein by reference. This application claims the benefit of priority to Japanese Patent Application No. 2024-122 912, filed on July 29, 2024, the entire disclosure of which is incorporated herein by reference. <Technical Field> The present invention is an invention related to nuclear power. The present invention relates to a muon-catalyzed fusion system. (An application based on an idea that requires verification) The present invention includes inventions related to devices and systems. It includes inventions related to accelerators, decelerators, nuclear conversion systems, light source devices, exposure devices, propulsion devices, centrifugal force devices, material pressurization devices, and high-pressure-induced superconducting experimental devices.

Background Art

[0002] The muon-catalyzed fusion method (muon-catalyzed fusion) is known as in Non-Patent Document 1.

[0003] Hydrogen molecules containing deuterium D or tritium T are used as a liquid, and muons are introduced therein, and the muons act like a catalyst for nuclear fusion to cause a nuclear fusion reaction. However, in hydrogen molecules, the charge of the nucleus after nuclear fusion increases from +1 of the hydrogen atom to +2 of the helium atom, and the muon is Coulombically captured and trapped by the nucleus with a +2 charge, the helium nucleus, the alpha particle nucleus, and the muon-catalyzed fusion stops (making the reaction difficult).

[0004] According to Non-Patent Document 2, a thermonuclear fusion method using protons and boron is known. In a thermonuclear fusion reactor, high-energy neutron rays that can activate the fusion reactor in D-T and D-D reactions are a problem. As an example of solving this problem, a system using protons and boron that does not emit neutrons and is difficult to do so (P-11B system, proton-boron system) has been studied. When performing the P-11B system in a thermonuclear fusion reactor, there was a problem that the temperature at which thermonuclear fusion occurs needs to be 10 times higher than that of the D-T system.

Prior Art Documents

Patent Documents

[0005]

Non-Patent Document 1

Non-Patent Documents

[0006]

Non-Patent Document 2

Summary of the Invention

Problems to be Solved by the Invention

[0007] <Problem> In the system of muon-catalyzed fusion using hydrogen atoms and hydrogen molecules, there is a problem that muons are captured and trapped by the Coulomb force, causing the muon-catalyzed fusion to stop (making the reaction difficult). Also, in systems using deuterium D, tritium T, etc. in muon fusion, neutrons that may activate the members of the fusion reactor or fusion system are generated. However, there may be a system that does not generate neutrons. <0033><Problem> In known muon-catalyzed fusion, there was a problem that muons were attached, captured, and trapped by helium, which is a product substance after fusion rather than a fusion fuel substance such as hydrogen, deuterium D, or tritium T, causing the catalytic fusion to stop. We want to solve the problem that the muon-catalyzed fusion reaction is difficult to proceed because muons are captured by the product substance after fusion rather than the fusion fuel substance. Also, we want to devise a system that is less likely to generate neutrons. <0059><Problem> In known muon-catalyzed fusion, there was a problem that muons (muons) were attached, captured, and trapped by helium, which is a product substance after fusion, in fusion fuel substances such as hydrogen, deuterium D, or tritium T, causing the catalytic fusion to stop. We want to solve the problem that the muon-catalyzed fusion reaction is difficult to proceed because muons are captured by the product substance after fusion rather than the fusion fuel substance. <0060><Problem> We want to make it easier to replace the muon target without stopping the muon fusion reactor. (We want to reduce the downtime during target replacement. We want to increase the target life.) Also, we want to miniaturize the muon generation section and the accelerator. <0061><Problem>The problems to be solved by the invention <Problems of reduction of activation and replacement maintenance of the muon target and downtime when muons cannot be generated> When generating muons, an accelerated high-energy proton beam is irradiated onto a muon generation target section made of carbon or lithium, and pions, pions, and muons are generated. At this time, the pion-muon generation target section and muon target that are irradiated with the proton beam deteriorate and become activated as they are used, and replacement is necessary. The target becomes highly activated to a level where it is difficult for humans to approach. Replacing the muon target has been a problem of stopping the muon generation device and the muon fusion system. Therefore, a rotating muon target has been developed in which the irradiated time is dispersed and averaged to other parts of a rotatable disk by rotating the target section. Also, in a muon fusion system, if replacement and maintenance of the muon target can be performed without stopping the muon generation section during operation of the muon fusion system (· downtime when muons cannot be generated can be reduced), it may be commercially preferable (for example, a muon fusion power plant does not need to stop power generation for a span of once every six months, three weeks, etc. for muon target replacement). <0066><Problem><Miniaturization of the device for generating muons, necessity of a small accelerator and a small muon generator> It is preferable to miniaturize a system for generating muons (accelerator, accelerating cavity, deflection magnet). When it is desired to mount the fusion system on a transportation device, a spacecraft, a spaceship, an aircraft, a vehicle, a ship, a submarine, various facilities, or robots, it is preferable that the size of the system including the accelerator and the muon generation device can be reduced. <0077><Problem>When using a target made of a carbon material or bulk carbon using carbon atoms for the muon target, there is a problem that the carbon atoms are highly activated through high-energy proton irradiation. Also, there may be the same problem when using beryllium or lithium for the target. It is desired to devise a system in which the muon target is less likely to become activated. Also, although the muon target undergoes a knockout reaction, the nucleus in the target is converted into alpha rays or the like and escapes, increasing voids and becoming brittle and unusable, and target replacement is necessary. However, it is desired to devise a system that reduces the load and man-hours of target replacement. <0082><Problem>Consider a device for decelerating muons. It is desired to decelerate muons from cosmic rays originating from natural cosmic rays over a large area. It is desired to decelerate muons obtained from mesons obtained by artificial device means such as colliding particles accelerated by an accelerator.

Means for Solving the Problem

[0008] In muon-catalyzed nuclear fusion, it is desired to bring a muon close to a hydrogen atom, which is a fuel substance before nuclear fusion, and cause nuclear fusion. However, the helium nucleus of the nucleus after nuclear fusion has an increased charge compared to the hydrogen nucleus of the nucleus before nuclear fusion, making it easier to capture the muon. Therefore, in the present invention, as a system for reversing the change in charge, a system using a proton and boron is disclosed as Example 1 in FIG. 1. Also, an assumed example of a spaceship 3 and a transportation device 3 equipped with it is shown in FIG. 5. <0033><Problem><Solution Means>In muon-catalyzed nuclear fusion, when nuclei fuse, a nuclear fusion reaction system is used that has the characteristic that the charge of the nucleus of the substance generated by nuclear fusion is smaller than the charge of the nucleus of the atom that becomes the nuclear fusion fuel. Specifically, a muon-catalyzed nuclear fusion system using a proton and boron, or diborane containing a proton as a hydrogen molecule and boron as nuclear fusion fuel is proposed. <0027>In FIG. 1, a proton is irradiated onto boron. However, as shown in FIG. 6, borane, diborane B2H6, or boron hydride in which boron is pre-bonded to a proton and a hydrogen atom may be used for the target part T1. For example, liquefied liquid diborane may be used for the nuclear fusion fuel F1 or the target T1 part. In the system of FIG. 6, since diborane containing hydrogen and a proton is used, there may be an advantage that the proton introduction part P1 described in FIG. 1 and the like becomes unnecessary. <0028>FIG. 7 shows a system 1F-SYS-RAM in which diborane is pressurized, compressed, circulated, irradiated with muons, and caused to undergo nuclear fusion. (FIG. 7 is one of the embodiments of FIG. 6.) FIG. 7 is an assumed view when the system using the diborane of the present application is applied to a system in which a nuclear fusion fuel fluid having a known ramjet part circulates in a closed loop system. <0029>The diborane within the 1F-SYS-RAM system in FIG. 7 is pressurized and compressed by a compressor PUMP and circulated. The pressurized fluid diborane is further compressed by the compression device section RAM to form a compressed BH1 section (PBH1 section). Muons are irradiated from the muon irradiation section M1 onto the PBH1 to promote nuclear fusion. (Since diborane is compressed, its density increases, making it easier for muons to come into contact, proximity, and interaction, and it is expected that the catalytic nuclear fusion reaction will occur more easily.) <0030>In the 1F-SYS-RAM system of FIG. 7, there is an advantage that both protons and boron can be supplied to the system as diborane in which hydrogen and boron are bonded. The proton introduction section P1 is unnecessary, and it is also possible to add fuel to the system and remove He (degas) from the system. (Utilize the feed control section FEEDC such as the helium He removal section and the diborane fuel supply section, etc.) <0031>Also, considering the ease of contamination by impurities with an atomic number larger than that of boron, gaseous diborane that can be purified may be better than solid boron. (Solid boron requires generation, purification, and refining as a solid crystal.) As described by taking sodium borohydride NaBH4 as an example in paragraph 0024 of the present application, the present application considers the presence of atoms, nuclear fusion products EX1, or impurities in the fuel with an atomic number larger than that of the nuclear fusion fuel to be unfavorable. *Although the system of proton-boron nuclear fusion is shown as an example, to avoid limiting the scope of the invention, when more generally disclosing the conditions of the present invention, it may be sufficient if it is a system in which the charge of the substance generated when atomic nuclei fuse is smaller than the charge of the atoms that become the nuclear fusion fuel. (And there may also be a system in which neutrons are not generated or are difficult to generate.)

[0009] <0060><Problem><Solution>In a circular accelerator (fixed magnetic field strong focusing accelerator FFAG accelerator, MERIT ring · MERIT accelerator * MERIT: Multiplex Energy Recovery Internal Target), a movable target in the form of a wedge or a thin disk · plate (insertable) is used. The movable target may be replaceable by a replacement device, or two or more movable target parts and solenoids for muon capture · muon extraction parts may be provided so that the movable target part can be moved in and out and back and forth (at the MOVE position in Fig. 12) from the outer periphery to the inner periphery of the accelerator. A proton particle beam may be irradiated onto the movable target to generate pion muons. <0062><Solution> <Means for Solving the Problem> <Mode for Carrying Out the Invention> <Muon Target Lifetime Extension and Downtime Reduction by Rotating Muon Target MU-DISK-TGT>In a circular accelerator 2MU-ACC-RING (FFAG accelerator 2MU-FFAG, MERIT ring · MERIT accelerator 2MU-MERIT-RING), (especially in the MERIT-type ring), a muon target part arranged to protrude in a wedge shape, which is a thin and sharp (sharp-shaped and protruding in a wedge shape) pharmaceutical research vehicle-type rotating target part on the outer periphery, or a record disk · disk-shaped rotating target part MU-DISK-TGT whose outer periphery is thin, thin, and sharp like a rotary saw (the thin and sharp disk at the tip of the outer periphery in FIGS. 10, 11, and 12, or the wedge-shaped rotating muon target MU-WEDGE-DISK-TGT in a wedge shape). By doing so, the activation of the MERIT-type wedge muon target (fixed muon target) is suppressed and averaged, the lifetime of the muon target is extended, the activation is delayed, and an attempt is made to increase the available time of the muon target. ※For example, the rotating muon target MU-WEDGE-DISK-TGT · MU-DISK-TGT in FIGS. 10, 11, and 12, which may be a wedge · triangle with a thin cross-section on one side of the disk facing the outer peripheral direction (or a thin disk), and a movable muon target unit (2MU-GEN-ROT-TGT) equipped with rotating means such as a motor for rotating the rotating muon target and rotating support means such as bearings may be configured. The muon target part MU-MOVABLE-TGT · MU-DISK-TGT may be inserted (· pulled out) into the particle beam orbit part of the accelerator (2MU-FFAG, 2MU-ACC-RING, 2MU-MERIT-RING) toward the particle orbit on the outer periphery of the accelerator. The rotating muon target part 2MU-GEN-ROT-TGT may be provided in the target part · pion muon generation part of the muon generation device 2MU. (※Regarding the circular accelerator as a donut shape, a rotating muon target like a rotary saw in the poloidal direction can be inserted, pulled out, and moved in the part where the particles circulate on the outer periphery of the donut · the protruding part of the wedge of the MERIT ring. A rotating target that can cut or pull out with a rotary saw in the ring can be inserted and removed from the 2MU-MERIT-RING in FIGS. 10 and 12.))※As shown in Fig. 10, a wedge-shaped rotating muon target MU-WEDGE-DISK-TGT, or a rotating muon target MU-WEDGE-DISK-TGT with a thin plate-like movable part (the target MU-WEDGE-DISK-TGT may be rotatable, and the shape of the target may be such that after the particle beam of the MERIT method hits the target, the particles can regain energy again inside the MERIT ring circular accelerator, and the shape may be wedge-shaped, with the part protruding into the ring part being thin, i.e., a thin plate shape.※In Fig. 10, the rotating muon target MU-WEDGE-DISK-TGT (with a wedge shape and a shape with a thin part) is inserted into a part of the outer peripheral side of the accelerator cross-section (so as to collide with the orbit of the particle beam accelerated and orbiting the outer periphery) and is rotatable, like a rotary saw that cuts the outer peripheral side through which the particles pass perpendicular to the toroidal direction of the circular accelerator, circular accelerator, FFAG, and toroidal shape (donut shape) of the MERIT ring in a vacuum. In Figs. 10, 11, 12, and 13, the operation and rotation of the particle accelerator or the insertion and movement (MOVE) of the rotatable or movable muon target may be possible while maintaining a vacuum, and the replacement (EXCHANGE·SET) of the movable muon target may be possible. Motors (MU-TGT-MOT) and bearings (MU-TGT-BRG) are used for rotation. The wedge-shaped rotating muon target MU-WEDGE-DISK-TGT attached to the axis (AXIS-TGT-BRG) rotates across a part of the outer periphery of the circular accelerator, FFAG, and MERIT ring (a part of the outer peripheral side of the ring donut). *Cross-sectional view CS part of Fig. 10, cross-sectional part CS from point CSP1 to CSP2.)

[0010] <Replacement during the activation of the muon target and removal of the activated part> Also, when the wedge-shaped rotating muon target is activated as shown in the right figure of Fig. 11, the activated tip can be cut, sliced, or severed to remove the activated part, and the less activated part can be recycled and used again. Also, machines or robots may be used for unmanned operation. In the case of a rotating muon target, compared with a fixed target or a thick rotating target, the part near the wedge or the thin part will be activated, and the thickness and volume of the location irradiated by the proton ion beam can be reduced, which is expected to lead to a reduction in the radioactive waste generated by activation. <During the muon generation operation and during the accelerator operation, a system for cutting and maintaining the irradiated portion of the rotating muon target where muon target activation is about to progress, and for removing the activated portion by grinding with a grinding stone. A system for cutting, grinding, and removing during the muon generation operation, accelerator operation, and device operation before the target is highly activated.> As shown in the right figure of Fig. 11 of the wedge-shaped rotating muon target, the rotating target part can approach the irradiation part of the disk with a device capable of grinding or cutting a part of the grinding stone or target during rotation during the operation of the muon generation part, accelerator, and MERIT ring, and grind or cut the irradiation part. Further, the activated part may be polished, cut, and removed by the cutting and removing device. (If it cannot be cut after thorough grinding, or if the surface of the disk cannot be formed by grinding during operation, it may be replaced with a new disk by a disk exchange machine or a robot arm.)

[0011] <0063><Automation of Replacement of Movable Muon Target> After proton irradiation and activation of a wedge-rotating muon target for muon generation, a replacement method, an alternating system, and an example of replacing the target when one muon target extraction port is fixed are disclosed in FIG. 10. <0064> For example, a device / robot part (TGT EXCANGE ROBOT / ARM (JUKE BOX MACHINE LIKE)) that can replace a record disk (wedge-rotating muon target MU-WEDGE-DISK-TGT) like a jukebox with a robot arm or the like, and a wedge-rotating muon target MU-WEDGE-DISK-TGT is mounted on a shaft (2TGT-EXCHANGE-AXIS) that can be rotated by a motor or the like (2TGT-EXCHANGE-MOT) in multiple (like a rotating magazine of a revolver) and a magazine part / disk holder / arm (2TGT-EXCHANGE-ARM) that can be rotated by the rotating means 2TGT-EXCHANGE-MOT. The arm can be rotated to replace the wedge-rotating muon target. The replacement can be automated. <0065> FIG. 12 describes the replacement after proton irradiation and activation of a wedge-rotating target for muon generation, an alternating system (when two muon extraction ports and solenoids are arranged, and one extraction port is in a standby state and its target is replaced). Two systems of muon extraction ports, solenoids, and muon irradiation systems for nuclear fusion fuel are required. However, without the above-described exchange rotation mechanism, the target T1 of the irradiation system and the nuclear fusion reaction part can also be made into two systems, with the intention of reducing the downtime when power generation cannot be performed. (There are two systems in FIG. 12, but multiple systems are also possible) In FIG. 12, a movable muon target part / wedge-rotating target part MU-WEDGE-DISK-TGT having two or more wedge-rotating target parts and muon capture solenoids / muon extraction parts can be moved in and out, moved back and forth, and inserted (at the MOVE part in FIG. 12) from the outer periphery to the inner periphery of the accelerator. The movable target part is moved (MOVE), pushed out, inserted, pulled out, and pulled back into the MERIT ring, and whether the proton beam collides with the wedge-rotating target part is controlled by the MOVE step and the insertion / removal step, and the generation of pions and muons at one extraction port can be controlled on and off.When replacing the target part in Fig. 12, it should be completely pulled out and pulled back from the MERIT ring for maintenance and replacement. The replacement etc. may be automated using a machine / robot (TGT EXCHANGE ROBOT / ARM).

[0012] <0082><Solution means><Means for solving the problem>The present specification and the invention regarding the solution means are described in Figs. 18 to 20. Also, a transport device 3 / structure 3 that decelerates cosmic rays and cosmic muons for use in nuclear conversion and uses the energy from the nuclear conversion as an energy source for propulsion or power generation is described in Fig. 21.

[0013] <Ionization Cooling> Negative muons may be decelerated using ionization cooling. Ionization cooling is based on a properly prepared muon beam passing through a suitable material (absorber) and losing momentum and decelerating by ionization. It is preferable to use absorbers made of atoms with a low atomic number Z, such as hydrogen and lithium. Cooling by both liquid hydrogen and lithium hydride absorbers is known from the following reference 1. (Reference 1: International Muon Ionization Cooling Experiment MICE collaboration, Nature volume 578, pages 53 - 59 (2020)) Construct and operate a part of the solenoid cooling and deceleration channel to perform ionization cooling and deceleration of muons using both liquid hydrogen and lithium hydride absorbers. * It may be possible to use a target part T1 containing nitrogen 15 and hydrogen (such as ammonia containing nitrogen and hydrogen) or borane containing boron and hydrogen (such as carbon 12) that has a low atomic number Z and binds muons in this application to promote nuclear conversion for muon nuclear fusion and nuclear conversion. * Muons may be combined with hydrogen ions to form muonic atoms and decelerated. Muons may be combined with atoms heavier than hydrogen, such as boron and nitrogen, to form muonic boron atoms, muonic nitrogen atoms MP1, MA1, etc. (decelerate MP1, MA1), and then introduced into a fuel substance target part T1 containing hydrogen. (In the configuration of B in Figure 16, form a muonic atom MA1 of atom A and decelerate MA1 by some means using an electric field (magnetic field), and then irradiate, introduce, and collide MA1 with a target part T1 - B that may contain atom B for nuclear fusion and nuclear conversion to cause muon nuclear fusion and nuclear conversion. <Frictional Cooling> * A carbon film may be placed on the target part T1 irradiated with negative muons, and the carbon film may be decelerated by friction (frictional deceleration, frictional cooling) when muons pass through it with a velocity. It may be attenuated with a carbon film containing carbon 12 (or a carbon film for frictional cooling made of carbon 12) for frictional cooling (frictional deceleration), and the muons decelerated within the carbon film may combine with carbon 12, and then carbon 12 may be muon - nuclear - converted. * In addition to the carbon film, solid and liquid parts such as boron hydride that have a low Z and can serve as T1 and FEED may also be considered. Elements with a low Z such as hydrogen are included, and the ionization cooling effect may also be used in combination.<Reducer Using a Deceleration Cavity>Particle accelerators and linear accelerators may be used for muon deceleration. The configuration using the pulse power supply and deceleration cell described in the following reference is known and may also be used in the muon deceleration section of this application. (Reference: Negative Muon Decelerator for Physical Research, Proceedings of the 16th Annual Meeting of Particle Accelerator Society of Japan, July 31 - August 3, 2019, Kyoto, Japan, PASJ2019 FRPI008).

[0014] <Assumed Example of Implementation><Muon Decelerator Using a Pulse Laser> A muon decelerator 2MUDECE and a nuclear conversion system 1EXP-SYS using a laser track field with a pulsed laser are shown in FIG. 18. FIG. 18 is similar to the configuration of an inertial confinement type nuclear fusion reactor by laser irradiation. However, in FIG. 18, in order to receive and decelerate muons descending from space or muons derived from an accelerator and pion generation section, instead of laser irradiation from all directions (opposite directions) of the inertial confinement method, a configuration may be adopted in which the target section is irradiated with a laser so as to face the direction for receiving high-speed muons. For example, in FIG. 18(A), when high-speed cosmic muons enter from space, the air, and the upper sky to the ground side, a pulsed laser is irradiated from a hemispherical dome-shaped laser irradiation section arranged on the ground to the central target section T1 to decelerate the muons, ((so as to face the incoming muons in (B)) laser irradiation, laser track field formation, and muon deceleration are attempted. The example of FIG. 18 is not limited to the use of cosmic muons. In FIG. 18, artificial muons M1 generated using the process of accelerator and accelerated particle collision may be decelerated and introduced into the target T1. While being able to irradiate the target section with artificial muons, the target section may be irradiated with a laser so that the muons can be decelerated.) *In one form of the present application, it is sufficient to implement a configuration in which a pulsed laser capable of forming a laser track field or an electric field can irradiate the target section T1. The T1 may be a target capable of nuclear fusion and nuclear conversion. According to one form, a nuclear fusion and nuclear conversion system using atoms with a small atomic number Z, such as carbon, nitrogen, boron, and hydrogen, for T1 may also be used. *For example, in the muon-catalyzed nuclear fusion reaction between hydrogen atoms (H, D, T), although helium is generated and the muon is trapped in helium and the catalytic nuclear fusion reaction stops, if the energy generated by the nuclear fusion of hydrogen atoms exceeds the energy obtained by decelerating cosmic rays and cosmic muons in nature and the balance is profitable, it may be possible to use it as an energy source. Therefore, in the system 1EXP-SYS having a portion for decelerating cosmic muons such as FIG. 18 and in the structure 3 and transportation equipment 3 including the same, it may also be implemented in the present application to attempt nuclear fusion between hydrogen atoms.(Although it describes a configuration for decelerating in an electric field, it is okay to change the trajectory of high-speed muons with a magnetic field if possible. A muon can be injected into the target part T1 by combining an electric field for deceleration and a magnetic field for deceleration and trajectory change.) Figure 18(A): When high-speed cosmic muons are incident from the cosmic, air, and upper air sides to the ground side, a pulsed laser is irradiated from a hemispherical dome-shaped laser irradiation part arranged on the ground part to the central target part T1 on the cosmic, air, and upper air sides, the target part is made into plasma, and a laser wakefield and an electric field facing the cosmic, air, and upper air sides are generated and used for decelerating muons. It is an explanatory diagram of a decelerator 2MUDECE. Also, the high-speed muons M1F generated by the muon generation device M1 may be incident on T1, form a laser wakefield and an electric field at T1, decelerate M1F to M1L, and then bond with the atoms of T1. Figure 18(B): It is an explanatory diagram of the pulsed laser incidence from the laser irradiation part MDCL to the target part T1 in FIG. 18(A), a diagram of muon incidence and deceleration, and an explanatory diagram of the formation of plasma 2LASER-PLASMA and a laser wakefield LWF and an electric field 2LASER-EF. Figure 18(C): It is an explanatory diagram when the decelerator 2MUDECE in FIG. 18(A) is continuously arranged horizontally to form an array of decelerators. *Cosmic muons reach the air and the ground at a rate of 1 per second per 60 cm². For example, 1.6×10⁸ muons can reach an area of 1 km×1 km per second. Therefore, a configuration is assumed in which the decelerator 2MUDECE is arranged to cover the area. *The array may be provided in a transport device 3 on the ground, at sea, in the air, or in space. Since muons can reach shallow water depths, it may also be mounted on a submarine or on 3 in water. *In one embodiment of the present application, the system may be a system capable of irradiating a pulsed laser as long as it is a system irradiated with cosmic muons and high-speed muons.)

[0015] <Example of implementation assumption><Muon decelerator using an element that generates an electric field> As an example of using an electric field, an element capable of generating an electric field (which may include an electric double layer generation unit) composed of atoms with a small Z is shown in FIG. 20. In the device of FIG. 20, a pulsed voltage and potential difference may be applied between the electrodes 2ER in a power supply unit so that an electric field can be generated pulsedly. As one embodiment of the present application, the configuration of FIG. 19(A) may be performed using the device of FIG. 20. *FIG. 20 shows an example of an element in which an electric field is formed. In the system described in FIG. 20, when muons are incident on electrodes, an insulator layer, etc., a decelerator and decelerating element composed of atoms with a small atomic number Z, which are difficult to trap muons and have a weak interaction at the incident location, may be used.

[0016] <Transport device 3, spaceship 3, space structure, residential area 3 capable of obtaining muons from cosmic rays>FIG. 21 shows an explanatory diagram of a transport device 3, spaceship 3, and space structure 3 that can receive cosmic rays and generate and utilize mesons and muons. The device 3 and structure 3 may be provided with a muon decelerator array described in FIGS. 18 to 20. 1EXP-SYS assumes the operation of an atomic battery, muon fusion battery, or muon nuclear conversion battery using cosmic rays (which is a power source that can operate even in places where sunlight does not reach on the lunar surface, for example). The cosmic rays (COSRAY1) are received at a cosmic ray receiving part in the transport device or structure 3, and mesons, pions, and muons are generated in a cosmic ray muon conversion part 2MU-COSRAY. The muons may be recovered (after being decelerated by a decelerator 2MUDECE) and transported and irradiated to a target T1. *As an image, (similar to how natural sunlight used in solar power generation is received by a large-area solar cell or photoelectric conversion element and collected in an electric circuit for use as power), for example, in a large-scale space residential area, a cosmic ray muon conversion part 2MU-COSRAY that receives natural cosmic rays over a large area, and a decelerator array part that decelerates the muons generated from the conversion part are provided. (Using something like a large-area net for capturing cosmic rays and muons and a circuit for decelerating and recovering muons), muons with a lower speed than cosmic rays are harvested and irradiated to a target T1 for use in nuclear conversion and power generation, and for power supply and propulsion of the structure 3. *An accelerator may be mounted on the transport device 3, and the accelerator may be used to accelerate and collide particles to generate mesons, pions, and muons, decelerate the muons, and use them in a nuclear conversion system using muons. *A target section and a muon target section (SMR1, 2MU-COSRAY) that collide with cosmic rays may be provided in the transport device 3 such as cosmic rays, artificial satellites, space probes, and space structures. The target section may contain a gas (including helium, hydrogen atoms, oxygen and nitrogen atoms in the atmosphere). The target section may contain a liquid such as water.

[0017] <Cosmic ray source> Cosmic rays flying in from outside the solar system or within the solar system (such as accelerated protons and helium ions) may be used as the source of cosmic rays. *Regarding a muon generation device using a known accelerator, it is possible to generate 1,000 to 100 million muons per second per centimeter of beam. On the other hand, on the ground and in the air, muons derived from cosmic rays pour down at a rate of 1 per second per palm. If it is possible to configure a muon deceleration section array, a muon capture section, a capture circuit, and a muon injection section into the target over an area and zone equivalent to 1,000 palms, it may be possible to use 1,000 muons per second for nuclear conversion without using an accelerator. Therefore, in the present application, a system for utilizing, decelerating, and capturing cosmic rays and cosmic muons over a large area is proposed. The muons may be used in the nuclear conversion system (for power generation applications by nuclear fusion and nuclear conversion, nuclear conversion applications) of the present application.

Brief description of the drawings

[0018]

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Explanation of reference numerals

[0019] This application claims the benefit of priority to Japanese Patent Application No. 2024-065053, filed on April 14, 2024, the entire disclosure of which is incorporated herein by reference. <Figures 1 and 3> Explanation diagram of a muon-catalyzed fusion system using a fusion reaction with boron and protons. M1: Muon generation means, means for injecting and irradiating muons into the fusion fuel target T1. Example: A system using a particle accelerator capable of generating muons. P1: Proton generation means, means for injecting and irradiating protons into the fusion fuel target T1. Example: A particle accelerator capable of accelerating protons and bombarding / irradiating the target. Elements of the fusion fuel in the boron-proton fusion reaction system. N1: Neutron generation means, means for injecting and irradiating neutrons into the fusion fuel target T1. Example: A particle accelerator capable of accelerating neutrons and bombarding / irradiating the target. A1: Particle accelerator A1. T1: Target part containing the fusion fuel. Fusion fuel T1, F1. B1: The part of T1 that uses boron. Boron target. Boron may be molten. L1: The part of T1 that uses lithium. Lithium target. Lithium may be molten liquid lithium. EX1: Product EX1 after fusion. In Figures 1, 3, etc., helium He and alpha rays generated after fusion. <Figure 5>3: Conveyor machine 1R: 1F-SYS which is a fusion reactor. A fusion reactor including 1F-SYS. It may be provided with a power generation unit that converts the energy of alpha rays into electric power energy. 1GENR: Power generation unit (the part that converts the energy obtained by the fusion system 1F-SYS or the nuclear conversion system 1EXP-SYS into electric power) * Although not specified in Figure 5, the nuclear fusion-derived electric power generated by 1EXP-SYS, 1F-SYS, and 1R may be supplied to the muon generation unit M1 and the proton generation unit P1 and used to generate muons and protons. This electric power may be used to drive the system of the present invention and each part of the system. 1TH: A fusion application propulsion device including 1F-SYS, a thrust generation device. Propulsion means. Moving means. (When 3 is a spacecraft, 1TH may be a particle beam emission part such as alpha rays, gamma rays, photons, particles, etc. When 3 is an aircraft, it may be a propulsion agent ejection part that takes in a propulsion agent and air using the electric power obtained by 1GENR, heats and compresses it, and ejects it to the rear of 3, or it may be an electric power-driven propeller part. When 3 is a ship, it is a part that can use the electric power obtained by 1GENR to rotate a propeller or generate a water flow. When 3 is a robot with an arm or a vehicle moving on land, it may be wheels, tires, a motor, or the motor and arm part of the robot that can be driven by the electric power obtained by 1GENR.) 1TH-NZ: Nozzle part of 1TH. When the product EX1 after nuclear fusion is helium or alpha rays with energy, it is a nozzle part that emits the alpha rays. It may also be a thrust deflection device or a nozzle. The alpha rays may be irradiated on the propulsion agent to heat and inject the propulsion agent. * Separately from 1TH-NZ, a propulsion device that operates by using the electric power generated by 1R to emit an ion thruster or a photon laser and propelling by the reaction may also be operated. <Figure 6> System using diborane B2H6: A boron-containing substance, B1, which is borohydride, diborane, or borane. T1 and F1 are diborane. The target of diborane. Diborane and BH1 may be gas, liquid, fluid, or (solid). (The configuration of Figure 7 using fluid is also possible.) In the system of Figure 6, since diborane containing hydrogen and protons is used, the proton introduction part P1 described in Figure 1 etc. becomes unnecessary. <Figure 7> 1F-SYS-RAM: Fusion system. (An assumed diagram when the system using the diborane of the present application is applied to a system in which a fusion fuel fluid having a known ramjet part circulates in a closed loop system) RAM: Ram pressure generation device part when compressing in a ramjet manner. PBH1: Compressed BH1 part. Target part of muon having a compressed diborane fluid part. FP: Fusion reaction part, muon irradiation part. FEEDC: Part for removing helium in the diborane fluid circulating in the system, removing excess substances, and adding necessary substances, diborane as fuel. Feed control part. Fuel supply system, fuel control system. Helium He removal part, diborane fuel supply part, etc. HX: Heat exchanger ENEX: Although not shown in the figure, a device part for generating electricity based on alpha rays and fusion energy, power generation part. It may be included in the system. PUMP: Compressor, pump. Pressurize, compress, and circulate the fluid in the system. Driven by a motor etc. (Driven by obtaining power from the power generation part) M1: Muon generation part, muon irradiation part. (Driven by obtaining power from the power generation part) EX1: Helium (requiring removal) generated after fusion. Symbols, etc. <Figure 8> 1F-SYS-MP1, 1F-SYS-MP1-RAM: A fusion system using a mixture of muonic hydrogen atoms and fuel. Muonic hydrogen atom MP1: AMP1: A muonic hydrogen atom generation irradiation unit (such as particle accelerator A1, neutral particle beam irradiation device NBI, etc., which can generate and incidentally input MP1 and MP12). S1: Path S1 (with a mixture of MP1 and boron hydride). MP1-XMB: A mixture of MP1 and boron hydride / diborane. Or a mixture of hydrogen and boron / (carbon·)nitrogen·oxygen·fluorine, etc. Or a part / mixture part containing a compound in which a raw material atomic nucleus with the first atomic number ZA and a raw material atomic nucleus with the second atomic number ZAA required for nuclear fusion are chemically bonded. PMP1-XMB: The mixture MP1-XMB compressed (and / or heated) by compression means such as RAM, or the mixture MP1-XMB compressed (and / or heated) by compression means such as RAM. RAM: Compression means such as a ram part. Inertial confinement fusion, which irradiates and confines a nuclear fusion target fuel pellet by laser irradiation (when the RAM part is of the laser confinement / inertial confinement type, the wavelength of the laser light may preferably use a short wavelength on the blue·ultraviolet·X-ray·gamma ray side so that the momentum of the photon can be taken larger), is known. Also in this application, the target part and the mixture may be compressed by a laser in the compression part RAM part. (A muon injection process may be added to the laser confinement type inertial confinement fusion.) The ram part may be irradiated with a laser, an ion beam, or an ion beam containing raw material atoms so as to converge from a plurality of emission parts to the part containing the raw material atoms (Figure 9). (It may also be an inertial type such as Z-pinch or magnetized target type that can compress raw material atoms and can be confined by inertia.))In the RAM section, while compressing and heating the raw material atoms that serve as fuel necessary for nuclear fusion and the parts of compounds or mixtures in which the raw material atoms are chemically bonded to each other using mechanisms such as lasers or ramjets, muons are irradiated. As a result, the molecular motion and atomic motion within the compound molecules or in the compounds / mixtures can be greatly increased by compression and heating. Consequently, the particles bonded to muons are more likely to approach each other due to thermal motion, with the intention of facilitating nuclear fusion, muon-catalyzed nuclear fusion, and muon-induced nuclear fusion. Additionally, there is also the aim of making it easier for the muons that act as catalysts after nuclear fusion to (be released, approach, and be captured by the next raw material atoms, and) initiate the next catalytic reaction. (Although irradiating muons onto hydrogen, DT, DD, or TT in a liquid cooled to extremely low temperatures may have a low effect of approaching raw material atoms due to thermal motion because of the low temperature, when muons, muonic atoms, or muonic hydrogen are introduced into the parts compressed and heated by a laser, ramjet section, etc., a proximity effect due to compression and thermal motion can be expected.) NZ: Nozzle section 1PP: Steam turbine generator HX: Heat exchanger, steam generation section, steam pipe, cooling pipe 1BKT: There may be a part or blanket that receives particles flying with energy due to nuclear fusion reactions such as neutrons and gamma rays, converts them into thermal energy, etc., and enables energy utilization. There may be a RAM or reaction vessel section, a container part for packing and ramming FEED, and a wall surface of the reaction vessel near the part where the nuclear reaction occurs. If so, a blanket 1BKT may be arranged within the RAM section or the container wall surface. AEC: Alpha-ray energy conversion device (a device that receives alpha rays and converts them into electricity. The AEC may generate radicals using alpha rays such as titanium oxide, decompose water (like a photocatalytic reaction) to obtain hydrogen and oxygen, and provide and output energy outside the system in the form of hydrogen chemical energy. *The AEC may be an alpha-voltaic-cell.* The AEC part may receive the energy of alpha rays and generate photons of synchrotron radiation (of bremsstrahlung). The photons of the synchrotron radiation may be used to cause chemical reactions or photochemical reactions in chemical substances. The photons may be irradiated onto the part to be heated to manufacture substances, heat and inject propellants or steam.It is also possible to use means for wavelength-converting the wavelength of photons of the synchrotron radiation to the longer-wavelength side, convert them to photons on the longer-wavelength side, receive the photons on the longer-wavelength side with a photoelectric conversion element, perform photoelectric conversion to obtain electric power, and output it outside the system. Alternatively, if the photons on the longer-wavelength side are photons having energy capable of causing a photocatalytic reaction with a photocatalyst, a photocatalytic reaction for generating hydrogen and oxygen from water may be caused to convert it to hydrogen energy. If the photons on the longer-wavelength side are photons having a wavelength capable of dissociating the bonds within carbon dioxide and nitrogen molecules and causing a photochemical reaction, carbon dioxide may be dissociated and converted as the energy of chemical substances such as carbon, carbon compounds, and nitrogen compounds, and output outside the system. <Figure 9>PMP1-XMB: A mixture MP1-XMB compressed (and / or heated) by a compression means such as RAM, or a mixture MP1-XMB compressed (and / or heated) by a compression means such as RAM. RAM: Compression means such as a ram section. In inertial confinement fusion where a nuclear fusion target fuel pellet is irradiated and confined by laser irradiation (when the RAM section is of the laser confinement / inertial confinement type, the wavelength of the laser light may preferably be a short wavelength on the blue, ultraviolet, X-ray, gamma-ray side so that the momentum of the photon can be larger), in the present application, the target section and the mixture may also be compressed by a laser in the compression section RAM section. (A muon injection process may be added to the laser confinement type inertial confinement fusion.) The ram section may be irradiated with a laser, an ion beam, or an ion beam containing raw material atoms so as to converge from a plurality of emission sections to the portion containing the raw material atoms (Figure 9). (It may also be an inertial type such as Z-pinch or magnetized target type that can compress raw material atoms and can be confined by inertia.) In the RAM section, by using a mechanism such as a laser or a ram jet, while compressing and heating the portion of raw material atoms that become fuel necessary for nuclear fusion and compounds / mixtures in which raw material atoms are chemically bonded to each other with a laser or the like, and irradiating with muons, the molecular motion and atomic motion within the compound molecule or in the compound / mixture can be increased by compression heating. As a result, particles bonded to muons are more likely to approach each other due to thermal motion, intending to facilitate nuclear fusion, muon nuclear fusion, and muon-catalyzed nuclear fusion caused by the approach. In addition, there is also an aim to make it easier for muons, which become catalysts after nuclear fusion, to cause the next catalytic reaction (released and repeatedly approach and capture the next raw material atoms). (Although irradiating muons to liquid hydrogen, DT, DD, TT cooled to an extremely low temperature of several kelvins may have a low proximity effect of raw material atoms due to thermal motion because of the low temperature, when muons, muonic atoms, and muonic hydrogen are introduced into the portion compressed and heated by a laser or a ram jet section, etc., a proximity effect due to compression and thermal motion can be expected.) RAMH: Heating means. (It may be included in the ram section. For example, means such as a laser or a microwave that can irradiate a substance remotely with electromagnetic waves or photons and can heat the substance. For example, in a system using water, hydrogen peroxide, and muons, water can be heated by microwave. Alternatively, the substance may be inductively heated electromagnetically.)For example, when using hydrocarbons as raw materials and promoting nuclear fusion between chemically bonded and adjacent carbon and hydrogen atoms in hydrocarbons using muons in the configurations of FIGS. 8 and 9, FIG. 9 is more likely than FIG. 8 to have the effect of promoting muon-catalyzed nuclear fusion because the raw materials can be heated by a laser or the like, and the movement of atoms and particles in the raw material substances becomes more active as the temperature rises due to heating means such as a laser, etc. (Heating means such as laser heating, or ion beam or neutral particle beam·NBI, ion beam or neutral particle beam·NBI containing raw material atoms, particle beam combining muons and ions·raw material atoms, millimeter wave, microwave, etc. may also be used.) RAM and RAMH may be irradiated with a laser or ion beam. Laser compression may also be possible. Also, laser heating may be possible. PUMP: Compressor, pump, motor FEED: Raw material substance (e.g., boron hydride, (hydrocarbon), hydrogen nitride, hydrogen oxide, etc.). (Lithium deuteride or the like may be a liquid or solid target. A substance serving as a raw material for a nuclear fusion reaction.) FEEDC: Control section of the feed. It may include a feed·raw material substance supply section, fuel supply section, etc., and a section for removing products after nuclear fusion such as helium. FP: Nuclear fusion (promotion) section, symbols, etc. <Figure 10>MU-MOVABLE-TGT: A target part (muon) where the part receiving the particle beam is movable. MU-DISK-TGT: A target part that may be a disk type where the part receiving the particle beam is rotatable and movable. Muon target part. MU-WEDGE-DISK-TGT: A muon target part that is movable and may be of the disk type, where the thickness of the part receiving the beam irradiation is thin, the cross-sectional shape becomes thinner towards the outer periphery of the disk, and it is wedge-shaped. MU-TGT-BRG: Support means such as bearings for supporting the movable part during movement and rotation. AXIS-TGT-BRG: When moving, if it rotates, its rotation axis. 2MU-GEN-ROT-TGT: Means for moving the muon target part and the muon target, a target unit part equipped with a motor and bearings. 2MU: An example of a muon generation part M1. (It may include a target, an accelerator, a charged conversion beam incident part, a part for adjusting the charge, a proton particle beam incident part, a proton particle beam accelerator part, a muon capture solenoid, etc.). It may be possible to generate muonic atoms MP1 by binding muons at M1 to protons and atomic nuclei (neutral particle beam). 2MU-ACC-RING: Circular accelerator, particle accelerator. 2MU-FFAG: FFAG accelerator. 2MU-MERIT-RING: MERIT ring type accelerator (A movable muon target that may be inserted, which becomes thinner towards the inserted tip part, may be inserted. The muon target part may be formed on the outer periphery of a rotatable disk or the tip of a chainsaw and be movable. A proton particle beam is irradiated on the inner peripheral side of the circumference of the circle, and then circular acceleration and spiral acceleration are performed by the accelerator and the ring, becoming high energy and high speed on the outer peripheral side and transitioning. Then, it may decelerate while colliding with the movable muon target and also recover energy and be able to collide with the target again. (The particles may decelerate due to target collision, move in the inner peripheral direction, be accelerated again, transition to the outer periphery, and collide again. An accelerator where particles are stored, accumulated, and re-accelerated in the ring.). 2MU-FFAG-CS·2MU-ACC-RING-CS·2MU-MERIT-RING-CS: The cross-section perpendicular to the toroidal direction and the cross-section cut in the poloidal direction when the accelerator is regarded as a donut, and the cross-section of the accelerator when cut between point CSP1 and point CSP2.A movable target (e.g., a thin disk-shaped muon target) into which a particle beam accelerated to high energy on the outer peripheral side of the circular accelerator and the MERIT ring is inserted can be inserted and moved in the outer peripheral direction of the circle of the accelerator cross-section. CS: Cross-section CS between point CSP1 and point CSP2 <Figure 12> · Replacement after proton irradiation activation of the rotating target for muon generation, an alternating system at two locations, a movable muon target section, a muon extraction port, and a muon capture solenoid that can be inserted, removed, and moved inside the accelerator. Explanation diagram when one extraction port is put on hold, the muon target section is removed from the accelerator and replaced, and the muon target section is replaced. 2MU-GEN-ROT-TGT: A movable muon target section unit system that can be MOVED, INSERTED, and EJECTED inside the accelerator. MUON CAPTURE TRANSPORT SOLENOID: Muon capture transport solenoid <Figure 11> 2TGT-EXCHANGE: A device for replacing a movable muon target with a robotic arm, target exchange section 2TGT-EXCHANGE-ARM: Arm section of the exchange section · Robot arm 2TGT-EXCHANGE-AXIS: Rotation axis of the exchange section 2TGT-EXCHANGE-MOT: Motor of the exchange section * It may be a device like the record replacement section of a jukebox. TGT EXCANGE ROBOT / ARM: (JUKE BOX MACHINE LIKE) <Figure 13> Examples of movable muon targets, examples with a part that can move a chain-saw-like (or cableway-like and lift-like) target. CHAIN-CATCHER: It is also the chain catcher part of a chain saw, and it is a part where the muon target section MU-MOVABLE-TGT on the saw chain can be replaced by a machine such as a robotic arm. Chain-Sow-and-TGT: Guide bar part for guiding the saw chain part with the muon target TGT of the chain saw attached. (In Figure 13, the muon can be decelerated by the muon decelerator MUDECE.))<Description of the Figures><Figure 14>Explanation diagram of a particle generation system that accelerates and circulates proton beams and helium in the first accelerator 2MU-ACC-RING, accelerates hydrogen or helium in a part where a particle accelerator may be used in the second accelerator 2HE-ACC-RING, collides them at the intersection 2CLP of the particle orbits of 2MU-ACC-RING and 2HE-ACC-RING, and generates mesons and muons. Protons can be collided with protons, or protons with helium, or helium with helium. (Explanation diagram of a particle generation system that accelerates and circulates proton beams in the first accelerator 2MU-ACC-RING, accelerates hydrogen or helium in a part where a particle accelerator may be used in the second accelerator 2HE-ACC-RING, collides them at the intersection 2CLP of the particle orbits of 2MU-ACC-RING and 2HE-ACC-RING, and generates mesons and muons. Protons can be collided with protons, or protons with helium, or helium with helium.)<Figure 15>As one of the embodiments of the present application, an explanatory diagram of a collision experiment system for meson generation using helium and protons as the target part. (B) A collision experiment system for meson generation equipped with two paths 2HE-FFAG-1ST and 2HE-FFAG-2ND looped. *The two paths 2HE-FFAG-1ST and 2HE-FFAG-2ND may be FFAG or MERIT-type accelerators or the particle orbits in the accelerator. In the case of the MERIT method, even when helium and hydrogen atoms collide in the paths of the two accelerators and then the energy decreases, it is intended to regenerate and re-accelerate the energy in the accelerator again to generate mesons (or some particles, elementary particles, atomic nuclei) again. <Figure 16>As one of the embodiments of the present application, explanatory diagrams of example (A) used for muon fusion or nuclear species conversion and example (B) used for the production of product atomic nuclei after element conversion and nuclear conversion. <Figure 17> As an example of one of the embodiments of the present application, it includes a step of decelerating cosmic muons such as cosmic muon SM1 and high-speed muons and irradiating and combining them with target atoms. (A) An example of decelerating high-speed cosmic muons with a dome-shaped decelerator array - decelerator 2MUDECE covering the celestial sphere and the upper sky, capturing them with the capture unit 2CAP, and irradiating the decelerated muons to T1 to attempt nuclear conversion. (B) An example of irradiating a laser directly to the target T1 of raw material atoms and molecules to form an electric field 2LASER-EF - laser track field having the intensity for decelerating cosmic muons, using the electric field to decelerate cosmic muons, and combining the decelerated muons with raw material atoms to attempt muon nuclear fusion and muon nuclear conversion.

[0020] <Description of Symbols><Fig. 13>(A) Example of a movable muon target (including a negative muon decelerator) MU-MOVABLE-TGT: Movable muon target 2MUCAP: Device for capturing and moving muons. Muon accelerator, solenoid, etc. MUDECE-ELEMENT: Decelerator element arranged in a direction to decelerate negatively charged muons with velocity (a decelerator using a laser wakefield applied accelerator may be used). MUDECE (MDC): Decelerator including MUDECE-ELEMENT. Muon decelerator (an accelerator using a laser wakefield may be used, or accelerator 2AC or accelerator A1 may be used for deceleration) <Fig. 14> 2MU: Muon generation device 2MESON: Meson generation device 2PARTICLE-COLLIDER: Particle collision device, device for generating mesons and elementary particles by particle collision 2MU-ACC-RING: Accelerator for accelerating, circulating, and moving protons·hydrogen (or helium) as ion beams. First accelerator. 2MU-FFAG: FFAG type 2MU-ACC-RING. 2MU-MERIT-RING: MERIT ring type 2MU-ACC-RING. 2HE-ACC-RING: Accelerator for accelerating, circulating, and moving helium (or protons·hydrogen) as ion beams, and the orbit of the accelerator. Second accelerator. 2HE-FFAG: FFAG type 2HE-ACC-RING. 2MU-FFAG-CS, 2MU-ACC-RING-CS, 2MU-MERIT-RING-CS: Cross-sectional view of the first accelerator MU-MOVABLE-TGT: Movable target. The atoms of the muon target are movable. MU-P-HE-ORBIT-TGT: Movable muon target composed of hydrogen or helium (ion beam·orbit in the accelerator). Target for generating mesons and elementary particle muons by accelerating, circulating, and moving helium or hydrogen in the accelerator. 2CLP: Intersection·collision point, or intersection·collision part of the orbit of the accelerated particle ion beam. Collision part (2CCP) of helium and hydrogen, helium and helium, hydrogen and hydrogen. Location where mesons and elementary particles can be generated by collision.*In the first accelerator 2MU-ACC-RING·2HE-FFAG-1ST, proton beams and particle beams (helium) are accelerated and circulated. In the second accelerator 2HE-ACC-RING·2HE-FFAG-2ND, hydrogen or helium particle beams are accelerated within a portion where a particle accelerator may also be used. Collision occurs at the intersection 2CLP of the particle orbits of 2MU-ACC-RING and 2HE-ACC-RING (2HE-FFAG-1ST and 2HE-FFAG-2ND) to generate mesons and muons (elementary particles and particles). The portion where the intersection and collision occur when attempting to generate them. <Fig. 15> 2AC: Acceleration cavity, acceleration means. The acceleration cavity of the laser track field may be used, and the laser may be a laser device, a photon of synchrotron radiation light (radiation light) using a particle accelerator or alpha rays, or a laser. 2MGF: Magnet, deflection means and focusing means for ions, ion beams and charged particles. Deflection magnets such as deflection electromagnets, and focusing magnets such as quadrupole electromagnets that focus and converge the beam to prevent it from spreading. 2ISRC: Ion source He (or, H / p). Ion incident part. It may include a device for ionization or a device for accelerating and incident ions. 2EXTEJ: Ion removal part. It may be an ion intake part or an ion extraction part. EX-ION: Among the ions that move and circulate in the 2HE-FFAG-2ND (accelerator orbit), the ions removed by 2EXTEJ. A separation method based on the difference in the mass of the ions used in mass spectrometry may be used. Ions may be separated by taking advantage of the difference in mass with respect to the charge of the ions by means of charge and magnetic field. 2HE-FFAG-1ST: The first accelerator. A circular accelerator that accelerates and circulates FFAG-type helium, etc. 2HE-FFAG-2ND: The second accelerator. A circular accelerator that accelerates and circulates FFAG-type helium, etc. 2CLP: The part where two He, particles, and beams collide <Fig. 16> 2MU, 2MESON-GENERATOR, 2PARTICLE-COLLIDER: Muon generation means, meson generation means, particle collision means. MUON-CAPTURE-TRANSPORT-SOLENOID: Means for capturing and transporting muons from mesons such as pions and K mesons. A solenoid that captures pions by a magnetic field, moves the pions, and transports muons while the pions change into muons. MUDECE: Means for decelerating muons. Negative muon decelerator. Low-speed muon generation part. MUDECE may be provided in the MUON-CAPTURE-TRANSPORT-SOLENOID part. A negative muon decelerator combining a pulse power supply and a deceleration cell has been studied and is known, and it may be used. It is preferable to use a negative muon decelerator that can decelerate to a lower speed. The energy of the negative muons generated using the accelerator and meson generation part is preferably about 300 keV (= 8 MeV / c) or more, and for example, it can be decelerated to 30 keV or less.If it is possible to arrange the laser track field and the acceleration cavity and acceleration section using the same in the reverse direction, i.e., the deceleration direction, they may be arranged and used for decelerating negative muons. 1F-SYS: Fusion system using muons. 1EXP-SYS: Experimental system using muons, nuclear conversion system (nuclear conversion system for LLFP·MA). FP: Fusion section, muon fusion section, part of the fusion section core. NCTP: Nuclear conversion section, muon nuclear conversion section, part of the nuclear conversion core. Muonic-Atom-Generator: Part that binds a negative muon to atomic nucleus A (or B) to generate muonic atom A (or B). MA1: Muonic atom A (or B). (Atom A / B irradiated to the target). FUSIONED-T1-AB-X: Atom X. Atom X generated by nuclear fusion and nuclear conversion of atomic nuclei A and B by muons. T1-AB: Target T1 part of muons composed of a compound or mixture in which atomic nuclei A and B are bonded. Atoms A and B may have different Z values or the same Z value. For example, atoms A and B may be the same carbon-12. T1-AB is a compound or mixture in which atomic nuclei A and B are bonded. T1-AB may be a mixture of atoms A and B collided with atom B or a structure in which A and B are arranged in the vicinity. FUSIONED-T1-MA1B-X: Atom X. Atom X generated by nuclear fusion and nuclear conversion of muonic atom A and atom B by muons. Atom Y may be generated from atom X through a radioactive decay process. T1-B: Target of atomic nucleus B (or A). T1-B is a movable T1·T1-B for muon and muonic atom irradiation part. (T1-B may be the film surface or solid / liquid surface of movable T1. Depending on the element, it may also be a gas, plasma, or beam). T1-B may be able to remove its surface in the atom X removal process. (Similar to polishing the movable disk-type muon target MU-DISK-TGT in solid in Fig. 11 with a grinding stone MU-DISK-GRINDING-DEVICE, after manufacturing atom X from atoms A and B on target T1 by muon nuclear conversion, atom X may be removed and recovered by a grinding stone or polishing / cutting means). T1-IN: Atom supply process / means. Supply part of atoms A and B. T1-OUT: Atom removal process / means. Removal part of atom X. <Fig. 17>(A) An example of decelerating high-speed cosmic muons with a dome-shaped decelerator array that covers the celestial sphere and upper sky side as seen from T1 placed on the ground side, irradiating T1, and attempting nuclear conversion. SM1: Cosmic muons flying in from above (cosmic-ray muons, cosmic-ray muon particles). High-speed cosmic muons SM1. When cosmic rays collide with the Earth's atmosphere (atmosphere), cosmic-ray pions and mesons are generated by the collision of atmospheric molecules and cosmic-ray particles, and cosmic-ray muons are generated from those mesons. Cosmic-ray pions can be generated at an altitude of about 20 km, and muons pour down below an altitude of 5 km. (The transport device 3 of the aircraft having the system in Fig. 17(A) is at an altitude where it receives cosmic muons. The aircraft 3 can use cosmic muons for nuclear conversion. Other transport devices 3 near the ground or on the sea can also receive cosmic muons.) Cosmic rays: Particles flying around in outer space with high energy. MDC-LASER: When the muon decelerator uses an accelerator that uses a laser track field as the decelerator, the laser light source and laser generation unit of the accelerator. The light source may use an existing laser device. The light source may also use emitted light. MDC: Decelerator. 2MUDECE: Decelerator. A decelerator for muons (an accelerator may be used for deceleration) (an accelerator such as 2AC or A1 that may use a laser track field may also be used for deceleration) 2MUDECE-ARRAY: An array of 2MUDECE. Photons or lasers may be distributed to 2MUDECE. It may also include circuits for electricity, power, signals, lasers, etc. for driving 2MUDECE. 2MUCAP: MUON CAPTURE TRANSPORT Device, a device that captures and moves muons. Such as a solenoid. T1: Target, FEED. According to one embodiment, the system 1F-SYS / 1EXP-SYS may attempt muon-catalyzed nuclear fusion or nuclear conversion in a configuration where muons decelerated by a decelerator 2MUDECE are combined with nuclear fuel atoms or raw material atoms for muon-catalyzed nuclear fusion, such as existing known hydrogen H, deuterium D, tritium T, or lithium 6 (or raw material atoms with each other). Also, the raw material atoms and fuel atoms for nuclear fusion and nuclear conversion such as hydrogen, boron, carbon, and nitrogen described in this application may be used in the systems 1F-SYS / 1EXP-SYS such as Fig. 13(B) or (A). The configuration, system, and device for decelerating the cosmic muons in Fig. 17 may be mounted on the transport device 3.If muon nuclear conversion can be performed using cosmic muons, a large accelerator is not required. Therefore, when installing it in the transport device 3, if the size of the transport device 3 can be made compact by eliminating the large accelerator for muon generation, there is an advantage. Note that an accelerator such as accelerator 2AC or A1 that uses a laser wakefield may be used to make the muon decelerator for cosmic muons compact, or accelerator 2AC or A1 may be used for deceleration. (A configuration for accelerating electrons and negatively charged particles to the GeV level using a laser wakefield is known, and this application assumes the use of a laser wakefield for decelerating negatively charged muons, which are also negatively charged particles.) Also, for the purpose of compactly installing a muon and meson generation section and a high-speed muon deceleration section in the transport device 3, an accelerator such as accelerator 2AC or A1 that uses a laser wakefield may be used to configure a device 2MU, 2MESON-GENERATOR, or 2PARTICLE-COLLIDER for meson generation. (B) An example of directly irradiating a target T1 of raw material atoms and molecules with a laser to decelerate muons and attempting muon nuclear fusion and muon nuclear conversion of T1. 2LASER-PLASMA: The plasma part generated by the laser and T1 when forming a laser wakefield by plasmaizing T1. 2LASER-EF: The electric field generated by the laser and T1, and the laser wakefield formed in T1. T1, FEED: The target atoms, raw material atoms, and fuel atoms to be nuclear-converted and nuclear-fused. 2LASER: The laser source. MDC-LASER: The laser used in the laser-based decelerator (in this figure, the laser may be generated by external energy, or the energy of alpha rays, gamma rays, etc. generated by nuclear fusion and nuclear conversion may be used to generate photons and gamma rays and used for laser generation. AEC is the conversion part of alpha ray energy, and in this figure, it can be taken out as the energy of photons by bremsstrahlung of alpha rays instead of electric power). <mudec1>A target atom and raw material atom nuclear conversion system, which includes a step of decelerating muons and is characterized by being capable of binding to target atoms and raw material atoms for nuclear conversion of muons. <mudec2>The nuclear conversion system described in MUDEC1 that performs nuclear fusion or nuclear conversion of target atoms and source atoms, which has the feature of irradiating the target atoms and source atoms with a laser to generate an electric field or a laser wake field. <mudec3>The nuclear conversion system described in MUDEC2 capable of decelerating muons in the electric field or laser wakefield. <mudec4>A nuclear conversion system according to MUDEC2, which irradiates a target atom or a raw material atom to be subjected to nuclear conversion with a laser to generate an electric field or a laser wake field, decelerates muons generated by cosmic muons, cosmic ray muons, or muons flying from the cosmic side to the ground side by cosmic rays, and has a feature capable of binding the decelerated muons to the target atom or the raw material atom to be subjected to nuclear conversion. <dlal1>A target atom / raw material atom nuclear conversion system comprising a step or means for decelerating muons, and having a feature that enables binding to a target atom / raw material atom for nuclear conversion of muons. <dlal2>The nuclear conversion system described in DLAL1 capable of decelerating muons in an electric field, or a laser wakefield, or an accelerator. <dlal3>The nuclear conversion system according to DLAL1, which performs nuclear fusion or nuclear conversion of target atoms and source atoms, having the feature of irradiating the target atoms and source atoms with a laser to generate an electric field or a laser wakefield. <dlal4>A nuclear conversion system according to DLAL1, which irradiates a target atom and a raw material atom to be nuclear-converted with a laser to generate an electric field or a laser wake field, decelerates muons derived from cosmic muons or muons flying from the cosmic side to the ground side, and has a feature capable of binding the decelerated muons to the target atom and the raw material atom to be nuclear-converted. <dlal5>A nuclear conversion system using muons, wherein the atomic number Z or the effective nuclear charge (of the 1S orbital) of atom A, which is the raw material for nuclear conversion when performing nuclear conversion, is greater than the atomic number Z or the effective nuclear charge (of the 1S orbital) of atom X generated after the nuclear conversion of said atom, and which has the characteristics of DLAL1 (or DLAL2) described in the nuclear conversion system. <dlal6>The nuclear conversion system described in DLAL2, which is characterized by injecting and irradiating muons into target atoms containing carbon and carbon-12. <dlal7>The nuclear conversion system described in DLAL2, which is characterized by injecting and irradiating muons into target atoms containing nitrogen and nitrogen-15. <dlal8>A nuclear conversion system according to DLAL2, which has a feature of introducing and irradiating a muon to a target atom containing boron. <dlal9>A power generation system using the energy generated by the nuclear conversion system described in DLAL5. <dlal10>Hydrogen or helium is being accelerated and circulated in the first accelerator (2MU-ACC-RING), and hydrogen or helium is being accelerated and circulated in the second accelerator (2HE-ACC-RING). A muon is generated using a particle generation system having a feature of colliding hydrogen or helium at the intersection 2CLP of the particle orbits of the first accelerator and the second accelerator to generate mesons, and the nuclear conversion system described in DLAL1 used for the nuclear conversion. <dlal11>The nuclear conversion system described in DLAL1 (or DLAL2) having the feature of converting nuclear fission products. <dlal12>A nuclear conversion system as described in 1·DLAL10 for converting nuclear fission products, the nuclear conversion system being characterized in that a muon beam is irradiated towards a compartment of a building having nuclear fission products. <Brief Description of the Drawings><Description of Reference Numerals><Figure 18>*Regarding a laser-induced inertial confinement fusion reactor, a configuration in which muon deceleration is combined with muon deceleration by a laser wakefield using a laser pulse (a system in which the target part of a pulsed laser inertial confinement fusion reactor is a nucleus with a small Z such as B, C, or N)*MDC-LASER (MDCL) laser source, pulsed laser source*Known laser source for a laser wakefield accelerator (A) 1F-SYS: Fusion system. 1EXP-SYS: Nuclear conversion system. MDCL: Laser irradiation unit T1 to target part T1. T1·FEED: Target part T1, source atom. (In the case of Figure 18, it may also serve as the gas, molecule, or atom that forms the plasma for forming the laser wakefield) 2MUDECE: Muon decelerator, particle decelerator (B) 2LASER-EF: Laser wakefield LWF formed by a laser. Electric field. 2LASER-EF is formed. Electric field for decelerating muons. 2LASER-PLASMA: Plasma generated by irradiating T1 with a laser. It may include T1 and muons may bind to T1 which is also a plasma after deceleration. SM1: Cosmic muon, cosmic muon source M1: Muon, muon source M1F: High-speed muon M1L: Decelerated muon (C) Explanation diagram of decelerating (capturing) muons by an array of decelerators using a laser wakefield over a wide area and irradiating and binding them to T1. M1, SM1, M1F: High-speed muon source (When using SM1, it covers an area such as the size of a thousand palms) 2MUDECE-ARRAY: Array of decelerators. M1L: Decelerated muon. T1: Target (When the target T1 part of a pulsed laser inertial confinement fusion reactor is a T1 part accessible to muons and an electric field for muon deceleration is formed by a pulsed laser and muons are decelerated by the electric field, muon nuclear fusion between the muons and the T1 part atoms may also be carried out simultaneously) <Fig. 19>(A) 2MDCE-2DFD: A planar element formed by an electric field (a large-area array is also possible) as one form of 2MUDECE. This part may be able to form an electric field or a magnetic field. 2MUDECE: Decelerator. Muon decelerator PWSP: Power supply unit. Apply a voltage or potential difference to 2MDCE-2DFD. Or means for applying an electric field. (Power supply when forming an electric field or a magnetic field) (Power supply for causing temperature change even when forming an electric field as in the case of a pyroelectric body. Temperature change source) 2MUCAP: Muon capture part. LM1Z: Section where muons are attenuated and removed. Muons are attenuated by 2MUDECE and captured, removed, and recovered by 2MUCAP, a location where cosmic rays and muons do not reach or are less likely to reach. (LM1Z may be formed from a muon decelerator and a capture part, or may be a section deep underground inside the ground containing high-Z atoms naturally) T1: Target T1-2COILB: Location when applying a magnetic field to T1 with a coil. 2COIL: Means for applying magnetic field B to target part T1 and muons. Coil. T1-2BMU: T1-2BMU: Location of T1 where muons that rotate (cyclotron motion) around magnetic field B come into contact with it (To increase the reaction area between muons and T1, muons are rotated by applying magnetic field B and stirred inside T1) (B) 2FDELE-PYR: Pyroelectric device (An element when causing a temperature change in a pyroelectric body to generate an electric field in the pyroelectric body and using the electric field for muon deceleration. In one embodiment, it may be said to be one form of a capacitor element sandwiched between a pyroelectric body and a dielectric by electrodes. The 2FDELE-PYR may be an element that can be arranged in a planar and large-area manner.) VOLT-C: GND / Voltage control unit T1: Target. FEED. (It may also be the electrode part 2ER of target T1 controlled by VOLT-C.) 2PYR-EF: Electric field by the pyroelectric body. Muons may be decelerated in this part. 2PYR: Pyroelectric body. *2PYR may sometimes become the target T1 of muons. P: Polarization. 2PYR-PEF: Internal electric field of the pyroelectric body. Muons may be decelerated in this part. 2ER: Electrode part TEMP-C: Temperature change means, heater / cooler part -Z plane: Regarding the thickness and height z direction of the pyroelectric body, the target direction, the direction on the drawing. +Z plane: The Z in the direction of the heater side and the lower direction on the drawing.<Figure 20> 2MUDECE: Muon decelerator configured using a capacitor element in this figure. (A) Applying a voltage to an insulator capacitor to form an electric field in the insulator (composed of low-Z atoms that are difficult to trap muons). 2ER: Electrodes (example) Electrodes made of low-Z atoms. Carbon electrode, lithium metal electrode. 2LZI: Insulators (example) Insulators made of low-Z atoms. Carbon insulator, diamond, hydrocarbon solvent, etc. 2ER and 2LZI may be made of low-Z atoms that are difficult to trap muons. Also, 2ER and 2LZI can become capacitor elements to form an electric field and decelerate muons, and can also serve as the target T1 part that binds to the decelerated muons. Therefore, for example, raw material atoms that can cause muon nuclear conversion and muon nuclear fusion such as carbon-12, nitrogen-15, and hydrogen can be included in 2ER and 2LZI. (For example, 2LZI is an insulator containing carbon-12, and 2ER is a carbon-based electrode made of carbon-12 containing metallic lithium as a current collector, mesh electrode, bus bar, or bus). * 2ER may be connected to other circuits. For example, 2ER may be drawn out from the deceleration part (away from the decelerator functional part) and connected to copper or aluminum wires, circuits, or bus bars so as not to interfere with muon deceleration or utilization. 2FDELE: An element that forms an electric field, a capacitor element formed by sandwiching 2LZI with 2ER. * When using a plurality of such capacitor elements, the elements may be electrically connected in series. * An explanatory diagram of decelerating cosmic muons by arranging capacitor elements in a large area. The element is a capacitor-type sheet device and is expected to be a planar element like a solar cell. 2FDELE-LAM: A laminate of the element 2FDELE. (Electrically connecting 2FDELE in series in the height direction and the stacking direction). PWSP: Power supply unit. A power supply unit that applies a potential difference or voltage to the capacitor element 2FDELE or 2FDELE-LAM to form an electric field inside the capacitor element. (B1) Applying a voltage to an electric double layer capacitor EDLC to form an electric field (composed of low-Z atoms that are difficult to trap muons). 2ER: Electrodes. 2FDELE-EDL-MPI: A part including an electric double layer part. A part that forms an electric double layer at the interface of a porous membrane and uses the electric double layer part as an insulator / dielectric (corresponding part). Porous electrode. PWSP: Power supply unit. Pulse power supply unit. 2ER and 2FDELE-EDL-MP may be made of low-Z atoms that are difficult to trap muons.In addition, 2ER and 2FDELE-EDL-MP can also serve as a capacitor element to form an electric field and become a target T1 part that combines with the decelerated muons when decelerating the muons. Therefore, for example, raw material atoms that can cause muon nuclear conversion and muon nuclear fusion, such as carbon-12, nitrogen-15, and hydrogen, may be included in 2ER and 2FDELE-EDL-MP. 2FDELE-EDL: Element that forms an electric field, 2FDELE-EDL-MPI is a capacitor element and an electric double layer capacitor element formed by sandwiching 2ER. 2FDELE-EDL-LAM: Stack of element 2FDELE-EDL (2FDELE-EDL is electrically connected in series in the height direction and stacking direction). (B2) Enlarged view of the EDLC part 2ER-MPI: Porous membrane, porous electrode (EG: Porous carbon electrode), porous electrode of an electric double layer capacitor. 2EDL: Electric double layer formed in the electrode part 2ER-MPI-MICRO; Enlarged part of 2ER-MPI, porous electrode part. 2ELYT: Electrolyte (including electrolyte). <Figure 21> Explanatory diagram of a spacecraft or space structure that generates muons from cosmic rays, decelerates the muons, and uses them for nuclear conversion and energy for driving transport equipment. 3: Transport equipment 3, Energy supply target 3 (including aircraft, spacecraft, space structures, artificial satellites, space bases, space habitats, lunar bases - far side lunar bases, structures in places not reached by sunlight) COSRAY1: Cosmic rays 2MU - COSRAY: Part that receives cosmic rays and generates mesons, pions, and muons. Muon generation source. SMR1. It may be an array - shaped 2MU - COSRAY or a configuration where muons can be input into 2MUDECE. SM1: Cosmic muons. Muons generated by cosmic rays. A1: Particle accelerator. Particle generator - irradiator M1: Muon system, P1: Proton system. MA1: Muonic atom generation section. Artificial muons (muonic atoms) may be decelerated by making them into muonic atoms. M1F: High - speed muons (SM1 or high - speed M1) 2MUDECE: *MUDECE muon decelerator, may be a decelerator array 2MUDECE - ARRAY. (2MUDECE may include 2MUCAP, the part that captures and moves muons.) M1L: Decelerated muons T1 - HARVESTER: Means to harvest T1 from other planets, satellites, celestial bodies, source of T1. External fuel collection means (asteroids, natural celestial bodies) FEEDC1: Fuel F1 (FEED), supply section for target T1. *Storage container for T1·F1, fuel storage section, target automatic replacement device, supply system for T1·nuclear fusion / nuclear conversion fuel. 1R: Nuclear conversion - nuclear fusion reactor. 1F - SYS: Nuclear fusion system. 1EXP - SYS: Nuclear conversion system. T1, F1: Target section of the atom to be nuclear - converted. Feed section. Nuclear conversion fuel section. Reaction section - core section of nuclear conversion. In the T1 section, muons are combined with T1 to promote muon - nuclear conversion. HE1: Product generated by nuclear conversion occurring at T1. As an example, high - energy helium - alpha rays. AEC: Alpha - ray energy conversion section. Part that converts the energy of alpha rays into other energy. AEC may be a traveling - wave direct energy converter TWDEC / Traveling - Wave Direct Energy Converter. AEC may also be a direct energy converter that converts the kinetic energy of the generated particles into electrical energy.Example: The part that bends the traveling direction of alpha rays with high energy (high kinetic energy) (by means of bending, such as the magnetic field of coil 2COIL) to cause synchrotron radiation and bremsstrahlung, and converts them into radiation light, gamma rays, and photons (light energy). (*Alpha rays can be stopped even by thin paper. Therefore, they may be stopped at a part that stops alpha rays such as paper or a sheet to cause bremsstrahlung. Photons may be generated by stopping alpha rays at a sheet part composed of low-Z atoms. Since it is desired to prevent the generation of gamma rays when alpha rays are stopped and the gamma rays cause the reactor to become radioactive, alpha rays may be stopped using atoms that are less likely to become radioactive (low-Z atoms).)* By the interaction between alpha rays and material atoms, the atoms may be excited by the excitation action of alpha ray collisions, or the electrons of the atoms may be ejected by the ionization action (ionization effect) to ionize the atoms. The phenomenon that alpha rays are scattered by atoms may also occur. *When the photon energy is 1.022 MeV or more in the interaction between gamma rays and matter, pair production (production of a pair of a positron and an electron) may occur. Therefore, pair production and positron production may be performed in the AEC section. Energy conversion may be performed using the photoelectric effect in the AEC section, or high-speed electrons (photoelectrons) may be generated. The Compton effect may occur, and as a result of gamma rays hitting electrons in matter and the electrons being scattered, Compton electrons may be generated. *Although it is desired to avoid the conversion of the nuclides of the materials constituting the AEC section and the reaction path 1R into radioactive elements by photonuclear reactions, since high-Z atomic nuclei may have many paths to emit neutrons and become radioactive atomic nuclei by photonuclear reactions, it may be advisable to refrain from using them and use low-Z atomic nuclei instead. (However, it is not necessarily limited to not using high-Z atoms because high-Z atoms have higher gamma ray absorption and shielding capabilities.)* When nuclear conversion occurs at T1 and alpha rays are generated, the traveling direction of the alpha rays may be deflected by the magnetic field of coil 2COIL to promote the generation of radiation light, gamma rays, and photons. 1PRPLT: Propellant. The propellant ejected rearward of 3 during acceleration propulsion. Photons, alpha rays, etc. Also, when performing electric propulsion or rocket propulsion, it is the propellant. (When propelling in the atmosphere, 1TH is the atmosphere or air ejected by a jet engine or a propeller motor) 1TH: Propulsion means. (A propeller that emits alpha rays, a propeller that ejects photons, an electric thruster, etc.Propeller motor, jet engine, etc.) 1TH-NZ: Nozzle (1TH and 1TH-ZL may be able to change the ejection direction when ejecting the propellant. For example, when accelerating at 3, eject the propellant backward at 3, and when decelerating at 3, eject it forward at 3) 1GENR: Power generation part. The part that generates power using the energy of helium in HE1. 3SYS: The system of 3 (may include the power and electrical system, the control system, and the control part of 3). It may receive power supply from 1GENR. It may supply power to the devices and locations belonging to 3 from 3SYS. <Figure 6> Figure 6 shows an assumed diagram of a fusion reaction system (A) using diborane (B) and a nuclear conversion system using carbon (C) and nitrogen (D). M1: Muon generation input / introduction means (negative muons at an appropriate speed) In (A), irradiate diborane composed of hydrogen and boron 11 with negative muons, perform muon nuclear fusion on boron 11 and hydrogen in diborane, convert it to excited carbon 12 atomic nuclei (12C*), and then convert carbon 12 into three helium. In (C1) of (C), for carbon materials such as graphite, carbon black, and diamond composed of carbon 12, after muons bind to carbon 12 in the carbon material to generate excited carbon 12 atomic nuclei (12C*), it shows the process of being converted into three helium. In (D), irradiate hydrazoic acid containing nitrogen 15 and hydrogen with negative muons, perform muon nuclear fusion on nitrogen 15 and hydrogen in hydrazoic acid, and convert it into carbon atomic nuclei (12C*) and one alpha ray. (The remaining carbon 12C* is then converted into three helium by nuclear conversion of carbon and muons.) (C2) and (C3) are assumed diagrams when irradiating muons in an alkane molecule. Although it has not been confirmed how the reaction actually occurs, carbon 12 and hydrogen in the alkane may undergo muon nuclear fusion. When a muon binds to a carbon 12 atom, it may be converted into three helium atoms. The effective nuclear charge Z of a carbon atom is larger than that of a hydrogen atom. <Atom production by nuclear fragmentation> It may be attempted to irradiate positive muons / muons to atomic nuclei such as carbon C and oxygen O to change them into other atomic nuclei. Also, irradiate high-energy positive muons / muons accelerated to a certain atomic nucleus A, collide the atomic nucleus A with the positive muons to perform a nuclear fragmentation reaction, and produce the atomic nucleus X that becomes the product. When protons accelerated to high energies of 100 MeV or more using an accelerator or the like are incident on target atoms (such as mercury, lead bismuth, lead, tungsten, tantalum, uranium, carbon, etc.), the high-energy protons collide with the atomic nuclei in the target, and the energy breaks up the atomic nuclei of the target. The reaction in which secondary particles such as neutrons and mesons are emitted from the atomic nuclei is called a nuclear fragmentation reaction. In one example of the present application, instead of protons, positive muons may be accelerated, irradiated, and collided with nuclear fragmentation targets such as bismuth, lead, and mercury to cause a nuclear fragmentation reaction of nucleus A to convert it into nucleus X. *When nuclear fragmentation by positive muon collision occurs compared to nuclear fragmentation by proton collision, there is an expectation that a nuclear fusion reaction (a reaction in which protons for collision are added or replaced in the atomic nucleus) does not occur when a proton collides with the atomic nucleus. When the protons and neutrons of nucleus A collided by positive muons are fragmented and scattered by the collision, even if positive muons are added or replaced in nucleus A, the positive muons only decay into positrons and neutrinos afterwards (positrons and leptons are replaced in nucleus A, and then the positrons combine with the electrons of the atom to emit photons and undergo pair annihilation), and there are characteristics and advantages that no protons or neutrons remain in nucleus A. <Muon decelerator, muon attenuation section> ○ Cosmic muons can be decelerated and irradiated onto hydrogen molecules and hydrogen, and used for muon-catalyzed nuclear fusion between hydrogens. (A plasma containing hydrogen, D, and T may be confined by a magnetic field, irradiated with muons, and magnetic confinement nuclear fusion may be promoted.) When cosmic rays or cosmic muons can be utilized, even when helium, which was a problem with hydrogen atoms, is generated and the reaction stops, if the energy is not required for muon generation and the energy balance for decelerating muons, irradiating them onto hydrogen fuel, and causing nuclear fusion pays off, it may be possible to use it for cosmic muon-catalyzed nuclear fusion power generation.

[0021] This application claims the benefit of priority to Japanese Patent Application No. 2024-082974, filed on May 26, 2024, the entire contents of which are incorporated by reference. An explanatory diagram regarding the assumption of a nuclear conversion and nuclear fusion system using muons considering the muon-nucleus capture reaction is described in FIG. 22. In this application, it is assumed that muons are irradiated onto a carbon material composed of carbon-12 to obtain excited carbon-12 atomic nuclei and then converted into helium. FIG. 22 is an explanatory diagram thereof. (A) Muons are bound to carbon-12 in the carbon material to cause a muon atomic nucleus capture reaction, which changes to a boron-12 atomic nucleus (12B*) having an excitation energy that may be 10-20 MeV. After that, excitation energy transfer occurs from 12B* to the adjacent carbon-12 atomic nucleus, generating excited carbon-12 (12C*), which is then converted into helium. The excitation energy is transferred to the adjacent carbon-12, and this process is repeated. This is an explanatory diagram of the assumption that the carbon-12 atomic nuclei in the carbon material of carbon-12 are converted into helium using muons. Muons are bound to carbon-12 to cause an atomic nucleus capture reaction to generate an excited boron-12 atomic nucleus, and then it may be converted into helium while transferring the excitation energy to the adjacent carbon-12 atom. Therefore, a nuclear conversion system 1EXP-SYS may be configured by irradiating and injecting muons into a carbon material containing carbon-12 to convert it into helium. (B1) An explanatory diagram of the case where muons are bound to nitrogen-15 in azane to cause a muon atomic nucleus capture reaction, which changes to carbon-15, and then nitrogen-15 is generated after the half-life of carbon-15 has elapsed. (B2) An explanatory diagram of the muon nuclear fusion of nitrogen-15. (In (B1), nitrogen-15 can be converted into carbon-15. The effective nuclear charge · Z of carbon-15 is lower than that of nitrogen-15, and it is described in combination with the consideration that the fusion reaction continues.) Note: In the sections of <Utilization of Carbon>, <Perspective when Muons are Irradiated onto Carbon-12>, and <Perspective of Adjacent Carbon Atoms and Excited Carbon Atoms> in paragraph number 0076 of the specification of this application, it is described that a carbon-12 atomic nucleus and a muon are bound, the carbon-12 atom is excited, and the excitation energy is transferred to the adjacent carbon-12 atom by excitation energy transfer to convert carbon-12 into helium (FIG. 22). In (C1) of FIG. 6, it is described that the state and excitation energy of excited carbon-12 move to the adjacent carbon-12. As a specific example, FIG. 22 is described. Although it is not written in FIG. 6 that muons are bound to carbon-12 to become boron-12, FIG. 6 shows that at least the carbon-12 atom is excited by muons, and then the excitation energy moves to the adjacent carbon-12 atom, exciting the adjacent carbon-12 atom and converting it into a helium atom. In FIG. 22, an example of the mechanism described in FIG. 6 is described in (A) of FIG. 22.) Regarding the case of muon nuclear fusion with nitrogen, boron, and hydrogen, considering the muon atomic nucleus capture reaction in the same manner as in FIG. 22, as one embodiment and assumption example of the present application, FIG. 23 shows an assumed diagram of muon nuclear fusion and muon nuclear conversion in a system in ammonia containing nitrogen-15, and FIG. 24 shows an assumed diagram of muon nuclear fusion and muon nuclear conversion in a system containing boron hydride and boron hydride anion (LiBH4) containing boron-11. (<Figure 25>Explanatory diagram of the communication system 1NUT-COM using neutrinos Symbol Explanation: 1NUT-COM: Neutrino communication system 1NUT-TX: Neutrino transmitter. TX part of 1NUT-COM. 1NUT-High: High-energy neutrino 1NUT-Low: Low-energy neutrino 2MUDECE: Decelerator 2MUCAP: Muon capture section 2MUTRAP: Muon trap section. Cosmic ray trap section, removal section. LM1Z: Muon attenuation and removal section. (With the intention of preventing cosmic rays and muons from invading the computer control unit such as the memory device and processing device in the structure 3 and transportation device 3, interfering with it, causing malfunction, or destroying it, the computer, memory device, and processing device may be placed in LM1Z within the transportation device 3. Also, in order to avoid malfunction, stop, or destruction of the communication device and detection device in 3 due to the influence of cosmic rays and muons, the communication device, input device, output device, sensor, detector, radio wave detector, particle detector, and neutrino detector may be placed in LM1Z in 3.) 1COMPUTER: Computer, calculator, electronic computer, quantum computer 1MEMORY: Memory device 1PROCESSOR: Processing device 1NETWORK: Communication network 1NUT-RX: Neutrino receiver. RX part of 1NUT-COM. 2PMT-HIE: High-energy particle, high-energy neutrino detector section 2PMT-LOWE: Low-energy particle, low-energy neutrino detector section 2SENSE: Sensor. Particle detection sensor 2PMT-CNT: Signal counter section, signal detection section 2PMT-CON: PMT control section 2NUTDET-CON: Control section. Detector control section 1NUT: Neutrino, neutretto 1NUT-BEAM: Neutrino beam 1NUT-TX: Neutrino transmitter that may also be a beam 1NUT-RX: Neutrino receiver 2MU-BY-NUT: Part that converts neutrino to muon 2MU: Muon generation section 1MU-TX: Muon transmitter 1MU-RX: Muon receiver 2MUDECE: Muon decelerator 2PMT: Photomultiplier tube 2SENSE: Sensor. Particle detection sensor. T1: Target for muons and particles. Target section for causing particles to act such as collision or combination. (Nuclear conversion of atoms by muons may be possible. The energy generated by nuclear conversion or particle decay may be detected by 2SENSE.))<Figure 26>Symbol Explanation, 3NTX-LEMT: A cosmic structure equipped with a neutrino transmitter 3NTX (the neutrino may be able to transmit neutrinos with different masses). In 2MS-NUT-GRAV or 3NRX, neutrinos of preferable mass, energy, and type (or a group of multiple types of neutrinos) for communication can be transmitted considering the effects of neutrino oscillation and gravity / gravitation. In 3NRX, while the neutrinos transmitted from 3NTX change due to oscillation and also considering the gravity of 2MS-NUT-GRAV, the mass and energy of the neutrinos can be measured. (The neutrinos when they are affected by gravity / gravitation and oscillating can be measured by 3NRX.) The neutrinos emitted from 3NTX may be a neutrino beam 1NUT-BEAM. Lepton muon neutrinos may be emitted from 3NTX. 1NUT-EMT-MIX: A collective part and orbital part of neutrinos that may contain several types of neutrinos with different masses. 1NUT-BEAM: One NUT of the beam. 1NUT-LEPTON: One NUT of the lepton. 2MS-NUT-GRAV: A part that separates neutrinos with different masses by gravity / gravitation (force). 1NUTE-ORBIT·1NUTM-ORBIT·1NUTT-ORBIT: The orbits of one NUT of neutrinos of electron (1NUTE), muon (1NUTM), and tau (1NUTT) that have different orbits due to gravity / gravitation (force) in 2MS-NUT-GRAV. 3NRX-ELEN / -MUN / -TAUN: A cosmic structure 3 with a neutrino detector (-ELEN: electron, -MUN: muon, -TAUN: subscript representing tau neutrino).)As the neutrino moves away from 2MS-NUT-GRAV, there is a possibility that the orbital and distance variations dEM and dET of the neutrino's orbital change and separation by 2MS-NUT-GRAV can be large (the distance difference dEM between the muon neutrino's orbit 1NUTM-ORBIT and the electron neutrino's orbit 1NUTE-ORBIT, the difference dET of the tau neutrino's orbit 1NUTT-ORBIT). For the purpose of taking a large difference within the vast cosmic space, a detector is equipped on the transport device 3 that can move in cosmic space, making it a neutrino-observing spaceship, artificial satellite, or structure 3NRX. The distance difference can be exploited to resolve and detect electron, muon, and tau neutrinos (by taking a large difference in position distance).) 3NRX may be equipped with a location LM1Z that attenuates cosmic rays and muons and a particle decelerator for neutrino detection. A sensor and detector may be placed within LM1Z of 3NRX to attempt neutrino detection.) <Figure 27> 4D-MUCF: Torus-shaped or annular container (which may be a plasma container, a vacuum container, or a container for solids, liquids, gases, or a pressure container), or a donut-shaped container. 4T-MUCF: Tube-shaped or cylindrical container (which may be a plasma container, a vacuum container, or a container for solids, liquids, gases, or a pressure container), or a cylinder-shaped container, a box-shaped container, or a tubular container. 1F-SYS: Fusion system, 1EXP-SYS: Nuclear conversion system, 1R: Fusion reactor, nuclear conversion reactor, furnace * In Figure 27, devices necessary for the fusion reactor of ITER's fusion reactor may be attached. For the muon fusion reactor, devices necessary for the fusion reactor, such as the supply system of T1·FEED as shown in Figures 10 to 7 and Figure 21, the power generation unit, the heat exchanger, the AEC, and the removal unit for fusion products and helium, may be attached to the containers 4D-MUCF and 4T-MUCF. (A) Annular container, view from directly above T1·FEED: Target of raw material atoms to be nuclear-converted, nuclear conversion raw material. M1: Muon, muon source, muon generation unit, irradiation unit, input unit to T1 MA1: Muonic atom, muonic atom generation unit, irradiation unit, input unit to T1 (4P-DEVICE: Device for injecting raw materials into T1·FEED which is plasma, into the 4D·container·FEED section, fuel supply section, device assisting the fusion reactor 1R) (4D-DEVICE: Device for injecting raw materials such as liquid or gas into T1·FEED, into the 4D·container·FEED section, fuel supply section, device assisting 1R,) 4D-IGNIS: Ignition device (the part that heats FEED in a thermonuclear reactor such as a CS coil and leads to the first fusion, or the muon irradiation section for leading to muon fusion first in muon fusion. Device for starting fusion, ignition section. * In the case of muon fusion, it may be a muon irradiation section, or a section that inertial-confines or magnetically confines FEED during muon irradiation and heats it. It may also be a neutral particle injection device or an FEED heating section by RF·photons) 4P-2MU: Muon irradiation section to plasma. It may also be an input section for muonic atoms and particles that bind muons to make them charge-neutral, or a neutral particle injection device. (It may include a muon decelerator) 4D-2MU: Muon irradiation section to liquid, gas, or solid T1·FEED. It may also be an input section for muons, muonic atoms, and particles, or a neutral particle injection device. (It may include a muon decelerator) LM14D: M1 introduction section, connection section to the container 4D-MUCF: Container. 4D-MUCF-ROT: Rotatable container.4D-IN: Container wall · Container wall surface. The part facing the FEED · T1 · fusion part inside the container. 4AXS: Axis of rotation of the container in the toroidal direction. In the case of the container 4D-MUCF-ROT that rotates in the toroidal direction, it is the central axis when rotating in the toroidal direction. 2COIL: Coil for forming a magnetic container. It may be a stellarator type or a helical type. A coil that forms a magnetic field in the toroidal direction. (It may include a tokamak type coil, a TF coil, and broadly, means for generating a magnetic field for confining charged particles such as muons and plasma inside the container) Stellarator · helical coil 2COIL-STR, coil for tokamak type 2COIL-TOK, TF coil, CS coil, PF coil, etc. FEED-MF: FEED inside the magnetic container · T1 T1-2BMU: Magnetic field, the magnetic field passing through the target T1. 4MFC-ORBIT: Magnetic container, a magnetic container formed in the toroidal direction around the 4AXS · Orbit of the magnetic container. 4MU-ORBIT: The state where muons are held and rotate in the magnetic container, or the magnetic container holding muons, muons held in the magnetic container. *4D-MUCF may rotate muons, charged particles, and plasma around the 4AXIS as the central axis in the 4MFC-ORBIT, T1-2BMU, and 4MU-ORBIT inside the magnetic container, or confine muons to this part. (cf: Also, as shown in FIGS. 10 to 15, insert a muon target part and a particle target part to form a 2CLP where plasma, particles, and muons orbiting around the 4AXS collide with the target part, and the particles may collide with each other to generate particles by the collision) (B) Annular container, cross-sectional view of the [A-A' section] (CS-COIL: CS-COIL when necessary) 4D-MUCF: Annular container. 4D-IN: Container wall surface. (It may be a conductor) 2COIL: Coil, TF-COIL, Helical-COIL. T1-2BMU, 4MU-ORBIT (Magnetic container, muons inside the magnetic container) 4D-MUCF-ROT: Rotatable container. (C) Cylindrical container (tubular container) 1F-SYS, 1EXP-SYS, 1R4T-MUCF: Container, tubular container 4T-MUCF-ROT: Rotatable container.M1, MA1, M1F: High-speed muons or muonic atoms 2MUDECE: Muon decelerator, decelerator for muonic atoms M1L: Decelerated muons (·muonic atoms) 4STAT: Support and fixing parts of the container (bearing 4B and container rotating part 4ROT when rotating) 2COILs-FOR-4T: Coil group for forming a magnetic field container inside a cylindrical container (The coil may be of any arrangement or container material that can form a magnetic container inside the cylindrical container.) (2ICF: Inertial confinement means part when performing inertial confinement of the T1 part. The part that compresses the T1 part with a laser or ion beam) AEC: Alpha-ray energy conversion part, charged particle direct generator (converter) (If necessary, 1TH-NZ nozzle, 1TH: Propulsion engine) 1GENR: Power generation part. It may be a part that generates electricity using light or electromagnetic waves generated by an AEC such as a photovoltaic conversion element. (Also, although the number of movable parts increases, it may also be a turbine-type power generation part that boils water to generate steam and rotates a turbine like a thermal power generation part.) 1PRPLT: Propellant (Particles generated after nuclear fusion · alpha rays, or propellant ejected by obtaining photon, particle, or their energy input generated by nuclear fusion energy) (A*) Magnetic field of the toroidal container and muon orbit 4MU-ORBIT: Orbit of the magnetic field that confines muons (·magnetic container) 2MUDECE: Decelerator (It may be possible to remotely and non-contactingly inject high-speed muons M1F into a rotating 4D-MUCF-ROT container, decelerate them in this part, and obtain decelerated muons M1L.) M1-CYCLB: Muons rotating, moving, circularly moving, helically moving, or performing cyclotron motion in T1 due to a magnetic field. 4D-MUCF-H: Container · 4D-MUCF that can generate a helical or stellarator-type magnetic container. 4D-MUCF: Container that can generate a magnetic container such as a helical or tokamak type. (In the case of a tokamak type, etc., it may be possible to heat the T1, FEED, and plasma parts using a CS coil.) <Figure 33>(B) Explanation diagram of the cylindrical containers 4T·4T-MUCF4T, 4T-MUCF, 4T-MUCF-ROT: Containers. (In this figure, it is a cylindrical container. *There is no shape limitation, and it can be a pressure vessel made of metal, or it can also be 4D, 4D-MUCF) 4T-IN: A wall surface that can be made of metal. In this figure, a thick pressure vessel metal wall surface is assumed. 2COILs-FOR-4T: Coils. For forming a magnetic container. 1NUT-TX: Neutrino transmitter, neutrino beam transmitter 2MU-BY-NUT: The part that generates muons from neutrinos (e.g., a discharge box that receives neutrinos) 2MU: Muon generation part, M1F: High-speed muons 2MUDECE: Muon decelerator T1·FEED: Nuclear conversion raw material, target part <Figure 34> Figure 34 is an assumed diagram of the reaction example "CD4 + muon -> 12C + D -> 14N + D -> 16O* -> 12C + 4He", in which methane (hydrocarbon, CD4) composed of deuterium D and carbon 12 is irradiated with negative muons, the negative muons are bonded to carbon 12 in the methane, D in the methane CD4 fuses with carbon 12 to form nitrogen 14, then deuterium D bonds to the nitrogen 14 to form an excited oxygen nucleus 16O*, and the 16O* is converted into carbon 12 and an alpha particle. In Figure 34, it includes an explanation diagram of the case where "CD4 + muon -> 12C + D + muon -> 14N + D + muon -> 16O* -> 12C + 4He + muon" is repeated twice in CD4 and the overall reaction formula becomes "CD4 + muon -> C (carbon 12) + 2×He (helium 4) + muon". Since two Ds are bonded to 12C in CD4 to form an excited oxygen nucleus and then return to the carbon 12 nucleus again, the reaction formula for bonding negative muons to methane CD4 described in Figure 34 is "a muon-based nuclear conversion system having a step of bonding a muon to a raw material atom to obtain an excited nucleus and then converting it into an atom having a smaller effective nuclear charge or atomic number than the raw material atom", and the raw material atoms are carbon 12 and deuterium D in the methane molecule composed of carbon 12 and deuterium. <Fig. 35><System for fusing fluorine atoms and hydrogen atoms within a molecule, in the case of fusing adjacent H and F in a PVDF resin, P-19F system>Fig. 35 is an explanatory diagram of the case where polyvinylidene fluoride PVDF (which may be PVDF composed of hydrogen, fluorine 19, and carbon) is used as the target part T1 and the muon decelerator 2MUDECE for the dielectric 2LZI of the electric field forming element 2FDELE of the muon decelerator 2MUDECE in Fig. 20, and the target and decelerator part T1-With-PVDF-2MUDECE is formed. The target and decelerator part T1-With-PVDF-2MUDECE contains carbon, fluorine, and hydrogen within the resin and within the molecule, and the fluorine and the hydrogen are polarized when an external potential difference and electric field are applied to PVDF, and there is a part where fluorine and hydrogen are close to each other between the chain parts of the PVDF molecules (the part T1-Hu19F in Fig. 35 where F and H are surrounded by a round dashed frame). (Or it may have a bonding part due to the intermolecular force between fluorine and hydrogen in the PVDF resin.) Electrodes 2ER (sheet A) may be attached to both ends of the dielectric part 2LZI using PVDF of the target and decelerator part T1-With-PVDF-2MUDECE (sheet B). The target and decelerator part T1-With-PVDF-2MUDECE may be applied with a potential difference and voltage from the outside, and the muons irradiated from the muon source M1 are decelerated by the electric field generated in T1-With-PVDF-2MUDECE, and the decelerated muons are combined with the part where the hydrogen and fluorine are close to each other in T1-With-PVDF-2MUDECE (T1-Hu19F) (or the fluorine and hydrogen atomic parts of the bonding part due to the intermolecular force between fluorine and hydrogen) to constitute a fusion system 1F-SYS that promotes muon nuclear fusion between the hydrogen and fluorine. In the configuration of Fig. 35, it is a configuration in which an attempt can be made to cause nuclear fusion between fluorine and hydrogen between adjacent fluorine and hydrogen in a solid PVDF resin that is non-corrosive and non-toxic like hydrogen fluoride. When PVDF is used for the target part T1, it can also serve as the electric field forming element 2FDELE and capacitor element for the muon decelerator and the target and fuel part T1.*Note that in FIG. 35, a configuration is described in which PVDF is used as the insulating part, dielectric part, and piezoelectric part (or pyroelectric part) of the capacitor element and the electric field forming element 2FDELE for electric field formation. For example, in the laser wake field LWF of FIG. 18, an electric field 2LASER-EF of the laser wake field is formed in the material part, and muons are decelerated by the electric field 2LASER-EF, and then muons are combined with T1. When PVDF is used for T1, compared with the case of using hydrogen fluoride HF for T1, PVDF is non-toxic like hydrogen fluoride, non-toxic, does not require pressure and container management as a pressurized gas, and is easy to install, arrange, and hold as the target part T1 of the laser irradiation part for both the muon irradiation part and the laser wake field generation. Therefore, in the present application, a fusion system 1F-SYS or a nuclear conversion system that fuses fluorine and hydrogen in PVDF using muons may be configured. (*In FIGS. 35 and 36, an attempt is made to decelerate muons in the T1-With-PVDF-2MUDECE part, guide muons to H and F in PVDF, combine them, and cause muon nuclear fusion. *In FIG. 36, the coil 2COIL confines the muons decelerated in the T1-With-PVDF-2MUDECE part in the magnetic container 2MAGC. T1 is inside the magnetic container 2MAGC, and the muons are directed to continuously diffuse T1 inside the magnetic container 2MAGC generated by the coil 2COIL so that the muons do not escape from T1. The coil prompts the muons to be confined in the T1 part and continue to be detained and diffused in the T1 part. The coil 2COIL passes a current for magnetic field generation through the coil by the coil power supply part 2PWSP-COIL and its control part). <When placed in a coil, a magnetic container, and a magnetic field>*In FIG. 36, 2MUDECE, which is also T1 using PVDF, T1-With-PVDF-2MUDECE, is stored in a magnetic container 2MAGC formed by a coil 2COIL. *As one form, the magnetic container may be a tube type or may be formed by a helical coil 2COIL, 2COIL-Helical. (For example, a tube type container 4T or a rotatable tube type container 4T-ROT is provided with the helical coil 2COIL-Helical described in FIG. 36 to form containers 4T-H, 4T-H-ROT. A twisted magnetic container part or a helical magnetic container stores a target part T1, and muons are irradiated onto the T1 part in the magnetic container to bind muons to T1.)<Resins and compounds containing fluorine, hydrogen, and carbon>In one form of the present application, a resin or compound containing fluorine, hydrogen, and carbon may be used. (An example thereof is PVDF. PVDF can also be used as a dielectric, insulator, piezoelectric, and pyroelectric.)(It is possible to attempt muon nuclear fusion between molecules of a substance, atomic molecular group containing hydrogen and fluorine.)When comparing VDF and PVDF, PVDF is formed from gaseous VDF by polymerization into a solid polymer or resin, and by bringing hydrogen and fluorine atoms close to each other within the solid polymer, there is an advantage that there is no toxicity such as HF. *It is also possible to attempt to make fluoromethane and difluoromethane (gases at normal temperature and pressure) into liquids or solids, bring hydrogen and fluorine close to each other between the fluoromethane molecules, bind muons to the proximity part, and promote muon nuclear fusion. (For example, HFC, hydrofluorocarbon, which is also used as a refrigerant, and simple ones such as CH2F2 and CH3F. In the liquid or solid of CH2F2, it is only necessary that adjacent hydrogen and fluorine between CH2F2 molecules can be brought close to a distance where muon nuclear fusion is possible, but if they cannot be brought close enough, there is a possibility that muon nuclear fusion will not occur.)When considering CH2F2 simply as a substance containing hydrogen and fluorine fuels (when considering CH2F2 as a non-toxic hydrogen fluoride nuclear fusion fuel gas like hydrogen fluoride), for example, when used in a laser track field generation as shown in Fig. 18 or in the laser-irradiated target T1 part for an inertial confinement fusion reactor by a laser, it may be attempted to laser-heat CH2F2 molecules, move the molecules and intra-molecular atoms, decelerate and bond muons, and cause muon nuclear fusion and laser confinement nuclear fusion). *According to the following document PF1, it is known that the dielectric breakdown strength of PVDF varies depending on the manufacturing method of the resin, its thickness, temperature, voltage application method, and pulse. (Refer to the document claiming priority of this application.) When forming an electric field for muon deceleration, PVDF can potentially have a high dielectric breakdown strength while containing fluorine and hydrogen within its molecule, which can also serve as a muon nuclear fusion target part for fluorine and hydrogen. Therefore, it may be used in the system, decelerator, and target part of this application. For PVDF with a thickness of submicron or 0.4 micrometers or less, electrodes (such as metal lithium and carbon conductive materials with low Z) are deposited by methods like vapor deposition and sandwiched with electrodes to form a PVDF capacitor 2FDELE-PVDF or a laminated PVDF film capacitor 2FDELE-LAM-PVDF, similar to a multilayer film capacitor or capacitor. An electric field can be applied to the capacitor to use it as a muon decelerator and a target part T1 for muon bonding. *Stacking submicron PVDF film capacitors may potentially form a capacitor laminate device 2FDELE-LAM-PVDF-1M with a length of 1 meter, which can serve as a capacitor, muon decelerator, and muon catalytic fusion fuel target part T1 with a withstand voltage of 2 GV. Cosmic muons have a kinetic energy and speed in the GeV class. If the capacitor laminate device 2FDELE-LAM-PVDF-1M can form an electric field of 2 gigavolts within the device, there is a possibility of decelerating GeV-class negative muons. There is also a possibility of separating positive and negative muons within cosmic muons with different charges within the device 2FDELE-LAM-PVDF-1M. It is assumed that positive muons are accelerated or pass through the device 2FDELE-LAM-PVDF-1M, while negative muons are decelerated within the device 2FDELE-LAM-PVDF-1M. *The device 2FDELE-LAM-PVDF-1M may be cooled. (It may be immersed in a low-Z solvent (e.g., liquid helium). At low temperatures, even if one wants to convert the alpha-ray energy generated after fusion into electricity using a heat exchanger HX, steam turbine, etc., heating liquid helium with alpha rays will make it unsuitable for PVDF cooling at high temperatures and high pressures, which may not be preferable. In such cases, it may be preferable to convert alpha rays into gamma-ray and photon energy by AEC for photoelectric conversion.)Solvents with a lower Z than fluorine in PVDF, such as liquid nitrogen N2, can be considered. The atomic number Z is smaller for He than for N in N2, and there is an expectation that muons are less likely to be trapped. A refrigerant for cooling consisting of low-Z atoms is also envisioned.). *In this application, it might be possible to express that the means for bringing atoms to be fused at T1 close to each other is carried out in two steps. In the first step of the means for bringing atoms close to each other, means for bringing atoms close to each other such as bonding atoms to each other like in an HF molecule or bringing them close to each other intermolecularly like H and F between PVDF molecules can be utilized. As the second step of the means for bringing atoms close to each other, muons are bonded to the atoms that are close to each other in the first step instead of electrons. Due to the weight of muons being about 200 times that of electrons, the two atomic nuclei in the muon molecule can be made to approach each other easily, and an attempt is made to cause nuclear fusion.) *In another example of the expression in this application, in order to cause nuclear fusion between atoms, first, atoms to be fused are brought close to each other to the distance between molecules - intermolecularly by including atoms for nuclear fusion within the molecule - intermolecularly, and the atoms have an arrangement of atoms that are close to each other within or between molecules. Muons are bonded to the arranged portion of the atoms that are close to each other, and an attempt is made to cause muon nuclear fusion between the atoms. <Figure 36>Figure 36 is an explanatory diagram of a cylindrical container 4T, in which a magnetic confinement coil 2COIL can form a helical magnetic container 2MAGC inside the container using the helical coil, i.e., a cylindrical container 4T-H (or a rotatable cylindrical container 4T-ROT-H in the theta direction). *The coil 2COIL, the reducer, and T1 may be stored in the cylindrical container 4T, for example. *The 2COIL may be a helical coil 2COIL-Helicals (Helical-COILs). *The solenoid coil may be inclined diagonally with respect to the longitudinal axis to form a helical coil (helical solenoid). In a normal solenoid coil, the coil loops are generally shown perpendicular to the longitudinal direction (the length direction of the axis of 4AXS-4T-TH) as shown in COIL of Fig. 33(A). Generally, when referring to a solenoid, the coil is often wound perpendicular to the longitudinal direction. However, the winding direction of the coil with respect to the longitudinal direction of the coil may have an angle so that the solenoid has a helical winding. (@Regarding a donut-shaped helical fusion reactor (LHC in Japan, W7-X in Germany), a means for closing both ends is combined with a part of the toroidal loop cut out and opened into an open-ended, tube-shaped object. )(The helical donut-shaped container 4D-TH includes a combination of a magnetic field in the toroidal direction, the longitudinal direction of the donut, and a magnetic field twisted in the poloidal direction of the donut. In a tokamak type, a toroidal magnetic field is formed by a TF coil, and a plasma current is passed through the plasma inside the donut by a CS coil to generate a magnetic field in the poloidal direction to form a helical magnetic container)* In the present application, in a donut-shaped container 4D or a tube-shaped cylindrical container 4T, a helical coil or a cage of a helical magnetic field, i.e., a magnetic container, may be formed, and charged particles, positive and negative muons, and plasma may be confined therein, or T1 may be arranged inside the container. *The coil and the magnetic container may be provided with a rotating means of the device such as a rotating means 4ROT, a bearing portion 4B, and a joint portion (e.g., a slip ring) for supplying power to the rotating coil and the reducer, so that the coil, the container, and the magnetic container portion (the container wall) may be rotatable in the theta direction.(*Both ends of the helical solenoid coil portion may be arranged such that the winding radius narrows toward both ends like those of a shellfish, a conch shell, or a croissant, and then the solenoid wire is taken out to the external coil power circuit side. The helical solenoid coil may confine charged particles or muons with a magnetic field and an electric field like a tandem mirror type device. There may be provided a cylindrical container 4T-H (a cylindrical container for muon fusion and a furnace including a helical solenoid, a coil, a magnetic container, and a magnetic field confinement portion 2MAGC) which is a cylindrical container 4T and in which a magnetic confinement coil 2COIL can form a helical magnetic container 2MAGC inside the container using the helical coil.*) <Figure 37><Arrangement example of a decelerator and fuel T1 using a capacitor element made of a material that may be PVDF>An arrangement example of the decelerator is described in FIG. 37. FIG. 37(A) is an explanatory diagram when a voltage application power supply 2PWSP is connected to a capacitor element and a deceleration element 2FDELE-LAM-PVDF-1M which may be of a size of about 1 m class. The 2PWSP is connected to an electric circuit 2ELECIR and a computer control unit 2CON, and is controlled by the 2CON to generate a DC or pulsed operation or AC voltage and apply a DC, pulsed, or AC voltage to the element 2FDELE-LAM-PVDF-1M. (The 2PWSP may be capable of generating and applying a gigavolt voltage.) Muons M1 which may be cosmic muons SM1 or high-speed muons M1F are incident on the 2FDELE-LAM-PVDF-1M to which a voltage is applied, and the M1F is decelerated by the electric field inside the element 2FDELE-LAM-PVDF-1M to become a decelerated muon M1L, and the M1L can be bonded to an atom inside the element 2FDELE-LAM-PVDF-1M, for example, a fluorine atom. Then, an attempt may be made to cause muon fusion and nuclear conversion between the fluorine atom and the adjacent hydrogen atom. <Fig. 38> As shown in Fig. 38, 2FDELE-LAM-PVDF-1M may be used as a negative muon decelerator. The element 2FDELE-LAM-PVDF-1M may be used as a positive muon accelerator. The high-speed negative muon M1F may be decelerated by the said element to become a negative muon M1L and guided to be combined with the target T1. The high-speed positive muon M1F may become a positive muon M1FA accelerated by the said element 2FDELE-LAM-PVDF-1M, pass through the element, and be emitted outside the element. The accelerated positive muon M1FA may then be collided with the TGT part and the particle collision part 2CLP of the muon target 2MU to generate muons, leptons, and particles. The M1FA of the positive muon may collide with, for example, electrons in an atom to generate pairs of positrons and electrons, positive and negative muons, and leptons as occur in a lepton collider. Also, when a positive muon collides with a proton, nuclear fragmentation, mesons, pions, kaons, etc. may be generated. * The element 2FDELE-LAM-PVDF-1M with a voltage applied to form an electric field may be arranged to decelerate the incident negative muons with a velocity, and in that arrangement, the positive muons may be accelerated in a direction opposite to that of the negative muons. The element 2FDELE-LAM-PVDF-1M is an accelerator and decelerator for positive and negative muons (depending on the application, electrons, positrons, positive and negative muons, positive and negative tauons, leptons, charged particles). The element 2FDELE-LAM-PVDF-1M is also a separator for positive and negative muons (depending on the application, positive and negative leptons, positive and negative particles). * The element 2FDELE-LAM-PVDF-1M may accelerate positive muons (charged particles) depending on its arrangement and the way the electric field is formed. For example, while attempting to decelerate negative muons among the positive and negative muons of cosmic muons with the element 2FDELE-LAM-PVDF-1M and combine them with T1, it may also be operated as an accelerator that accelerates positive muons and collides them with a particle collision target such as electrons, atoms, particles, or a muon target. <Fig. 39> Fig. 39 is an explanatory diagram of a configuration in which a plurality of 2FDELE-LAM-PVDFs are installed as decelerators to decelerate muons each time they pass through each 2FDELE-LAM-PVDF, and the decelerated muons can be combined with a target part T1·FEED (fuel substances such as T1 containing hydrogen and oxygen-18, T1-H2O, T1-D2O containing deuterium and oxygen-16, T1-NH4 containing nitrogen-15 and hydrogen, T1-ND4 containing nitrogen-14 and deuterium, etc.) different from the decelerator. In Fig. 39(A), high-speed muons are decelerated by a plurality of 2FDELE-LAM-PVDFs and then combined with T1. At that time, a muon capture part 2MUCAP for capturing muons is arranged between T1 and the plurality of 2FDELE-LAM-PVDFs, and M1L decelerated by 2FDELE-LAM-PVDF is captured and transported by 2MUCAP (2MUCAP can generate a magnetic field by a magnetic field generation means such as a coil 2COIL or a solenoid to capture and transport muons) and transported to T1 to combine T1 and M1L. Fig. 39(B) is an explanatory diagram of a configuration in which a target T1·FEED (for example, assuming T1 is not PVDF but another substance, ammonia NH4·ND4, water H2O·D2O, NaH·AlH3, etc. to be described later, T1-NaH, T1-AlH3 are also assumed) is inserted between the arrays of the elements 2FDELE-LAM-PVDF. In Fig. 34F(B), for example, the element 2FDELE-LAM-PVDF and T1 are alternately arranged, and negative muons enter the alternating arrangement part 2FDELE-T1-ARRAY of the element 2FDELE-LAM-PVDF and T1 from the left side and cross the arrangement part. On the way of crossing the element 2FDELE-LAM-PVDF, the negative muons are decelerated, and it is an explanatory diagram of a configuration in which the muons try to combine with the T1 part (fuels such as T1, T1-NH4, T1-H2O, T1-NaH, T1-AlH3, etc.) even when they are in the process of being decelerated.In the figure, three T1s are inserted between four elements in the alternating array section 2FDELE-T1-ARRAY. However, the repetition numbers of the elements and T1 do not have to be limited to the representation in the figure. For example, sub-micron elements and 1-micron fuel T1 parts can be alternately arranged over a length of 2 meters (for example, a set of 2-micron-thick elements and T1 can be arranged in, say, 10^6 or 1 million layers over 2 meters) to obtain the alternating array section 2FDELE-T1-ARRAY. An electric field can be applied to each element of the alternating array section to decelerate negative muons and muons in the element part, and the muons decelerated in the T1 part arranged adjacent to the element can be combined. <Figure 40>Figure 40 is an explanatory diagram of the cube device 2MUDECE-R3D. A deceleration electric field in the three-dimensional XYZ directions is formed by applying a potential to the electrodes to decelerate cosmic muons and attempt muon deceleration. It can also be used to accelerate leptons such as muons and electrons with opposite charges. <Figure 41><Meteorite Orbit Change Device Using the Energy of the Muon Fusion System>As shown in Figure 41, for a meteorite MTO that can fall to the Earth, a transport machine 5 or a robot 5·5WKR for meteorite interception can be configured to SET·attach a container 4T-MUCF carrying the muon fusion fuel such as methane CD4·B2H6·ND3·etc. to the meteorite MTO. <Figure 42><Configuration for Excavating a Meteorite and Generating Energy Inside the Meteorite by Nuclear Fusion>An attempt can be made to change the orbit of the meteorite by hitting it with a mass driver 3·a centrifuge gun (·a device for hitting a mass). (The DART mission by NASA, which hits a meteorite with a spacecraft to change the meteorite orbit, is known and has been implemented.) And for meteorites flying towards the Earth, using energy from nuclear fission or fusion for blasting is also being considered. If the time until collision avoidance is short (less than 10 years), it may be considered to blast the meteorite with a nuclear weapon to divide the mass and deflect the fragments of the meteorite from the Earth, or to reduce the mass of the meteorite fragments flying towards the Earth so as not to receive a fatal damage. <Placement and driving of nuclear fuel deep into the ground>*It may be possible to project and launch a nuclear fuel with a hammer or a hammer part and a load with a muon generation part (3LOAD) from a centrifuge gun (a structure including a centrifuge gun part and a mass driver part such as 3, 3SPINFSAT), strike the hammer against a meteorite part, and try to drive the hammer into the meteorite like a pile driver to make a hole. After the hammer strikes and the 3LOAD penetrates into the meteorite and advances to the inside, from the outside, using a mechanism such as neutrino communication, irradiate the muon generation part and the nuclear fuel left in the iron meteorite with neutrinos or ignition particles. The ignition particles generate muons, the muons bind to the fuel T1, cause muon fusion, and cause an explosion or blast inside the meteorite. (To investigate where the fuel is driven into the meteorite, it may be possible to obtain a CT of the meteorite after fuel injection using muography or particles such as neutrinos to confirm the distribution of the injected fuel)*The muon generation device, muon deceleration device, and nuclear fuel T1 that make up the muon fusion and muon nuclear conversion system 1F-SYS / 1EXP-SYS of the present application may be mounted on a load 3LOAD (missile, rocket, warhead) projected by a projection means such as a centrifuge gun 3SPINFSAT. It may also be possible to accelerate and project a 3LOAD including a bullet (e.g., a long bullet like a pile or a nail) with the penetrability of a tank gun, bullet, armor-piercing fin-stabilized discarding sabot (APFSDS) that penetrates metal or ceramic armor from the surface side of the meteorite to the inside of the meteorite. (The kinetic energy K of the bullet 3LOAD is K = 1 / 2 × the square of the velocity v of the bullet) A nuclear fusion fuel part T1, a muon generation part 2MU·2MU-BY-NUT, a muon deceleration part, and a part capable of decelerating and binding muons to the fuel may be mounted on a 3LOAD that is a penetrating bomb or penetrating warhead accelerated at high speed like a penetrator bomb. In the device of the present application, a solid nuclear fusion fuel T1 (e.g., (C2D4)n of hydrocarbon resin, lithium borohydride LiBH4) is described. When driving a bullet 3LOAD with penetrability into an iron meteorite MTO, the material of the bullet (accelerated by a centrifuge gun 3SPINFSAT and possibly described as a speed such as X% of the speed of light) may be, for example, hydrocarbon resin.Install a solid nuclear fusion fuel and a muon generation unit (a nucleus that generates muons by neutrinos) inside the armor-piercing projectile, and try to push the armor-piercing projectile into the iron meteorite by the inertia and pressure of the armor-piercing projectile as it penetrates the iron meteorite. Using the material of the projectile that penetrates the surface and armor of the MTO as fuel·T1, if there are nuclear fusion fuel and neutrino·muon generation units in the projectile, it may be possible to irradiate the remaining T1 part of the projectile type embedded in the metal with neutrinos and cause muon nuclear fusion. (As shown in (B) of Fig. 45, after driving the T1 nuclear fuel projectile 3LOADT1(balls) into the metal meteorite, a projectile with a muon generation part·nucleus·particle 2MU-GEN-ATOM may be driven in.) At least, it may be possible to drive a projectile of nuclear fusion fuel accelerated in the metal body of the meteorite, leave the projectile·nuclear fusion fuel in the metal, and place the fuel T1. (Since it is inside the metal, transmit muon-generation particles that can penetrate the metal to the T1 part and the muon generation part), and if muons can be combined with the placed fuel, muon nuclear fusion may occur. *The surface is also assumed to be surrounded by a case of, for example, carbon-12 diamond, carbon fiber, BN·BNNT to increase the strength of the projectile case. * Try hitting the projectiles ejected from the centrifuge gun·mass driver continuously against the metal surface like a pile-driving hammer·pile (or as a hammer ball instead of the sand in sandblasting) to break, crush, and remove the metal surface part and dig in. <Fig. 43> Fig. 43 is an explanatory diagram showing the transmission of neutrinos·muons·particles from the particle transmission unit 5BTX (which may be multiple units) for detonation attached to the transportation device 5SHIP or the iron meteorite MTO toward the particle reception unit 5BRX in the hole 5T-HOLE. The neutrino transmission unit·particle transmission unit 5BTX for detonation attached to the iron meteorite MTO may be equipped with a communication unit·radio wave reception unit 5TX-RAD using radio waves, transmit and receive the detonation signal from 5SHIP, etc. by radio waves·wireless using 5TX-RAD, and then operate the neutrino transmission unit 1NUT-TX of 5BTX from the radio wave wireless signal to transmit neutrinos to 5BRX(2MU-BY-NUT). <Fig. 44> Fig. 44 is an explanatory diagram showing the formation of a muon fusion section near the iron of the excavation head section 5REMV-HEAD by supplying nuclear fusion fuel T1 such as methane or ammonia to the material section and iron section of the meteorite, injecting muons, and decelerating them with the excavation body section 5REMV-BODY (FP section and MLTFE of Fig. 48). <Fig. 45> Fig. 45 is an explanatory diagram of projecting and firing a hammer or a nuclear fuel with a hammer part and a load with a muon generation section (3LOAD) from a centrifuge gun (a structure including a centrifuge gun section and a mass driver section such as 3SPINFSAT), hitting the hammer on the meteorite section like a pile driver to make a hole in the meteorite. Also, it is an explanatory diagram of driving nuclear fuel T1 (·2MU-GEN-ATOM) and a load with a muon generation section (3LOAD) into an iron meteorite by the acceleration projection means of a load such as a centrifuge gun, irradiating the implanted T1·2MU-GEN-ATOM with neutrinos to generate and bind muons to the T1 section to cause muon fusion inside the meteorite. <Fig. 46> In Fig. 46, for example, it may be attempted to manufacture a plurality of fiber material parts 2NTLP such as closed carbon nanotubes CNT or boron nitride nanotubes BNNT at both ends of a loop, ring, or circular shape, and form a chain 2LPST composed of 2NTLP. If we describe 2LPST, it is like the pattern of "different angles, different corner-cutting angles, different circles" of a family crest, combining a plurality of corners, circles, rings, and loops in a chain-like manner to form a continuous 2LPST that combines the starting loop 2LPST and the ending loop 2LPST, and this 2LPST can be used for the frame, cable, and structural part 2LPST that can withstand the centrifugal force when 3SPINFSAT rotates. 2NTLP may enclose a wire, tube, loop, or ring part 2NTLP-I2 made of another material (such as metal or alloy). 2NTLP·2NTLP-CHAIN may enclose a wire, tube 2NTLP-I2 made of another material or atomic and molecular parts. 2NTLP may also be a hybrid material that can withstand centrifugal force and includes a wire, tube, loop, or ring part 2NTLP-I2 made of another material. By adopting the above configuration, an attempt is made to use it as the frame and structural material for parts that require strength, such as the centrifugal gun or the wire part of the orbital elevator. 2NTLP encloses a continuous wire, tube, loop, or ring part 2NTLP-I2 made of another material (such as metal or alloy). Since the material is the wire, tube, loop, or ring part 2NTLP-I2, even if the tube part of the 2NTLP part enclosing 2NTLP-I2 breaks due to deterioration or the like, the internal wire tube part remains, and the connection can be maintained because the metal nanotube ring part remains.The chain 2NTLP-CHAIN composed of 2NTLP uses a plurality of chain groups 2NTLP-CHAINs in actual use in a centrifugal gun, an orbital elevator, etc., and bundles them to withstand centrifugal force, weight, and mechanical force. It constitutes a (macroscopic) rope, cable, ribbon, string, and frame part 2LPST composed of nanotube chains. However, there is also a possibility that the atoms in the BNNT and CNT parts of 2NTLP are sputtered or chemically reacted by cosmic rays, atomic oxygen AO, etc., resulting in a decrease in strength and breakage. Even if one 2NTLP or 2NTLP-CHAIN breaks, the chain does not leave the wire, tube, loop, or ring part, but remains intertwined. Therefore, it may be a hybrid ring 2NTLP or chain 2NTLP-CHAIN that includes a metal or alloy wire part in 2NTLP. Even if a certain ring 2NTLP (A) in a certain chain 2NTLP-CHAIN (C) breaks or the tube bursts, as long as the 2NTLP-I2 (A) contained in 2NTLP (A) does not break, the contained 2NTLP-I2 (A) combines with another adjacent and combined 2NTLP (B) as a chain, so the chain (C) containing them can be arranged in the chain group 2NTLP-CHAINs without breaking immediately and remaining intertwined and immobile. For example, when maintaining the chain group, if there is a camera part or an X-ray observation part 2LPST-MEAS for observing the chain part or the chain group, the chain structure 2NTLP-I2-CHAIN of the metal part 2NTLP-I2 is maintained, and it is also possible to see whether the high-strength tube part 2NTLP such as BNNT breaks or has a tendency to be damaged during actual use. (When maintaining the chain 2NTLP-CHAIN, by putting the metal wire 2NTLP-I2 inside the ring part 2NTLP of the components of the chain 2NTLP-CHAIN, when observing with X-rays, by using the fact that the metal atoms in 2NTLP-I2 have a high Z in the X-ray observation image, the metal wire 2NTLP-I2 can absorb X-rays more strongly than BNNT or CNT, and the X-ray CE image shows shades, which can be used to check whether the metal wire part 2NTLP-I2 is broken or whether the loop or tube 2NTLP containing it is damaged. It can be advantageous for grasping the criteria during maintenance, state observation, quality confirmation, and chain replacement of the chain part or chain group part 2NTLP-CHAINs. Therefore, in one form of the present application, it may include a metal wire.))In addition, when obtaining transmission image CT of BNNT or CNT composed of low-Z atoms and observing their structure and degradation state, in addition to X-ray, X-ray CT, and X-ray application measurement means, muography, muon microscope, and muon application measurement means using muons may also be used. Gamma rays and X-rays of photons are easily absorbed by high-Z elements such as metals, but are hardly absorbed by low-Z atoms. On the other hand, muons, for example, positive muons with a positive charge, are leptons with mass. When the muons irradiated with the low-Z atomic nuclei or high-Z atomic nuclei (and protons and neutrons in the nuclei) of the object to be observed by muography collide with the muon leptons, the muon leptons change their orbits and their states are detected by a detector, so that the object can be observed. Therefore, it can be used for observing the object (the ring part 2NTLP, the chain part 2NTLP-CHAIN, the chain group part 2NTLP-CHAINs, and the frame part 2LPST). * 2NTLP-CHAIN and 2NTLP-CHAINs may be used for cables, chains, wires, ropes, and ribbon parts that require strength, such as centrifugal guns and orbital elevators. * It is preferable that a single seamless CNT or BNNT can be synthesized into a loop for one rotation of the centrifugal gun (similarly, when used for an orbital elevator or the like, it is preferable that a seamless tube can be formed over a wide distance). However, in case it cannot be synthesized, if the ring-shaped BNNT tube, the ring part 2NTLP without joints can be combined into a chain to form a chain 2NTLP-CHAIN, each 2NTLP constituting the chain can exhibit the strength of seamless CNT or BNNT, and the chain may also (although it is not chain-shaped and should be stronger if it is a straight tube, as a compromise point) be able to exhibit the strength of CNT or BNNT as a chain device. Therefore, in the present application, a chain 2NTLP-CHAIN composed of a ring 2NTLP as shown in FIG. 46 can be constructed and used for the frame part of a structural material or system that requires strength, such as a centrifugal gun. * 2NTLP-CHAIN may be encapsulated in another nanotube. * 2NTLP-CHAIN and 2NTLP-CHAINs may be coated with another material to prevent reaction with atomic oxygen and protect against cosmic ray collisions. For example, it may be covered with a ceramic or insulator tube for insulation, or may be covered with a metal film or tube for protection against atomic oxygen and cosmic ray collisions.*2NTLP, 2NTLP-CHAIN, and 2NTLP-CHAINs may be components of an electric wire (e.g., the power transmission wire of an orbital elevator). [*If 2NTLP (·2NTLP that may include 2NTLP-I2) can be made large over a macro length such as the size of an orbital elevator or a centrifugal gun 3SPINFSAT, 2NTLP (·2NTLP that may include 2NTLP-I2), which is a continuous loop portion, may be included in and used with the loop-shaped frame portion 2LPST. *However, in case it is difficult to create a nanotube loop with a length over a macro length such as the size of an orbital elevator or a centrifugal gun (e.g., a length on the scale of kilometers to 100 kilometers or more from the ground to outer space, where the radius of the loop is not at the nano level or micro level but macro), a frame using 2NTLP-CHAIN may be considered.]

[0022] This application claims the benefit of priority to Japanese Patent Application No. 2024-082974, filed on May 22, 2024, the entire disclosure of which is incorporated herein by reference. <Document Name>Specification of Japanese Patent Application No. 2024-082974<Invention Title>Nuclear Conversion System<Technical Field> <0001><Technical Field> The present invention is an invention related to nuclear power. The present invention relates to a muon-catalyzed nuclear fusion system. (An application based on an idea that requires verification)<Background Art> <0002> As described in Non-Patent Document 1, the muon-catalyzed nuclear fusion method (muon-catalyzed nuclear fusion) is known. <0003> A hydrogen molecule containing deuterium D or tritium T is used as a liquid, and muons are introduced into it, causing a nuclear fusion reaction as if the muons act as a catalyst for nuclear fusion. However, in a hydrogen molecule, the charge of the nucleus after nuclear fusion increases from +1 of a hydrogen atom to +2 of a helium atom, and the muon is captured and trapped by the Coulomb force by the nucleus with a +2 charge, the helium nucleus, and the alpha particle nucleus, resulting in the problem that the muon-catalyzed nuclear fusion stops (making it difficult to react). <0004> According to Non-Patent Document 2, a thermonuclear fusion method using protons and boron is known. In a thermonuclear fusion reactor, high-energy neutron rays that can radiate the nuclear fusion reactor in D-T and D-D reactions are a problem. As an example of solving this problem, a system that does not emit neutrons, is difficult to do so, and uses protons and boron (P-11B system, proton-boron system) has been studied. When performing the P-11B system in a thermonuclear fusion reactor, there is a problem that the temperature at which thermonuclear fusion occurs needs to be 10 times higher than that of the D-T system.<Prior Art Documents><Patent Documents> <0005> <Non-Patent Document 1>High Energy Accelerator Research Organization KEK, Muon-Catalyzed Nuclear Fusion [Internet, Web Page, URL: https: / / www2.kek.jp / imss / msl / muon-tour / fusion.html, Accessed on September 18, Reiwa 5]<Non-Patent Document> <0006> <Non-Patent Document 2>Nuclear Fusion Science Institute NIFS, Demonstration of Fusion Reaction Using Advanced Nuclear Fusion Fuel - The First Step Towards a Clean Fusion Reactor Utilizing the Light Hydrogen-Boron Reaction that Does Not Generate Neutrons - [Internet, Web Page, URL: https: / / www.nifs.ac.jp / news / researches / 230309-01.html, Accessed on September 18, Reiwa 5]<Summary of the Invention><Problems to be Solved by the Invention> <0007> The problem to be solved is that in the system of muon-catalyzed nuclear fusion using hydrogen atoms and hydrogen molecules, muons are captured and trapped by the Coulomb force, causing the muon-catalyzed nuclear fusion to stop (making the reaction difficult). Also, in systems using deuterium D, tritium T, etc. in muon nuclear fusion, neutrons that may irradiate the members of the fusion reactor or fusion system are generated, but there may be a system that does not generate neutrons.<Means for Solving the Problems><0008> In muon-catalyzed nuclear fusion, it is desired to bring muons close to hydrogen atoms, which are the fuel substances before nuclear fusion, for nuclear fusion. However, the helium nucleus of the nucleus after nuclear fusion has a higher charge than the hydrogen nucleus before nuclear fusion, making it easier to capture muons. Therefore, in the present invention, as a system that reverses this charge change, a system using protons and boron is disclosed as System 1 in FIG. 1. Also, an assumed example of a spacecraft 3 and a transportation device 3 equipped with it is shown in FIG. 5.<0009> As the intention of FIG. 5, a spacecraft or a space exploration robot 3 that travels between stars and planets may be required to generate electricity and propulsion using the fuel carried on the spacecraft even in interplanetary and interstellar space where sunlight and starlight do not reach. Against this background, it was considered that if the vacuum environment of the universe could be used to operate a particle accelerator to generate muons and protons to construct a fusion reactor and a fusion thruster as a power source.<0010> Also, although there is a possibility of neutrons being emitted, as (2) from another perspective of the present invention, as an example not limited to the system using proton boron, a system using protons and lithium, etc. is also disclosed.The intention of disclosing a lithium-based system is that lithium has a lower melting point than boron and is easily heated to form liquid lithium. On the other hand, for a system using boron, it is necessary to heat it to a temperature exceeding 2000 degrees Celsius as the melting point of boron. <0011> The present invention focuses on the fact that in a proton-boron fusion reaction system (P-11B system), the charge of the boron atomic nucleus serving as the fusion fuel is +5, and the charge of the helium generated after fusion is +3. The P-11B system is a system in which the charge of the atomic nucleus decreases when the fusion reaction occurs from boron to helium. (*On the other hand, as described above, the D-T system is a system in which the charge increases after fusion and trapping occurs.) <0012> In Figure 1 of this application, the following reaction is assumed. (Not proven) 1. A proton with a charge of +1 collides with a boron atomic nucleus with a charge of +5 that has captured a muon with a charge of -1 (a muon molecule containing boron) to initiate a fusion reaction and promote the reaction. 2. Through fusion, 3 helium alpha rays with a charge of +3 and energy are generated from 1 proton and 1 boron. 3. It is considered that the muon is more likely to be trapped by boron with a charge of +5 that exists in a large amount in bulk around the muon rather than being trapped by the generated +3 helium. (Electrically attracted) 4. The muon tends to stay near boron rather than helium, traps the muon, and boron (muon molecularizes and the proton can easily approach electrically and is prone to fusion) fuses with the incident proton repeatedly, and the muon catalyzes the fusion reaction between the proton and boron. <0013> In the present invention or invention, in a proton-boron fusion reaction system (P-11B system), since the boron serving as the fusion fuel has a charge of 5 (+5) and the charge of the helium generated after fusion is 3 (+3), a system (Figure 1) is proposed in which muons and protons are irradiated onto a boron target to cause muon-catalyzed fusion. *This application is at the idea stage and has not been proven, but in the P-11B system, it is assumed that the fuel has a charge of +5 of boron and is a system that can strongly capture and trap negatively charged muons more easily than the +2 charge of the generated helium, and the application is filed. *In the reverse system, the known hydrogen-D-T system muon-catalyzed fusion system, negatively charged muons are easily captured by helium.<0014>*Although the present invention has been shown by taking the proton-boron fusion system as an example, in order not to limit the scope of the invention, more generally, when disclosing the conditions of the present invention, it may be sufficient that the system is such that the charge of the substance generated when the atomic nuclei fuse is smaller than the charge of the atom that becomes the fusion fuel. *For example, a reaction formula system as described in FIG. 2 may be considered. A system using boron B or lithium Li as in the example of FIG. 2 may also be used. <0015>● The boron and lithium of the present application may be heated above room temperature and used as a liquid. For example, liquid lithium may be used. In existing muon-catalyzed fusion systems, cooled liquid hydrogen (melting point: minus 250 degrees Celsius) is used. On the other hand, since the melting point of liquid lithium is about 180 degrees Celsius, liquid lithium may have the advantage of being easier to liquefy than liquid hydrogen when it is desired to liquefy and use it in the target part of muons. ● Regarding boron, the melting point is 2070 degrees Celsius and the boiling point is 4000 degrees Celsius. Although the temperature is higher than that of lithium, it can be used in the target part where muons and protons are irradiated as liquid boron. In the target part, it is expected that muon-catalyzed fusion will occur using boron with a nuclear charge of +5 or lithium with a nuclear charge of +3 as the fusion fuel. After the muon-catalyzed fusion, helium alpha rays with a nuclear charge of +2 are generated and released from the system. (The system using boron and protons is disclosed in FIG. 1, and the system using protons, neutrons, and lithium is disclosed in FIG. 3.) <0016> The most important feature of the present invention is to use, in a muon-catalyzed fusion system, a system in which the charge of the substance (He, alpha rays in FIG. 1) generated when the atomic nuclei fuse is smaller than the charge of the atom (B in FIG. 1) that becomes the fusion fuel. <Effects of the Invention> <0017> The present invention is a fusion system that does not emit neutrons possessed by the P-11B system, and has the advantage that there is a possibility that the substance activated during fusion is less likely to occur. <Brief Explanation of the Drawings> <0018><FIG. 1>FIG. 1 is an explanatory diagram of a muon-catalyzed fusion system 1F-SYS using boron and protons. <FIG. 2>FIG. 2 is an example of a fusion reaction system having the feature that when the atomic nuclei fuse, the nuclear charge of the substance generated by the fusion is smaller than the nuclear charge of the atom that becomes the fusion fuel.(Figure 2 is an explanatory document. Although not all examples described in Figure 2 are used in the invention of this application, examples of reaction systems with such characteristics are described. For example, in Group A of Figure 2, reaction equations of systems using protons and lithium, protons and boron-11, protons and nitrogen-15, protons and nitrogen-15, protons and oxygen-17 / oxygen-18, etc. are described. In Group B, reaction equations of lithium-6 / lithium-7 with protons, D, neutrons, and helium-3 are described. In Group C, reaction equations related to carbon are described. Regarding carbon, examples of nuclear fusion reactions between carbons are also described.) <Figure 3> Figure 3 is an explanatory diagram of a muon-catalyzed nuclear fusion system 1F-SYS using lithium and protons. Examples of irradiating and injecting protons, neutrons, and deuterium into lithium are described in (A), and an example using lithium-6 deuteride in which lithium-6 and deuterium are chemically bonded (ionically bonded) is described in (B). <Figure 4> Figure 4 is a comparative explanatory diagram of an existing muon-catalyzed nuclear fusion method using D or T and the muon-catalyzed nuclear fusion method of this application using protons and B or Li. (The upper part of Figure 4 is the method using D and T, and the lower part of Figure 4 is the method of this application using protons and B and Li) <Figure 5> Figure 5 shows a fusion reactor 1R and a fusion application thruster 1TH including the 1F-SYS of this application and its application examples. *For example, the 1F-SYS may be installed on a spacecraft 3 or a exploration robot 3 that propels and moves in the air, outer space, between planets, or between stars. There may be a spacecraft 3 that generates muons, protons, and neutrons by an accelerator, collects and stores nuclear fuels B and Li, and causes the above nuclear fusion reaction to emit He alpha rays, etc. backward of 3 to propel itself by the reaction force. *3 is not limited to spacecrafts, but may also be various transportation devices, airplanes, spacecrafts, ships, submarines, vehicles, automobiles, robots, various industrial machines, and space exploration robots. <Figure 6> Figure 6 is an explanatory diagram / conceptual diagram of a muon-catalyzed nuclear fusion system 1F-SYS / 1EXP-SYS using diborane, boron hydride, alkane, and azane. (It is an explanatory diagram of a system in which the target T1 is diborane, alkane, or azane, excluding the part that irradiates protons in Figure 1) <Figure 7> Figure 7 is an explanatory diagram of a muon-catalyzed nuclear fusion system 1F-SYS using a diborane and boron hydride part pressurized by a ramjet method. <Figure 8> Figure 8 is an explanatory diagram of a system 1F-SYS-MP1 that mixes and compresses diborane and other boron hydrides with muonic hydrogen atoms in a compression part.)<Figure 9>Figure 9 is an example of the 1F-SYS having a compression unit and a heating unit. (A laser irradiation system may be provided.) <Figure 10>Explanation diagram of a case where a movable muon target for muon generation and a rotating muon target are inserted into a MERIT type accelerator and a MERIT ring, the target is rotated and made movable, and a particle beam is applied to the target to generate pion muons. (The cross-section of the rotating disk may be thin and the outer peripheral part may be thin like a wedge.) <Figure 11>Explanation diagram when mechanically replacing a disk-shaped movable muon target. <Figure 12>Explanation diagram of a case where one extraction port is put on hold, the movable muon target part is removed and moved from the accelerator, and the muon target part is replaced with another muon target. <Figure 13>Explanation diagram of an apparatus that uses a movable muon target and performs muon target replacement and particle collision with the muon target and pion muon generation in parallel, and a muon fusion and muon nuclear conversion system. (Including a muon deceleration part.) <Figure 14>Explanation diagram of a system for generating mesons and muons in which a movable muon target contains hydrogen atoms, protons, or helium atoms. <Figure 15>Explanation diagram of a system for generating mesons and muons that uses helium atoms (or hydrogen atoms, positively charged particles) moving in a circular accelerator as a muon target. <Figure 16>Explanation diagram of a fusion system, a nuclear conversion system, and an atomic manufacturing system using a meson generation system. <Figure 17>As one of the embodiments of the present application, an explanatory diagram of attempting nuclear conversion and nuclear fusion by decelerating cosmic muons and high-speed muons and irradiating, injecting, and bonding them to the target part T1 atoms. (A) Regarding the target T1 on the ground side, the celestial sphere side and the cosmic side. ·An example of decelerating high-speed cosmic muons with a dome-shaped decelerator array covering the upper space side and irradiating T1 to attempt nuclear conversion. (B) An example of irradiating a target T1 of direct raw material atoms / molecules with a laser to form an electric field capable of decelerating muons, decelerating the muons, and attempting muon nuclear fusion / nuclear conversion of T1. <Figure 18> An explanatory diagram of an example of irradiating a target T1 of direct raw material atoms / molecules with a pulsed laser to form an electric field capable of decelerating muons, decelerating the muons, binding the muons to the atoms of T1, and attempting muon nuclear fusion / nuclear conversion. <Figure 19> An explanatory diagram of a configuration using an element with an electric field formed as a muon decelerator. (A) An explanatory diagram when using an element with an electric field formed to decelerate muons. (A) is a configuration where muons incident on the target part T1 can rotate due to the magnetic field B and move inside the atoms of the target part. (B) An explanatory diagram when using a pyroelectric body or an array of pyroelectric bodies to form a decelerating electric field and decelerating muons with the electric field. (B) is a configuration where the temperature of the end of the pyroelectric body is changed to generate an electric field in the pyroelectric body and use the electric field as a means for muon deceleration. <Figure 20> An explanatory diagram of an element for forming an electric field. (A) When using a capacitor element using an electrode and an insulator / dielectric. (B1) When using an electric double layer capacitor type element. (B2) An explanatory diagram of an element including an electric double layer part. <Figure 21> An explanatory diagram of a transport device / structure 3 having a part for generating neutrons / muons from cosmic rays. <Figure 22> An explanatory diagram regarding the assumption of a nuclear conversion / nuclear fusion system using muons considering the muon nuclear capture reaction. (A) An explanatory diagram of the assumption that muons bind to carbon-12 in a carbon material, undergo a muon nuclear capture reaction, change to a boron-12 nucleus (12B*) having an excitation energy of about 10 - 20 MeV, then excitation energy transfer occurs from 12B* to the adjacent carbon-12 nucleus, an excited carbon-12 (12C*) is generated, and then it is converted to helium, and the excitation energy moves to the adjacent carbon-12 and repeats, and the carbon-12 nuclei in the carbon material of carbon-12 are converted to helium using muons. (B1) An explanatory diagram of the case where muons are bound to azane containing nitrogen-15, a muon nuclear capture reaction is caused to change to carbon-15, and then nitrogen-15 is generated after the half-life of carbon-15 has passed. (B2) An explanatory diagram of the muon nuclear fusion of nitrogen-15.(In B1, nitrogen-15 can be converted to carbon-15, but the effective nuclear charge Z of carbon-15 is lower than that of nitrogen-15, and it is described in combination with the assumption that the fusion reaction continues)<FIG. 23>Explanatory diagram regarding the assumption of a muon-induced nuclear conversion / fusion system considering the muon-nucleus capture reaction when muons are irradiated and introduced into ammonia containing nitrogen-15. <FIG. 24>Explanatory diagram regarding the assumption of a muon-induced nuclear conversion / fusion system considering the muon-nucleus capture reaction when muons are irradiated and introduced into boron hydride containing boron-11 (system of boron hydride anion and lithium cation). <FIG. 25>Explanatory diagram of the neutrino communication system 1NUT-COM and the muon communication system 1MU-COM. <FIG. 26>Explanatory diagram of the neutrino communication system 1NUT-COM having a part 2MS-NUT-GRAV for separating neutrinos with different masses. <FIG. 27>Explanatory diagram of a configuration in which muons M1 are irradiated onto a target T1 in a container 4D-MUCF·4T-MUCF equipped with a coil 2COIL and confined and moved by a magnetic field. <FIG. 28>The upper left figure 1 of FIG. 28 is an explanatory diagram of system 1 using a vacuum pump 4RFP using a deep eutectic solvent or the like as a working liquid. (Example of using a Sprengel pump type as pump 1) The upper right figure 2 of FIG. 28 is an explanatory diagram of system 1. (Explanatory diagram of system 1 used as a food pump as pump 2. Here, the pump type may be a pump using a working liquid such as a liquid-sealed pump or a rotary pump.) The lower left figure 3 of FIG. 28 is a comparison diagram between a vacuum exhaust system including a low-vacuum pump RP and a high-vacuum pump FP and the present vacuum pump 4RFP·system 1, and is an explanatory diagram of the combination. The lower right figure 4 of FIG. 28 is an explanatory diagram of a general liquid-sealed pump and a rotary pump. (For example, using NADES and ionic liquid IL for the working liquid, liquid seal, liquid seal ring, and seal part) <FIG. 29>FIG. 29 is an explanatory diagram of one of the coils of the annular vacuum container 4D. (Annular vacuum container: including donut-shaped, annular vacuum tank, plasma containers 4D, 4D-T, 4D-ST, 4D-H. Coil 4C-EDL) <FIG. 30>FIG. 30 is an explanatory diagram of the annular vacuum container. (The annular vacuum container may be provided with a rotating means 4ROT.)<Fig. 31>Fig. 31 is an explanatory diagram of a vacuum vessel using a motor and a bearing for the rotating means 4ROT (4ROT is a motor - rocket motor). <Fig. 32>Fig. 32 is an explanatory diagram of a vacuum vessel equipped with a propulsion device (propulsion device 4ROT - TH). <Fig. 33>(A) Fig. 33(A) is an explanatory diagram when rotating a cylindrical tube - shaped vacuum vessel (4T, 4T - IN) in the circumferential direction (theta direction) of the cylinder (an example when rotating a cylindrical tube - shaped vacuum vessel used in a magnetic mirror type, magnetic field inversion configuration type, etc.). (B) Fig. 33(B) is an explanatory diagram of a cylindrical container 4T·4T - MUCF. <Fig. 34>Examples of assumed muon nuclear fusion and nuclear conversion of deuterated carbon 12 formed by combining deuterium and carbon 12. (A) An example of assumed muon nuclear fusion and nuclear conversion of methane CD4 composed of carbon 12 and deuterium D. (B) An example of assumed muon nuclear fusion and nuclear conversion of a polymer - resin deuterated carbon formed by combining deuterium and carbon 12. Specific example: An example of assumed muon nuclear fusion in a hydrocarbon deuteride molecule (C2D4)n. <Fig. 35>An explanatory diagram of an example of assumed muon nuclear fusion of H and F atoms in a polyvinylidene fluoride PVDF resin. (In one form, the PVDF part may serve as both the target part T1 and the muon decelerator 2MUDECE.) <Fig. 36>An explanatory diagram of an assumed example of a muon nuclear fusion system where the target part T1 and the decelerator 2MUDECE are arranged in the coil 2COIL, and muons may be confined in T1 in the magnetic container - magnetic field cage 2MAGC inside the coil. (Here, T1 and the decelerator 2MUDECE are capacitor elements 2FDELE - PVDF using PVDF, a decelerator - element 2FDELE - PVDF using two electrodes, and may contain atoms (hydrogen and fluorine 19) for the T1 part for muon nuclear fusion. Also, the coil 2COIL and the magnetic field cage 2MAGC may be a helical coil 2COIL - Helical and a helical magnetic field cage 2MAGC - Helical.) <Fig. 37>An explanatory diagram of a system including a control unit, a power supply, auxiliary equipment, etc. when driving the device in Fig. 36. (It may be possible to apply a voltage from the power supply 2PWSP to the capacitor elements 2FDELE - PVDF, 2FDELE - LAM - PVDF.) <Fig. 38>A negative muon decelerator / positive muon accelerator using a capacitor element. [It may be possible to apply a voltage from the power supply 2PWSP to the capacitor elements 2FDELE - PVDF, 2FDELE - LAM - PVDF. An explanatory diagram of a configuration capable of decelerating negative muons and accelerating positive muons (capable of separating positive and negative muons).In the figure, the insulator / dielectric part describes an example of PVDF, but it may also be another insulator such as diamond. <Figure 39> Example of the arrangement of the deceleration element, capacitor element, and T1. <Figure 40> Explanatory diagram of a device that uses a cube of insulator / dielectric with electrodes attached to six faces for decelerating the velocity components in the three-dimensional XYZ directions as a capacitor element, muon decelerator, and muon accelerator. <Figure 41> Explanatory diagram of an attempt to change the orbit, attitude, and motion of a threatening meteorite MTO by detonating it and injecting a propellant using a muon fusion system. A container 4T-MUCF loaded with muon fusion fuel T1 is installed in a threatening meteorite MTO (using meteorite exploration robots 5, 5WKR), and muons or neutrinos / particles are irradiated (from the 1NUT-TX installation location) onto the muon generation part and muon deceleration part installed inside the container, so as to initiate muon fusion ignition of T1 in the container 4T-MUCF from a remote location (the installation location), detonate / explode it, and use the explosive force to detonate / engage the MTO or change the orbit, direction, and attitude of the meteorite. <Figure 42> Explanatory diagram of an attempt to detonate from inside the meteorite and divide / crush the meteorite MTO using a muon fusion system with T1 loaded in a hole drilled inside the meteorite MTO. A borehole / hole 5T-HOLE is drilled in a threatening meteorite MTO, T1 is loaded into the hole and sealed, a container 4T-MUCF loaded with muon fusion fuel T1 is installed (using meteorite exploration robots 5, 5WKR), T1 is initiated for muon fusion ignition and detonated / exploded, and a muon fusion explosion is caused from inside the MTO to detonate / explode the MTO and use the explosive force to divide / decompose the MTO. <Figure 43> Explanatory diagram of an attempt to remotely detonate by generating muons through a charged current reaction or the like by irradiating neutrinos that can penetrate the iron wall of a hole inside an iron meteorite with T1 inside the hole from multiple irradiation parts towards a single T1 part. <Figure 44> Explanatory diagram of a metal / material heating / evaporation / removal / ablation device 5REMV-HEAD or the like having a fusion part and an alpha-ray irradiation part. <Figure 45> Explanatory diagram of driving fuel T1 into an iron meteorite using a centrifugal gun, driving in and excavating a blast ball 3LOAD, and igniting T1. <Figure 46> Explanatory diagram of the structure 2LPST of a centrifugal gun. <Figure 47> Explanatory diagram of the initiation of detonation and destruction of a muon fusion system with a neutrino-muon conversion part (conversion atoms / neutrons / particles).<Fig. 48>Explanatory drawing of the submarine 3SUBM including a muon nuclear fusion reactor and a transmitter / receiver for muon neutrinos. <Fig. 49>Explanatory drawing of a muography system for obtaining muography / CT of celestial bodies, satellites, and meteorites MTO. (Explanatory drawing of a CT system using muons and neutrinos. Explanatory drawing showing that the transmitter and receiver for muons, etc. for obtaining a transmission image of a large meteorite or celestial body may be mounted on a spacecraft or space vehicle 3. The three may be able to communicate via a wireless communication network 1NETWORK.) <Fig. 50>Explanatory drawing of a muography system for obtaining muography / CT of the human body and objects. <Fig. 51>Explanatory drawing of an aircraft / spacecraft 3 including a muon nuclear fusion reactor and a transmitter / receiver for muon neutrinos. <Fig. 52>Explanatory drawing / conceptual drawing when the energy of charged alpha rays, particles, and photons having kinetic energy generated in a muon nuclear fusion reactor is taken out as electric power or motive power and used in the propulsion device of a transportation device 3. <Fig. 53>Explanatory drawing of an example when the energy of charged alpha rays, particles, and photons having kinetic energy generated in a muon nuclear fusion reactor is used in a rocket propulsion device. The upper part of the figure is an example of a solid rocket. The lower part of the figure is an example of a solid self-consuming rocket. <Fig. 54>Explanatory drawing of a device including a pressurizing part of a reciprocating engine type fuel T1 part. <Fig. 55>Explanatory drawing of a muon generation device of a lepton collider type. (Or explanatory drawing of a particle collision type muon generation device. A particle accelerator using a laser / LWF for lepton acceleration may be used.) <Mode for Carrying Out the Invention> <0019> Fig. 1 is 1. Focusing on the trap problem of muon-catalyzed nuclear fusion, as described in M1, T1, and B1 of Fig. 1, a muon-catalyzed nuclear fusion system using boron was devised. As an actually used form in Fig. 1, the form of a spacecraft or exploration robot 3 moving between planets and between stars where sunlight does not reach is shown in Fig. 5. <1> <0020> Fig. 1 is an explanatory drawing of the device / system of the present invention using boron for the fuel F1 and the target part T1. *Since this system uses muons and protons, there is also a point that equipment such as an accelerator is required. A vacuum is required for driving the accelerator. When arranging the accelerator in space, the vacuum in space may be used. <2> <0021>Fig. 2 is an explanatory drawing of the device / system of the present invention using lithium for the fuel F1 and the target part T1. Lithium has a lower melting point than boron.<Industrial Applicability> <0022>Although it is necessary to secure resources such as boron and lithium, it may be possible to generate electric power by nuclear fusion. The invention of the present application uses an accelerator that requires a vacuum, etc., and generates alpha rays that are assumed to have a high injection speed. It may also be used for the propulsion device of a spacecraft traveling in the vacuum of outer space as shown in Fig. 5. <Description of Signs> <0023><Figs. 1 and 3>1F-SYS: Schematic diagram of a muon-catalyzed fusion system using a fusion reaction with boron and protons. M1: Muon generation means, means for injecting and irradiating muons into the fusion fuel target T1. Example: A system using a particle accelerator capable of generating muons P1: Proton generation means, means for injecting and irradiating protons into the fusion fuel target T1. Example: A particle accelerator capable of accelerating protons and hitting and irradiating a target. An element of the fusion fuel in the boron-proton fusion reaction system. N1: Neutron generation means, means for injecting and irradiating neutrons into the fusion fuel target T1. Example: A particle accelerator capable of accelerating neutrons and hitting and irradiating a target. A1: Particle accelerator A1. T1: Target part containing fusion fuel. Fusion fuel T1, F1. B1: The part of T1 using boron. Boron target. Boron may be molten. L1: The part of T1 using lithium. Lithium target. Lithium may be molten liquid lithium. EX1: Product EX1 after fusion. In Figs. 1, 3, etc., helium He and alpha rays generated after fusion. <Fig. 5>3: Transportation equipment 1R: 1F-SYS which is a fusion reactor. A fusion reactor including 1F-SYS. A power generation unit for converting the energy of alpha rays into electric energy may be provided. 1GENR: Power generation unit (the part for converting the energy obtained by the fusion system 1F-SYS or the nuclear conversion system 1EXP-SYS into electric power) *Although not specified in Fig. 5, the fusion-derived electric power generated by 1EXP-SYS, 1F-SYS, and 1R may be supplied to the muon generation part M1 and the proton generation part P1 to generate muons and protons. This electric power may be used to drive the system of the present invention and each part of the system. 1TH: A fusion application propulsion device including 1F-SYS, a thrust generation device. Propulsion means. Moving means. (When 3 is a spacecraft, 1TH may be a particle beam emission part such as alpha rays, gamma rays, photons, particles, etc. When 3 is an aircraft, it may be a propulsion agent ejection part that uses the electric power obtained by 1GENR to take in a propulsion agent and air, heat, compress, and eject it backward from 3, or a propeller part driven by electric power. When 3 is a ship, it is a part capable of rotating a propeller and generating a water flow using the electric power obtained by 1GENR.In the case of a robot having 3 arms or a vehicle moving on land, it may be driven by the power obtained by 1GENR, which may be a wheel, tire, motor, or the motor and arm part of the robot. ) 1TH-NZ: The nozzle part of 1TH. When the product EX1 after nuclear fusion is helium or alpha rays with energy, it is the nozzle part that emits the alpha rays. It may also be a thrust deflection device or nozzle. The alpha rays may be irradiated onto a propellant to heat and eject the propellant. Separately from *1TH-NZ, a propulsion device that operates by using the power generated by 1R to release an ion thruster or a photon laser and propels by reaction may be operated. <Figure 6> System using diborane B2H6 BH1: A substance containing boron, which is boron hydride, diborane, or borane B1. T1 and F1 are diborane. The target of diborane. Diborane and BH1 may be gas, liquid, fluid, or (solid). (The configuration of Figure 7 using fluid is also possible) In the system of Figure 6, since diborane containing hydrogen and protons is used, the proton introduction part P1 described in Figure 1 etc. becomes unnecessary. <Figure 7> 1F-SYS-RAM: Nuclear fusion system. (An assumed diagram when the system of the present application using diborane is applied to a system in which a nuclear fusion fuel fluid having a known ramjet part circulates in a closed loop system) RAM: Ram pressure generation device part when compressing in a ramjet type. PBH1: Compressed BH1 part. The target part of muons having a compressed diborane fluid part. FP: Nuclear fusion reaction part, muon irradiation part. FEEDC: The part that removes helium in the diborane fluid circulating in the system, removes surplus substances, and adds necessary substances and diborane as fuel. The control part of the feed. Fuel supply system, fuel control system. Helium He removal part, diborane fuel supply part, etc. HX: Heat exchanger ENEX: Although not shown in the figure, it is a device part that generates electricity based on alpha rays and nuclear fusion energy, the power generation part. It may be included in the system. PUMP: Compressor, pump. Pressurizes, compresses, and circulates the fluid in the system. Driven by a motor or the like. (Driven by obtaining power from the power generation part) M1: Muon generation part, muon irradiation part. (Driven by obtaining power from the power generation part) EX1: Helium generated after nuclear fusion (which needs to be removed).<0024><Other> In this application, by using a system in which the positive charge of the atomic nucleus of nuclear fuel substances (e.g., B, Li) is greater than that of the post-fusion product (e.g., He), it is intended to hold muons with negative charges in the atomic nuclei of the nuclear fuel substances. It is intended that having muons located in the nuclear fusion fuel rather than in the nuclear fusion product results in greater Coulomb force, charge, electric field, and electrical stability. *For example, in the case of a boron system where there are impurities with an atomic number Z greater than that of boron, if following the idea of this application, impurities with a Z greater than that of boron may trap muons and stop the reaction. (For example, considering sodium borohydride NaBH4, which is a raw material for diborane, sodium has a Z greater than that of boron, and according to the idea of this application, muons should be trapped by Na in NaBH4.) <0025> The concepts and embodiments of this application have been described, but these embodiments are presented as examples and are not intended to limit the scope of the invention. These novel embodiments can be implemented in various other forms, and various omissions, replacements, and changes can be made without departing from the gist of the invention. <0026><<Supplementary part based on the application claiming priority>> The following items are added to the previous application, Japanese Patent Application No. 2023-150635. <0027> In FIG. 1, protons are being irradiated onto boron, but as shown in FIG. 6, borane, diborane B2H6, and boron hydride in which boron is pre-bonded to protons and hydrogen atoms can be used in the target part T1. For example, liquefied, liquid diborane can be used as the nuclear fusion fuel F1 or in the target T1 part. In the system of FIG. 6, since diborane containing hydrogen and protons is used, there may be an advantage that the proton introduction part P1 described in FIG. 1 and the like becomes unnecessary. <0028> FIG. 7 depicts a system 1F-SYS-RAM in which diborane is pressurized, compressed, circulated, irradiated with muons, and caused to undergo nuclear fusion. (FIG. 7 is one of the embodiments of FIG. 6.) FIG. 7 is an assumed diagram when the system using diborane of this application is applied to a system in which a nuclear fusion fuel fluid having a known ramjet part circulates in a closed loop system. <0029> The diborane within the 1F-SYS-RAM system of FIG. 7 is pressurized and compressed by a compressor PUMP and circulated. The pressurized fluid diborane is further compressed by a compression device part RAM to form a compressed BH1 part (PBH1 part).Muons are irradiated from the muon irradiation unit M1 to PBH1 to promote nuclear fusion. (Since diborane is compressed, its density is high, making it easier for muons to come into contact, proximity, and interaction, and it is expected that the catalytic nuclear fusion reaction will occur more easily.) <0030>In the system 1F-SYS-RAM of FIG. 7, there is an advantage that protons and boron can be supplied to the system together as diborane in which hydrogen and boron are bonded. The proton introduction unit P1 is unnecessary, and it is also possible to add fuel to the system and remove He from the system (degassing). (Using the feed control unit FEEDC such as a helium He removal unit and a diborane fuel supply unit, etc.) <0031>Also, considering the ease of contamination by impurities with an atomic number larger than that of boron, gaseous diborane that can be purified may be better than solid boron. (Solid boron requires production, purification, and refining as a solid crystal.) As described by taking sodium borohydride NaBH4 as an example in paragraph 0024 of the present application, the present application considers the presence of atoms with an atomic number larger than that of the nuclear fusion fuel, the post-fusion product EX1, or impurities in the fuel to be unfavorable. <0032>Also, in the systems such as FIGS. 1, 3, 6, and 7 of the present application, it is assumed that there are no atoms with an atomic number larger than that of the nuclear fusion fuel, the post-fusion product EX1, or impurities in the direction where the muons travel. For example, it is premised that there are no atmospheric molecular atoms with an atomic number larger than that of boron B (for example, nitrogen N or oxygen O). If nitrogen N is present, it may be trapped. The configuration of the present application may need to be considered so as to avoid atoms with an atomic number larger than that of boron (or other candidate elements / atoms such as lithium) used as fuel. <0033><Document Name><1>A muon-catalyzed nuclear fusion system using a nuclear fusion reaction system, which has the characteristic that the electric charge of the nucleus of the atom / particle generated by the nuclear fusion reaction is smaller than the electric charge of the nucleus of the atom of the nuclear fuel substance. <2>The muon-catalyzed nuclear fusion system according to 1, wherein the nuclear fusion fuel contains boron or lithium, and the atom / particle generated by the nuclear fusion reaction is helium / alpha rays. <3>The muon-catalyzed nuclear fusion system according to 2, wherein the fuel is in a liquid or fluid state.<4>A system having the characteristic of being less likely to generate neutrons by a nuclear fusion reaction, wherein the nuclear fusion fuel uses boron and boron hydride, and the atoms and particles generated by the nuclear fusion reaction are helium and alpha rays, the muon-catalyzed nuclear fusion system according to 1. <Document Name>Document <><Problem>In known muon-catalyzed nuclear fusion, there is a problem that muons adhere to, capture, and trap helium, which is a product substance after nuclear fusion rather than a nuclear fusion fuel substance such as hydrogen, deuterium D, and tritium T, and the catalytic nuclear fusion stops. It was considered to solve the problem that muons are captured by the product substance after nuclear fusion rather than the nuclear fusion fuel substance, making it difficult for the muon-catalyzed nuclear fusion reaction to proceed. Also, a system less likely to generate neutrons was devised. <Solution Means>In muon-catalyzed nuclear fusion, when atomic nuclei fuse, a nuclear fusion reaction system is used that has the characteristic that the electric charge of the atomic nucleus of the substance generated by the nuclear fusion is smaller than the electric charge of the atomic nucleus of the atom serving as the nuclear fusion fuel. Specifically, a muon-catalyzed nuclear fusion system is proposed that uses protons and boron as the nuclear fusion fuel, or diborane containing protons as hydrogen molecules together with boron. <0034><<Supplementary Part by Application Claiming Priority>>The following items were added to the previous applications, Japanese Patent Application No. 2023-150635 and Japanese Patent Application No. 2023-151787. <0035><Figure 8: When P1 and M1 in Figure 5 are combined and introduced into the target part on the same ray line as muonic hydrogen>In this application, as shown in Figure 5, the proton P1 and the muon M1 can be irradiated onto the target part T1 by combining and mixing them on the same ray line. As shown in Figure 5, using the particle accelerator A1, the proton P1 of the fuel and the muon M1 serving as a catalyst can be irradiated onto the target part T1 containing boron by combining and mixing them on the same ray line. <0036>Also, in this application, as shown in Figure 5, using the particle accelerator A1 or the neutral beam injector NBI, the muonic hydrogen atom MP1 (or in some cases, the electrically neutral muonic hydrogen molecule MP12 composed of two muonic hydrogen atoms) formed by the combination of the proton P1 of the fuel and the muon M1 (muon M1) serving as a catalyst can be irradiated and introduced into the boron hydride of the target part T1. (Or MP1 and MP12 can be mixed with boron hydride and blown into the target part for compression.))When irradiating and injecting muonic hydrogen atom MP1 into the pressurized boron hydride in the target part T1, in the path during the injection or near the target part T1, the muonic hydrogen atom MP1 and boron hydride are pressurized, (furthermore, inside the gas fluid, MP1 and boron hydride, MP12 and boron hydride can also be mixed by pressurization,) and a mixture MP1-XBH of muonic hydrogen atom and boron hydride is formed. The mixture MP1-XBH of muonic hydrogen atom and boron hydride is pressurized and transported to the ram part (RAM), and in the ram part, it is further pressurized and compressed into a compressed mixture PMP1-XMB. The mixture MP1-XBH (compressed mixture PMP1-XMB) of muonic hydrogen atoms MP1·MP12 and boron hydride compressed in the ram part increases the temperature during the muon-catalyzed reaction and the density per volume of muons and protons·boron, muons. This leads to promoting the catalytic nuclear fusion reaction. Also, using the ramjet method with the ram part, the mixture MP1-XMB can be pressurized, compressed, and heated to a high temperature. In addition to increasing the temperature during the muon-catalyzed reaction and the density per volume of muons and protons / boron, the mixture of muonic hydrogen atoms MP1·MP12 and boron hydride can cause the muon-catalyzed reaction under conditions of high temperature and vigorous movement of molecules and particles. In the present application, muonic hydrogen atoms are used to increase the temperature during the muon-catalyzed reaction, the density per volume of muons and protons / boron, and the thermal motion of muons and protons / boron, thereby promoting the muon-catalyzed nuclear fusion reaction. <0037>When a single muon (muon beam line) is irradiated onto the surface of boron, the surface of lithium, or the surface of boron hydride gas / fluid, it becomes negatively charged and repels other muons, which may prevent the muons from being concentrated or compressed at one point. Therefore, as shown in FIG. 8 of the present application, the muons are combined with the protons of the proton-boron fuel to neutralize the charge into neutrons, and then the compressed muons and proton-boron fuel are densely gathered in one place, bringing more muons and fuel closer to each other to promote muon-catalyzed nuclear fusion. *Due to the problem of the negative charge of muons, there is a risk that muons will electrically repel each other and be difficult to compress at one point. However, by combining muons with protons / hydrogen nuclei (which are also fuels in proton-boron fusion) to form muonic hydrogen atoms MP1 (or MP12) and electrically neutralize them, they can be compressed without electrical repulsion. <0038>Lithium hydride has a high melting point and usually exists as a solid or liquid. Compared with boron hydride, it is more difficult to turn lithium hydride into a gas. Since lithium hydride and solid boron are solids at normal temperature and pressure as described above, they are more difficult to mix with boron hydride, which is a gas at normal temperature and pressure, and it may also be difficult to pump and compress them into the ram part. On the other hand, MP1, which is considered to be a gas, MP12, which is also considered to be a gas, and boron hydride gas can be mixed using means such as pressurization and mixing means, and then pressurized, pumped, further compressed, and adiabatically heated towards the ram part. <0039>In the known D-T reaction, a maximum of 2 muons are required, while 4 muons are required for lithium and protons, and 6 muons are required for boron. It may be necessary to compress and confine muons, protons, and boron in a limited space.From the well-known D-T reaction system, it may be necessary to mix muons and nuclear fusion fuel and confine them in one place to a high density and react them with the nuclear fusion fuel in the p-11B reaction system studied in the present application. Therefore, in the present application, the electrically neutral muonic hydrogen atom MP1 and boron hydride are used, mixed, compressed, confined in one place to a high density, and an attempt is made to cause muon-catalyzed fusion (or fusion assisted by muons). <0040><Muon-catalyzed fusion during flight>The muonic hydrogen atom MP1 has a smaller Bohr radius and a lower Coulomb barrier (or is more likely to tunnel quantum mechanically) than a hydrogen atom composed of ordinary protons and electrons, and is expected to fly toward other atoms and be more likely to undergo a fusion (muon-catalyzed fusion during flight) reaction when colliding with and approaching other atoms. The muonic hydrogen atom having a velocity and colliding with boron then generates alpha rays having energy, and the boron hydride is heated using the energy of the alpha rays. When the boron hydride passes through the heat exchanger HX, thermal energy is transmitted to an external steam generator or the like, and the thermal energy and kinetic energy are transmitted from the steam generator supplied with water to the turbine generator 1PP to rotate and operate the steam turbine generator 1PP to generate electric power. <0041>In FIG. 8, the muonic hydrogen atom MP1 or the neutral particle beam incident device NBI · particle accelerator A1 serving as a source of the muonic hydrogen atom MP1 passes through the path or route S1 filled with boron hydride (such as B2H6) and passes through the nozzle portion NZ, and MP1 and the mixture MP1-XMB of MP1 and boron proceed toward the target portion T1 and the ram portion RAM. At this time, the muonic hydrogen atom MP1 may react with the boron hydride on the path S1. *When MP1 is incident on the surface of solid boron, molten boron, or solid-liquid lithium hydride, it can be expected that a fusion reaction will occur on the surface and energy will be generated. As an example of the present application, muon-catalyzed fusion can be promoted when solid or liquid boron, lithium hydride, or lithium is used as the target T1. (However, it may not be possible to compress the mixture or mixed fluid or mixed gas MP1-XMB of MP1, MP12 and boron hydride to a high density and high temperature to promote fusion as shown in FIG. 8 and the above.))<0042>Symbols, etc. <Figure 8> 1F-SYS-MP1, 1F-SYS-MP1-RAM: A fusion system using a mixture of muonic hydrogen atoms and fuel. Muonic hydrogen atom MP1: AMP1: A muonic hydrogen atom generation irradiation unit (such as particle accelerator A1, neutral particle beam irradiation device NBI, etc., which can generate MP1 and MP12 and can be incident / input). S1: Path S1 (with a mixture of MP1 and boron hydride). MP1-XMB: A mixture of MP1 and boron hydride / diborane. Or a mixture of hydrogen and boron / (carbon·)nitrogen·oxygen·fluorine, etc. Or a part / mixture part containing a compound in which a raw material atomic nucleus with the first atomic number ZA and a raw material atomic nucleus with the second atomic number ZAA required for nuclear fusion are chemically bonded. PMP1-XMB: The mixture MP1-XMB compressed (and / or heated) by compression means such as RAM, or the mixture MP1-XMB compressed (and / or heated) by compression means such as RAM. RAM: Compression means such as a ram part. Inertial confinement type nuclear fusion that irradiates and confines a nuclear fusion target fuel pellet by laser irradiation (when the RAM part is of the laser confinement / inertial confinement type, the wavelength of the light of the laser may preferably use a short wavelength on the blue, ultraviolet, X-ray, gamma-ray side so that the momentum of the photon can be taken larger) is known. In this application, the target part / mixture may also be compressed by laser in the compression part RAM part. (A muon injection process may be added to the laser confinement type inertial confinement nuclear fusion.) The ram part may be irradiated with a laser, an ion beam, or an ion beam containing raw material atoms so as to converge from a plurality of emission parts to the part containing raw material atoms (Figure 9). (It may also be an inertial type such as Z-pinch or magnetized target type that can compress raw material atoms and can be confined by inertia.))In the RAM section, while compressing and heating the raw material atoms that serve as fuel necessary for nuclear fusion, and the compounds or mixtures formed by chemically bonding the raw material atoms together, using mechanisms such as lasers or ramjets, muons are irradiated. As a result, the molecular motion or atomic motion within the compound molecules or in the compound / mixture can be significantly increased by compression and heating. Consequently, the particles bonded to muons are more likely to approach each other due to thermal motion, with the intention of facilitating nuclear fusion, muon-catalyzed nuclear fusion, and muon-induced nuclear fusion. Additionally, there is also the aim of making it easier for the muons, which act as catalysts after nuclear fusion, to (be released and approach / capture the next raw material atoms, repeating this process) initiate the next catalytic reaction. (Although irradiating muons onto extremely low-temperature liquid hydrogen, DT, DD, or TT may have a low proximity effect of raw material atoms due to thermal motion because of the low temperature, when introducing muons, muonic atoms, or muonic hydrogen into the compressed and heated parts such as by lasers or ramjets, a proximity effect due to compression and thermal motion can be expected.) NZ: Nozzle section 1PP: Steam turbine generator HX: Heat exchanger, steam generation section, steam pipe / cooling pipe 1BKT: There may be a part / blanket that receives particles flying with energy due to nuclear fusion reactions such as neutrons and gamma rays, and converts them into thermal energy, etc., enabling energy utilization. There may be a RAM or reaction vessel section, and a container part for packing / ramming FEED near the part where the nuclear reaction occurs. When there are walls for the reaction vessel, a blanket 1BKT may be arranged inside the RAM section or the container wall. AEC: Alpha-ray energy conversion device (a device that receives alpha rays and converts them into electricity. The AEC may generate radicals using alpha rays such as titanium oxide, and decompose water (similar to a photocatalytic reaction) to obtain hydrogen and oxygen, and provide / output energy outside the system in the form of hydrogen / chemical energy. *The AEC may be an alpha-voltaic-cell.* The AEC part may receive the energy of alpha rays and generate photons of synchrotron radiation (of bremsstrahlung). The photons of the synchrotron radiation may be used to cause chemical reactions or photochemical reactions of chemical substances. The photons may be irradiated onto the part to be heated to manufacture substances, heat / propel propellants, steam, etc.Means for wavelength-converting the photons of the synchrotron radiation to longer-wavelength photons may be used to convert them to longer-wavelength photons, and the longer-wavelength photons may be received by a photoelectric conversion element for photoelectric conversion to obtain electric power and output it outside the system. Alternatively, if the longer-wavelength photons have energy capable of causing a photocatalytic reaction by a photocatalyst, a photocatalytic reaction may be caused to generate hydrogen and oxygen from water and convert it to hydrogen energy. If the longer-wavelength photons have a wavelength capable of dissociating the bonds within carbon dioxide and nitrogen molecules and causing a photochemical reaction, carbon dioxide may be dissociated and converted as the energy of chemical substances such as carbon-carbon compounds and nitrogen compounds and output outside the system. <0043><1>The fusion fuel contains protons (P1) and boron (B1), and an atom or particle generated after the fusion fuel is fused by a muon-catalyzed fusion reaction or a fusion reaction using muons is helium or an alpha ray. A muon-catalyzed fusion system, wherein the fusion fuel uses boron hydride. A muon-catalyzed fusion system, characterized in that a muonic hydrogen atom in which a muon (M1) and a proton (P1) are combined and electrically neutralized is introduced and incident on the boron hydride to form a mixture (MP1-XMB) of the muonic hydrogen atom and the boron hydride. A muon-catalyzed fusion system, characterized in that a muonic hydrogen atom is introduced and incident on the boron hydride using an irradiation means (NBI) for muonic hydrogen atoms. A muon-catalyzed fusion system, characterized in that the mixture (MP1-XMB) is pressurized by a first pressurizing means (PUMP). A muon-catalyzed fusion system, characterized in that the mixture (MP1-XMB) is mixed by a first pressurizing means (PUMP). A muon-catalyzed fusion system, characterized in that the mixture (MP1-XMB) is compressed (to become a compressed mixture PMP1-XMB) by a second pressurizing means (PUMP) to a pressure higher than the pressure by the first pressurizing means and heated (muon-catalyzed fusion system (FIG. 8, 1SYS-MP1)).<2>The second pressurizing means is performed in a compression section using a ram section (RAM) of a ramjet. The muon-catalyzed fusion system according to 1 (FIG. 8, 1SYS-MP1-RAM).<0044><<Addendum by the application claiming priority>>The following items were added to the previous applications, Japanese Patent Application No. 2023-150635, Japanese Patent Application No. 2023-151787, and Japanese Patent Application No. 2023-174791.<<<Examples of systems with decreasing atomic number Z>>>In addition to the system using boron-11 in this application, a system using nitrogen-15 is also disclosed. (At the time of filing, it is necessary to confirm whether nuclear fusion occurs using boron-11 or nitrogen-15 with muons. The said system may be a system of a nuclear fusion system or an experimental system / experimental system regarding atomic nuclei in physics.) The following examples of boron-11 and nitrogen-15 are one example of the invention to be expressed. Consider elements with atomic numbers Z from 3 (lithium) to 9 (fluorine) as in Group A of FIG. 2 of this application. <System using boron-11> A nuclear fusion reaction in which a proton and boron-11 fuse to produce three helium-4 (alpha rays) and energy is known. (p + 11B -> 3×4He + 8.7 MeV) A molecule in which a boron atom and a hydrogen atom are chemically bonded may be used as a raw material substance and nuclear fusion fuel before causing the nuclear fusion reaction. For example, borohydride, borane, or diborane may be used. When borohydride in which hydrogen and boron-11 are combined is used, since they are bonded within the molecule, the atoms can be brought close to each other in advance. When boron and a proton are brought close and irradiated with muons, boron is a solid (liquid even when heated to a high temperature) in its elemental form, and even if a hydrogen raw material is blown into boron, hydrogen will come into contact with the solid surface of boron, and muon-catalyzed nuclear fusion may occur on the surface of solid boron. Therefore, in the present application, by using a bulk fluid, gas, or liquid of borohydride in which a proton and boron-15, which are raw materials for the nuclear fusion reaction, are brought close to each other by chemical bonding and covalent bonding as a raw material substance, the first raw material atom (proton) and the second raw material molecule (boron-11, and the same applies to the case of nitrogen-15 described later) involved in the nuclear fusion reaction can be arranged in a configuration where they are easily brought close to each other, or in a state where the two raw material atoms are mixed and close to each other in advance. Therefore, preferably, borohydride such as B2H6, ammonia such as NH3, etc. are used. Muons or muonic hydrogen may be irradiated and introduced. <0045> <System using nitrogen-15> A nuclear fusion reaction in which a proton and nitrogen-15 fuse to produce carbon-12, helium-4 (alpha rays), and energy is known. (In nature, a reaction in which nitrogen-15 and a proton produce carbon-12 and helium-4 in the CNO cycle reaction in a star is known.) (p + 15N -> 12C + 4He + 5.0 MeV) In the present application, a nitrogen-15 molecule consisting only of a hydrogen molecule and nitrogen-15 may be mixed to form a liquid mixture, a gaseous mixture, or a fluid mixture, and the above-mentioned nuclear fusion using the muons may be attempted in the mixture and used in a nuclear fusion system. Also, similar to the example of the borohydride, a molecule in which a nitrogen atom and a hydrogen atom are chemically bonded, such as ammonia NH3, may be used as a raw material substance and nuclear fusion fuel before causing the nuclear fusion reaction. For example, hydrogen nitride, azane, ammonia NH3 may be used. (Azane and diazane may be used.) Muons or muonic hydrogen may be irradiated and introduced.<Use of Azane and Ammonia Molecules, Use of Ammonia in Fluids and Gases>For example, irradiate ammonia 15NH3 composed of nitrogen 15 and hydrogen with muons, so that the muons are bonded and substituted to the nitrogen 15 atom and hydrogen atom in the ammonia 15NH3 molecule (with respect to the electrons of these atoms), shorten the radius of said atoms, and promote the proximity of the nuclei of the nitrogen 15 atom and hydrogen atom to cause nuclear fusion between both nuclei, thereby attempting to initiate a nuclear fusion reaction. (In an ammonia molecule in a gas, liquid, or fluid containing 15N and P, a nuclear fusion reaction of generating 12C and 4He from p + 15N may be initiated using muons)<0046><Use of Organic Compounds and Organic Molecules Containing Nitrogen 15>For example, there is an organic compound CHN15 composed of carbon, nitrogen 15, and hydrogen, and the compound may be a compound CHN15 in which nitrogen 15 and hydrogen are bonded. Or it may be a compound CHN15 having a molecular structure with the characteristic that the nuclear fusion fuel and raw material atoms, nitrogen 15 and hydrogen, are close to each other within the compound CHN15 molecule. When the organic compound CHN15 is irradiated with muons and the muons cause the nuclear fusion of nitrogen 15 and hydrogen in CHN15 to be in the above proximity, carbon 12 is generated within the compound. However, it is intended that the catalytic reaction by muons continues when the muons bond to another nitrogen 15 present in the surroundings within the bulk of the compound rather than to carbon 12. (For example, as a simple compound example, there is methylamine CH3-15NH3 which becomes a liquid, gas, or fluid containing nitrogen 15 (15N).) Boranes and ammonia are gases but have toxicity and corrosive effects, and it is necessary to compress the gas into a tank and handle it with care. However, for an organic compound, a compound in which hydrogen can be arranged close to nitrogen 15, an organic compound, a carbon-nitrogen 15-hydrogen compound CHN15, it is less corrosive and less toxic than boranes and ammonia, and as a gaseous or liquid substance CHN15 (without being compressed and liquefied and enclosed in a cylinder), a liquid raw material substance CHN15 such as a volatile oil or hydrocarbon fuel can be stored in a tank and transported as the fuel substance CHN15 to a region with demand or a power generation system section.And then, when supplying to the subsequent nuclear fusion system, reactor, and nuclear reactor, heat the liquid compound CHN15. By heating, it becomes possible to circulate or compress the liquid with changed physical properties such as viscosity or the substance CHN15 that has become a gas or vapor by heating inside a reactor having a compression section. By using the compound CHN15, which may be a liquid for nuclear fusion fuel, it may be easier to transport to the power generation system section while suppressing toxicity and corrosiveness compared to borane-ammonia and being able to be transported in the city like volatile oil or oil. Note that the compound CHN15 may have the characteristic that for the atoms in the compound, regarding the atomic number ZA of the raw material atom with the largest atomic number that undergoes nuclear fusion reaction and the atomic number ZB of the generated atom with the largest atomic number among the atoms and particles generated by the nuclear fusion reaction, the atomic number ZB is of a magnitude less than or equal to the atomic number ZA. In the case of using nitrogen 15, the raw material atom nitrogen 15 has an atomic number of 7 (the atomic number ZA is 7), and carbon 12 generated by the reaction of nitrogen 15 and a proton has an atomic number of 6 (the atomic number ZB is 6), and it has the characteristic that the atomic number ZB is of a magnitude less than or equal to the atomic number ZA. In the case of using nitrogen 15, even if carbon 12 is generated by the nuclear fusion reaction, the positive charge of the atomic nucleus is the same as that of the carbon 12 contained in the original compound CHN15 (for example, as the carbon skeleton part of an organic compound). The muon moves around towards another nitrogen 15 with a more positive nuclear charge than the generated carbon 12 and is captured by nitrogen 15 to generate carbon 12 and helium and is recaptured by nitrogen 15 repeatedly. It is assumed that a muon-catalyzed nuclear fusion reaction continuously occurs. <0047><Cross-sectional area>From the perspective of the cross-sectional area of the nuclear reaction (*Reference B), *hydrogen 1-H-1: 33.22 barns, *1-H-2: 4.70 *lithium 6: 942.1 *lithium 7: 1.22 *beryllium 9: 7.33 *boron 11: 5.96 *nitrogen 15: 5.35 barns. Others are fluorine 9: 4.23 and carbon 12: 5.57. The cross-sectional areas of nitrogen 15 and boron 11 are between 5 and 6 barns. On the other hand, the cross-sectional area of lithium 7 is about 1, which is smaller than the case of nitrogen and boron. From the perspective of the cross-sectional area, it may be preferable to use boron 11 or nitrogen 15.[*Reference B: Japan Atomic Energy Agency website https: / / wwwndc.jaea.go.jp / jendl / j33 / J33_J.html, Internet, accessed on November 17, 2023. Neutrons in each table are cited from the Maxwellian Average of MT1. Although there may be differences in cross sections in an actual system using muons and atoms, it is described in order to consider the cross section at the time of muon fusion by comparing burn values under the same conditions between isotopes.〇Reference B: JENDL-3.3 - JAEA Nuclear Data Center K. Shibata, T. Kawano, T. Nakagawa, O. Iwamoto, J. Katakura, T. Fukahori, S. Chiba, A. Hasegawa, T. Murata, H. Matsunobu, T. Ohsawa, Y. Nakajima, T. Yoshida, A. Zukeran, M. Kawai, M. Baba, M. Ishikawa, T. Asami, T. Watanabe, Y. Watanabe, M. Igashira, N. Yamamuro, H. Kitazawa, N. Yamano and H. Takano: "Japanese Evaluated Nuclear Data Library Version 3 Revision-3: JENDL-3.3," J. Nucl. Sci. Technol. 39, 1125 (2002). (Eds.) T. Nakagawa, H. Kawasaki and K. Shibata: "Curves and Tables of Neutron Cross Sections in JENDL-3.3 (Part I and II)," JAERI-Data / Code 2002-020, Part I, Part II (2002). (Ed.) K. Shibata: "Descriptive Data of JENDL-3.3 (Part I and II)," JAERI-Data / Code 2002-026, Part I, Part II (2003).]<0048><System using lithium><Lithium-7> The system using lithium-7 and protons has the characteristics of low cross section, being difficult to be made into gas molecules, and existing in solid or liquid states. Although it is used as a material for lithium-ion batteries and other applications and its resource amount is limited, it is disclosed as one example of the present application. When using lithium, lithium hydride composed of lithium-7 and hydrogen can be utilized. Irradiate muons onto the surface of liquid lithium hydride.p + 7Li -> 2×4He + 17.2 MeV <Lithium 6> When using lithium 6 (denoted as 6Li in this application) and deuterium D (when using lithium deuteride 6, 6LiD), it is speculated that the cross-section of the nuclear fusion reaction of lithium 6 is larger than that of lithium 7 and is advantageous for the nuclear fusion reaction. In this case, the compound of lithium 6 and deuterium D, which is the raw material FEED, may be heated by the heating means RAMH, for example, by laser, radio wave, or electromagnetic wave. Or the mixture·FEED and / or its storage container (the container·part that holds the FEED within the reaction system) may be heated by heating means such as an electric resistance heater·electric heating means, and the mixture FEED may be in the state of a bulk liquid. * It may be lithium deuteride 6 (6LiD), which is a bulk liquid capable of muon irradiation. When using deuterium D and lithium 6 as described below, reactions that produce alpha rays·helium 4, protons, neutrons, etc. may occur. (The reaction formulas related to lithium are described in Group B of Figure 2.) D + 6Li -> 2×4He (alpha ray) + 22.4 MeV D + 6Li -> 7Li + p + 5.0 MeV D + 6Li -> 4He (alpha ray) + p + 2.6 MeV D + 6Li -> 3He (helium 3) + 4He + n + 1.8 MeV * It is possible to use lithium 6, which has a larger cross-section than lithium 7, and deuterium chemically bonded (ionic bond) as the raw material FEED, and the raw material FEED may be heated by the heating means RAMH, arranged in the target part T1, FP, PBH1, PMP1-XMB, and irradiating / introducing muons (·muonic atoms) into the arranged FEED may promote nuclear fusion using muons (and connect it to a nuclear fusion system·nuclear fusion reactor·nuclear fusion reactor). As described above, in the case of the invention·device that uses lithium 6, which has a large cross-section, and deuterium chemically bonded as the raw material FEED, the cross-section can be made larger than when using lithium 7, boron 11, nitrogen 15, oxygen 18, and hydrogen·deuterium for nuclear fusion·muon nuclear fusion, and there is an advantage that it can be more easily fused. <0049> <System using beryllium> Disclosed as one example of this application. A system for nuclear fusion reaction of beryllium 9 and protons may be used. Beryllium hydride BeH2 may be used as the raw material to be irradiated when irradiating muons.Hydrogenated beryllium is a solid and separates near its melting point, making it difficult to use as a fluid in a fusion system and there is a point where it cannot be used. p + 9Be -> 4He + 6Li + 2.1 MeV p + 9Be -> d + 2×4He + 0.6 MeV Beryllium 9 is a stable isotope of natural beryllium and occupies 100 percent of beryllium, so the isotope separation process can potentially be made unnecessary. Beryllium 9 exists in a large ratio in nature. Compared with lithium-7 of the lithium isotope in question (compared with boron-11 and nitrogen-15 as well), it has the characteristic of a larger cross-sectional area and may be advantageous in terms of cross-sectional area when using the system of this application. Beryllium borohydride Be(BH4)2 is a compound composed of boron, beryllium, hydrogen, and protons, and is a compound, inorganic compound, and inorganic polymer compound in which boron-11, beryllium-9, and hydrogen atoms can be chemically bonded and arranged in a close state, and can also be used as one form of this application. This substance can be used in liquid, solid, etc. In the reaction of boron-11 (Z = 5), helium (Z = 2) is produced, and in the reaction of beryllium-9 (Z = 4), lithium (Z = 3) and helium and deuterium are produced. The final products ZB group (helium, lithium, deuterium, ZB is 3) produced in these two reactions are fusion fuel atoms ZA group (boron-11, beryllium-9, hydrogen, ZA is 11 or 9). Therefore, since the nuclei of the fusion fuel atoms ZA group have a larger positive charge than lithium-6 with a positive charge of 3 in the final product, it can be inferred that negative muons are more likely to be captured by the fusion fuel atoms and can be used. <0050><Regarding resource quantity, etc.> From the perspective of the resource quantity in the universe and the earth's atmosphere, oxygen-18 and oxygen-17 of magic number 8 oxygen may be dominant. In addition, nitrogen-15 and boron-11 are dominant. Oxygen-18 and nitrogen-15 are contained in atmospheric nitrogen and can be separated from other isotopes of oxygen and nitrogen in the atmosphere by oxygen and nitrogen distillation processes. Carbon also has a large resource quantity. As the atomic number increases, there are also effects such as muons decaying into electrons and neutrinos due to weak interactions (the lifetime of negative muons decreases). Therefore, in nitrogen-15 (Z = 7) with a larger Z than lithium (Z = 3), this effect needs to be considered. In this application, the use of lithium is not restricted. (If Z is about 1 to 10, the lifetime of negative muons is close to microseconds. Therefore, if the time for acting as a catalyst in the fusion reaction can also be maintained at about microseconds, atoms up to Z = 10 can be used as candidates for the raw material atoms of the system of this application. Or up to Z = 20, etc. The lifetime of negative muons can be considered.) In this application, preferably, elements from Z = 9 to 3 are considered, and lithium-6, oxygen-18, nitrogen-15, and boron-11 are disclosed as examples, and examples using compounds in which they are chemically bonded to protons and deuterium as the second raw material are disclosed.<0051><Fluorine-based system>In an experimental system, a nuclear fusion system that generates oxygen-16 (Z = 8) and helium from fluorine-19 (Z = 9) and protons may be used. It is also possible to irradiate hydrogen fluoride, which is a compound of fluorine-19 and protons, with muons. (Hydrogen fluoride is highly toxic.) <0052><Oxygen-based system>A nuclear fusion system that generates nitrogen-15 and helium from oxygen-18 and protons may be used. It is also possible to irradiate hydrogen oxide, which is a compound of oxygen-18 and protons, water H2O (liquid, gas, vapor, fluid water H2O) with muons. In this case, nitrogen-15 is obtained (the reaction formula is Group A in FIG. 2 of the present application), and after that, nitrogen-15 and protons may be reacted as described above and used in a nuclear fusion reaction that generates carbon-12 and helium. Oxygen-18 exists at 0.2 percent. For example, on Venus, it exists as carbon dioxide in the atmosphere, and in the rocks of the moon, Mars, and asteroids (which may contain silicon oxide, aluminum oxide, iron oxide, etc.), oxygen atoms combined with metal elements (silicon, aluminum, iron, etc.) are contained, and there is a possibility that it can be easily obtained as a resource and may be collected when navigating in space. For oxygen isotopes, the desired oxygen isotope may be separated from oxygen in the atmosphere or substances combined with oxygen in celestial bodies (oxygen obtained by reducing rocks containing silicon oxide, etc.) by a known separation process. Oxygen-17 and protons may also be used. <0053><<Example where the atomic number Z does not decrease but the raw material atoms are chemically bonded to other raw material atoms>>As an example of the present application, an example is disclosed in which, before the nuclear fusion reaction, the atomic number ZB is greater than or equal to the atomic number ZA, and the first raw material atom ZA and the second raw material atom ZB serving as raw materials are provided in the same compound molecule. <Carbon-based system>In an experimental system, hydrocarbons containing protons and carbon may be irradiated with muons. A molecule in which carbon atoms and hydrogen atoms are chemically bonded may be used as a raw material substance, a nuclear fusion fuel, before the nuclear fusion reaction. For example, organic compounds containing carbon and hydrogen such as hydrocarbons and methane may be used. Muons or muonic hydrogen may be irradiated and introduced into organic compounds containing carbon and hydrogen such as methane.In the system using carbon and the system using hydrocarbons and organic substances such as methane, the hydrocarbons and organic substances such as methane (in the form of gas or fluid) may be compressed by the compression unit PUMP·RAM as shown in FIGS. 7 and 8. Muons such as muons or muonic hydrogen atoms may be introduced into the compressed locations (target parts T1, FP, PBH1, PMP1-XMB) to promote muon nuclear fusion at these locations. When using hydrocarbon gases such as methane and propane, the existing gas transportation, transport, and storage infrastructure can be utilized. Gas pipes, pipelines, valves, pumps, etc. can be diverted. (On the other hand, gases such as ammonia and boron hydride may require dedicated infrastructure, pipes, and pumps.) (When a negative muon approaches the atomic nucleus, the negative muon undergoes a weak interaction with the protons in the atomic nucleus, causing the protons in the atomic nucleus to change into neutrons and converting the atomic nucleus into an atomic nucleus with an atomic number one less. When carbon-12 is irradiated with muons, it becomes boron-11, and then a reaction between boron-11 and hydrogen atoms or protons can also be expected due to the muons that arrive again.) <Nuclear fusion between carbon atoms, carbon combustion, nuclear fusion reaction with atoms having a carbon or higher Z>Regarding the raw material FEED of the organic compound in which carbon atoms are bonded to each other as shown in FIG. 9 and the like, while heating (and compressing) the FEED using heating and compression means such as RAM and RAMH, muons and muonic atoms may be irradiated and introduced into the FEED to promote the nuclear fusion reaction between carbon atoms using muons. Also, for the purpose of experiments or for the purpose of nuclear conversion and artificially synthesizing elements with a larger atomic number Z, muonic carbon atoms having carbon atoms among muonic atoms may be collided with other atoms to promote nuclear fusion. In addition to nuclear fusion between carbon atoms, nuclear fusion between oxygen atoms in the oxygen combustion process, silicon combustion process, and nuclear fusion reactions between elements with a larger atomic number Z may be attempted in the system of the present application. <0054><System capable of heating or compressing the raw material FEED>As a configuration that can be compressed and heated in the RAM section (RAMH section) more than the configuration of FIG. 8, FIG. 9 discloses a system capable of irradiating a target section from an emission source such as (a plurality of) lasers, ion beams, microwaves, etc. to heat the FEED in the target section. (It may be compressed by a laser or an ion beam.) FIG. 9 is an example of a system 1F-SYS having a compression section and a heating section for the raw material FEED.(The figures are examples and are not limited to the experimental systems, reaction systems, devices, structures, and arrangements described in the figures. For example, in FIGS. 8 and 9, the FEED circulates within a closed cycle, but the FEED may be stored in a closed container or a batch-type container. The heating unit RAMH may be provided in the container storing the FEED or the reaction unit, and muons and muonic atoms may be irradiated and introduced into the FEED while heating the FEED with the heating unit RAMH. A laser may be irradiated (from a light source unit that may be a plurality of light source units) onto the container storing the FEED, such as in laser confinement inertial fusion, and the FEED may be confined and heated by the laser. Lasers, millimeter waves, microwaves, which are electromagnetic waves, electromagnetic induction, particle-based ion beams, and particle beams may be irradiated onto the container storing the FEED to heat the FEED. ) For example, the compression unit RAM in FIG. 9 may be irradiated with a laser or an ion beam. Laser compression may also be possible. Also, heating by lasers, photons, electromagnetic waves, electric and magnetic fields, radio waves, and beams may be possible. <3> <0055> As one form of the present application, FIGS. 7, 8, and 9 are explanatory diagrams of a fusion system using a raw material substance FEED containing raw material atoms in the molecule, the fusion system having a step of irradiating and introducing muons into the raw material substance, the raw material atoms including two or more raw material atoms having a first atomic number ZA, or raw material atoms including one or more atoms having a first atomic number ZA and one or more raw material atoms having a second atomic number ZAA, and the raw material atoms having a first atomic number ZA and a second atomic number ZAA that fuse are chemically bonded, covalently bonded, or ionically bonded and contained in the raw material substance. <4> <0056> As one form of the present application, FIG. 9 is an explanatory diagram of a fusion system including a step of irradiating and introducing muons and muonic atoms into the FEED, provided with a heating means RAMH and a compression means RAM for the raw material substance FEED. The heating means RAMH may use, for example, heating means by laser heating, ion beam heating, microwave, millimeter wave, electric and magnetic fields, or electromagnetic induction. FIG. 9 is, for example, an inertial fusion system that irradiates a laser (from a light source unit that may be a plurality of light source units) and confines with the laser, or a fusion system that may be heated by a laser, and is an explanatory diagram of a fusion system including a step of irradiating and introducing muons and muonic atoms into the FEED.Alternatively, FIG. 9 is an explanatory diagram of a fusion system that irradiates a container storing FEED with electromagnetic waves such as laser, millimeter wave, and microwave, electromagnetic induction, particle-based ion beam, particle beam, or millimeter wave to heat the FEED (in some cases, for example, by directing the ion beam at a single point so that the ion beam is irradiated multiple times toward a single point FP, T1, where the FEED is located, and the ion beam traveling toward a single point compresses, packs, or rams the FEED to compress it, performing compression and heating). It is an explanatory diagram of a fusion system including a step of irradiating and injecting muon - muonic atoms into the FEED. <5> <0057> As one form of the present application, (B) in the lower part of FIG. 3 of the present application shows lithium deuteride 6 in a solid, liquid, or molten state in the raw material FEED (when it is considered that the raw material atoms can move due to heat and the raw material atoms are likely to approach each other, preferably in a liquid or molten state), arranged in the target part T1. It is an explanatory diagram of a system for irradiating and injecting muons (muonic atoms) into the lithium deuteride 6. In (B) of FIG. 3, the lithium deuteride 6 and the T1 - FEED part may be heated using the heating means RAMH. (The FEED may be melted using the heating means RAMH and heated to a liquid state.) * Using lithium 6 with a larger cross - sectional area than lithium 7 and chemically bonding deuterium to form the raw material FEED, the raw material FEED may be heated by the heating means RAMH and arranged in the target parts T1, FP, PBH1, PMP1 - XMB. By irradiating and injecting muons (muonic atoms) into the arranged FEED, it is intended to promote muon - based nuclear fusion and connect it to a fusion system, fusion reactor, or fusion reactor. When lithium 6 with a larger cross - sectional area and deuterium are chemically bonded to form the raw material FEED, the cross - sectional area can be made larger than when using lithium 7, boron 11, nitrogen 15, oxygen 18, and hydrogen or deuterium for nuclear fusion or muon - nuclear fusion, and there is an advantage that nuclear fusion is easier. From the perspective of the cross - sectional area, lithium 6 is preferred over lithium 7, and it is preferable to use lithium 6 and deuterium. When using lithium 7, there is a problem of a small cross - sectional area. Therefore, in one example of the present application, the use may be limited to lithium 6 and deuterium to increase the cross - sectional area and attempt to solve the problem of the small cross - sectional area.<0058>Symbols, etc. <Figure 9> Mixture MP1-XMB compressed (and / or heated) by a compression means such as PMP1-XMB:RAM, or a mixture MP1-XMB compressed (and / or heated) by a compression means such as RAM. RAM: Compression means such as a RAM section. By laser irradiation. (When the RAM section is of the laser confinement / inertial confinement type, the wavelength of the laser light may preferably be a short wavelength on the blue, ultraviolet, X-ray, or gamma-ray side so that the momentum of the photons can be larger. Inertial confinement fusion that irradiates a nuclear fusion target fuel pellet and performs confinement is known. In the present application as well, the target section and the mixture may be compressed by a laser in the compression section RAM section. (A muon injection process may be added to inertial confinement fusion of the laser confinement type.) The RAM section may irradiate with a laser, an ion beam, or an ion beam containing raw material atoms so as to converge from a plurality of emission sections to a portion containing the raw material atoms (Fig. 9). (Inertial types such as Z-pinch and magnetized target type that can compress raw material atoms and can be confined by inertia may also be used.) In the RAM section, by compressing and heating a portion of raw material atoms that become fuel necessary for nuclear fusion, compounds or mixtures in which the raw material atoms are chemically bonded to each other, with a laser or the like while irradiating with muons, the molecular motion or atomic motion within the compound molecule or within the compound / mixture can be increased by compression and heating. As a result, particles bound to muons are more likely to approach each other due to thermal motion, and there is an intention to facilitate nuclear fusion, muon-catalyzed nuclear fusion, and muon-catalyzed fusion caused by the approach. In addition, there is also an aim to facilitate the next catalytic reaction in which muons that act as catalysts after nuclear fusion are (released and repeatedly approach and are captured by the next raw material atoms). (When irradiating muons to liquid hydrogen, DT, DD, or TT cooled to an extremely low temperature of several kelvins, there is a possibility that the effect of approaching raw material atoms due to thermal motion is low because of the low temperature. However, when injecting muons, muonic atoms, or muonic hydrogen into a portion compressed and heated by a laser or a ramjet section, etc., an approaching effect due to compression or thermal motion can be expected.) RAMH: Heating means. (It may be included in the RAM section. For example, means such as a laser or microwave that can irradiate a substance remotely with electromagnetic waves or photons and can heat the substance. For example, in a system using water, hydrogen peroxide, and muons, water can be heated by microwaves. Alternatively, the substance may be inductively heated electromagnetically.)For example, when using hydrocarbons as raw materials and promoting nuclear fusion between chemically bonded and adjacent carbon and hydrogen atoms in hydrocarbons using muons in the configurations shown in FIGS. 8 and 9, FIG. 9 is more likely than FIG. 8 to allow heating of the raw materials by a laser or the like. As the atoms and particles in the raw material substance reach a high temperature due to heating means such as a laser, their movement becomes more active, which may have the effect of promoting muon-catalyzed nuclear fusion. (Heating means such as laser heating, ion beam, neutral particle beam · NBI, ion beam or neutral particle beam · NBI containing raw material atoms, particle beam combining muons and ions · raw material atoms, millimeter wave, microwave, etc. may be used.) RAM and RAMH may be irradiated with a laser or ion beam. Laser compression may also be possible. Laser heating may also be possible. PUMP: Compressor, pump, motor FEED: Raw material substance (e.g., boron hydride, (hydrocarbon), hydrogen nitride, hydrogen oxide, etc.). (Lithium deuteride or other liquid or solid targets may also be used. Substances serving as raw materials for nuclear fusion reactions.) FEEDC: Feed control section. It may include a feed raw material substance supply section, fuel supply section, etc., and a section for removing products after nuclear fusion such as helium. FP: Nuclear fusion (promotion) section <0059><>. <nb1>A nuclear fusion system using a raw material substance containing raw material atoms, wherein the raw material substance is a nuclear fusion system using a fluid, gas, or liquid raw material substance, and having a step of irradiating and introducing muons into the raw material substance. The raw material atoms include two or more raw material atoms having a first atomic number ZA, or the raw material atoms include one or more atoms having a first atomic number ZA and one or more raw material atoms having a second atomic number ZAA. For the atomic number ZA of the raw material atom with the largest atomic number that undergoes nuclear fusion reaction and the atomic number ZB of the generated atom with the largest atomic number among the atoms and particles generated by the nuclear fusion reaction, the atomic number ZB is less than or equal to the atomic number ZA. <nb2>The nuclear fusion system according to NB1, wherein the atom of the first atomic number ZA and the raw material atom of the second atomic number ZAA that undergo nuclear fusion have a chemical bond, a covalent bond, or an ionic bond and are contained in the raw material substance. <nb3>The atom of the first atomic number ZA is boron 11 and nitrogen 15, and the raw material atom of the second atomic number ZAA is hydrogen and a proton. The fusion system described in NB1. <nb4>A muon-catalyzed nuclear fusion system characterized by introducing and incident on the nuclear fusion fuel material an atom, particle, or muonic atom in which a muon is bound to and added to a atomic nucleus. <nb5>A muon-catalyzed nuclear fusion system characterized in that, after muons or muonic atoms are introduced and incident on the nuclear fusion fuel substance, the nuclear fusion fuel substance is pressurized by a pressurizing means. <nb6>The muon-catalyzed nuclear fusion system according to NB1, which has the feature that after a muon or a muonic atom is introduced into and incident on the nuclear fusion fuel substance, the nuclear fusion fuel substance is mixed by a pressurizing means. <mmf1>A fusion system using a raw material substance containing raw material atoms, the fusion system having a step of irradiating and introducing muons into the raw material substance, (the raw material atoms include two or more raw material atoms with a first atomic number ZA, or the raw material atoms include one or more atoms with a first atomic number ZA and one or more raw material atoms with a second atomic number ZAA), the raw material atoms for fusion are (or the raw material atoms with a first atomic number ZA and the raw material atoms with a second atomic number ZAA are) chemically bonded, covalently bonded, or ionically bonded and are contained in the raw material substance. <mmf2>The atom of the first atomic number ZA is boron-11 or nitrogen-15, and the raw material atom of the second atomic number ZAA is hydrogen or a proton, or the atom of the first atomic number ZA is lithium-6 and the raw material atom of the second atomic number ZAA is deuterium, the nuclear fusion system described in MMF1. <mmf3>The atom of the first atomic number ZA is carbon, and the raw material atom of the second atomic number ZAA is hydrogen or a proton. (The raw material substance is an organic compound containing methane, hydrocarbon, and a bond between carbon and hydrogen.) The nuclear fusion system described in MMF1. <mmf4>A nuclear fusion system using a raw material substance containing raw material atoms, the nuclear fusion system having a step of irradiating and introducing muons into the raw material substance, wherein the raw material substance uses lithium deuteride (liquid) in which lithium-6 and deuterium are chemically bonded. <mhf1>A fusion system equipped with a heating means RAMH for a raw material FEED, the fusion system including a step of irradiating and introducing muon-muonic atoms into the raw material FEED. <mhf2>The heating means RAMH uses heating performed by irradiating a raw material substance FEED with a laser, an ion beam, a particle beam, a neutral particle beam, an ion beam or a neutral particle beam containing raw material atoms, or a particle beam in which muons are combined with ions and raw material atoms, or uses heating by radio waves, millimeter waves, microwaves, heating by an electric field or a magnetic field, or heating by electromagnetic induction for the raw material substance FEED, and is a fusion system described in MHF1 having this feature. <Document name>Book <><Problem>In known muon-catalyzed fusion, there has been a problem that in fusion fuel substances such as hydrogen, deuterium D, and tritium T, muons (muons) are attached, captured, and trapped by helium, which is the product substance after fusion, and the catalytic fusion stops. It was thought to solve the problem that muons are captured by the product substance after fusion rather than the fusion fuel substance, making it difficult for the muon-catalyzed fusion reaction to proceed. <Solution means>A system is disclosed in which, in fusion using muons, a fusion fuel substance and a raw material substance contain a raw material atom with a first atomic number ZA and a raw material atom with a second atomic number ZAA chemically bonded together. A muon-catalyzed fusion system using lithium hydride containing lithium 6 and deuterium, or diborane containing a proton and boron 11, or ammonia containing a proton and nitrogen 15 is proposed. Also, a fusion system using muons equipped with heating means and compression means is proposed. <0060><<Supplementary part by application claiming priority>>The following items were added to the previous applications, Japanese Patent Application No. 2023-150635, Japanese Patent Application No. 2023-151787, Japanese Patent Application No. 2023-174791, and Japanese Patent Application No. 2023-196029. <Document name>Book <><Problem>It is desired to make it easier to replace the muon target without stopping the muon fusion reactor. (It is desired to reduce the downtime during target replacement. It is desired to increase the target life.) Also, it is desired to miniaturize the muon generation unit and the accelerator. <Solution means>In a circular accelerator (fixed magnetic field strong focusing accelerator FFAG accelerator, MERIT ring, MERIT accelerator *MERIT: Multiplex Energy Recovery Internal Target method), a wedge-shaped or thin disk-shaped (insertable) movable target is used.The movable target may be replaceable by a replacement device, or there may be two or more movable target parts and solenoid muon extraction parts for muon capture, and the movable target part may be moved in and out and back and forth (at the MOVE position in Fig. 12) from the outer periphery to the inner periphery of the accelerator. The movable target may be irradiated with a proton particle beam to generate pion muons. <Embodiments for Carrying Out the Invention><0061><Problems to be Solved by the Invention><Problems of radiation of the muon target, replacement and maintenance, and reduction of downtime when muons cannot be generated>When generating muons, an accelerated high-energy proton beam is irradiated onto a target part for generating muons of carbon or lithium to generate pions, pions, and muons. At this time, the target part for generating pions and muons and the muon target that receive the proton beam irradiation deteriorate and become radioactive over time and need to be replaced. The target becomes highly radioactive at a level where it is difficult for humans to approach. Replacing the muon target has the problem of stopping the muon generation device and the muon fusion system. Therefore, a rotating muon target has been developed in which the irradiated time is dispersed and averaged over other parts of a rotatable disk by rotating the target part. In the muon fusion system, it may also be preferable if the replacement and maintenance of the muon target can be performed without stopping the muon generation part during the operation of the muon fusion system (·if the downtime when muons cannot be generated can be reduced) (commercially, for example, a muon fusion power plant does not need to stop power generation for a span of once every six months, three weeks, etc. for muon target replacement).<0062> <Solution> Means for solving the problems, form for carrying out the invention <Extending muon target life and reducing downtime with rotating muon target MU-DISK-TGT> In the circular accelerator 2MU-ACC-RING (FFAG accelerator 2MU-FFAG, MERIT ring, MERIT accelerator 2MU-MERIT-RING), (particularly in the MERIT-type ring) the muon target part is arranged to protrude in a wedge shape, and the rotating target part is a carburette-shaped rotating target part with a thin and sharp outer periphery (protruding in a sharp shape and wedge shape), or By using the rotating target MU-DISK-TGT, which is shaped like a record or disk and resembles a sharp rotating saw (a thin, narrow disk with a sharp outer tip, or a wedge-shaped rotating muon target MU-WEDGE-DISK-TGT in Figures 10, 11, and 12), we attempt to suppress and average the activation of the MERIT-type wedge-shaped muon target (fixed muon target), extend the muon target's lifetime, delay activation, and increase the time the muon target can be used. * For example, a rotating muon target MU-WEDGE-DISK-TGT or MU-DISK-TGT may be configured as shown in Figures 10, 11, and 12, which may be a wedge or triangle with the cross section of one side of the disk becoming thinner toward the outer periphery (it may also be a thin disk), and a movable muon target unit (2MU-GEN-ROT-TGT) may be configured which is equipped with a rotation means such as a motor that rotates the rotating muon target and a rotation support means such as a bearing, and the rotating muon target part MU-MOVABLE-TGT or MU-DISK-TGT may be capable of being inserted (or removed) into the particle beam orbit part of the accelerator (2MU-FFAG, 2MU-ACC-RING, 2MU-MERIT-RING) toward the particle orbit on the outer periphery of the accelerator. It may be provided in the target part and pion muon generation part of the muon generation device 2MU. (※Regarding the circular accelerator as a donut shape, a rotating muon target like a circular saw in the toroidal direction is inserted, pulled out, and can be moved in the part where particles circulate on the outer periphery of the donut and the protruding part of the wedge of the MERIT ring. A rotating target that can cut or pull out a cut with a circular saw in the ring may be inserted and removed from the 2MU-MERIT-RING in FIGS. 10 and 12.) ※As shown in FIG. 10, a wedge-shaped rotating muon target MU-WEDGE-DISK-TGT, or a rotating muon target MU-WEDGE-DISK-TGT with a thin plate-like movable part (the target MU-WEDGE-DISK-TGT may be rotatable, and the shape of the target is such that after the particle beam of the MERIT method hits the target, the particles can recover energy again inside the MERIT ring and circular accelerator, such as a wedge shape, a shape with a thin protruding part in the ring part, or a thin plate shape. ※In FIG. 10, a rotating muon target MU-WEDGE-DISK-TGT (having a wedge shape and a shape with a thin part) like a circular saw that cuts the outer peripheral side where particles pass perpendicular to the toroidal direction of the circular and donut-shaped particle accelerator, FFAG, and MERIT ring is inserted (so as to collide with the orbit of the particle beam accelerated and orbiting the outer periphery) into a part of the outer periphery of the accelerator cross-section and can rotate. In FIGS. 10, 11, 12, and 13, the operation of the particle accelerator, rotation, or insertion and movement (MOVE) of the rotatable or movable muon target may be possible while maintaining a vacuum, and replacement (EXCHANGE·SET) of the movable muon target may be possible. Motors (MU-TGT-MOT) and bearings (MU-TGT-BRG) are used for rotation. The wedge-shaped rotating muon target MU-WEDGE-DISK-TGT attached to the axis (AXIS-TGT-BRG) rotates across a part of the outer periphery of the circular accelerator, FFAG, and MERIT ring (the outer peripheral side of the ring donut). *Cross-sectional view CS part of FIG. 10, cross-sectional part CS from point CSP1 to CSP2.) <Replacement during muon target activation and removal of the activated part> Also, when the wedge-shaped rotating muon target is activated as shown in the right figure of FIG. 11, the activated tip may be cut, sliced, or severed to remove the activated part, and the less activated part may be recycled and used again.In addition, machines and robots may be used for unmanned operation. In the case of a rotating muon target, compared to a fixed target or a rotating target with a certain thickness, the area near the wedge-shaped and thinner part will be irradiated, and the thickness and volume of the area irradiated by the proton ion beam can be reduced, which is expected to lead to a reduction in the radioactive waste generated by irradiation. <During the muon generation operation and the accelerator operation, a system for cutting, maintaining the part of the rotating muon target irradiated by the beam where muon target irradiation is about to progress, and grinding and removing the irradiated part with a grindstone. A system for cutting, grinding, and removing during the muon generation operation, accelerator operation, and equipment operation before the target is highly irradiated.> As shown in the right figure of FIG. 11 of the wedge-shaped rotating muon target, during the operation of the muon generation unit, accelerator, and MERIT ring, a device capable of grinding or cutting a part of the target while rotating can be brought close to the irradiation part of the disk to grind and cut the irradiation part. Also, the irradiated part may be ground, cut, and removed by a cutting and removing device. (If grinding is exhausted and cutting is not possible, or if the surface of the disk cannot be formed by grinding during operation, it may be replaced with a new disk by a disk exchange machine or a robot arm.) <Use in space> This application also assumes use as a power unit of a spacecraft. For the accelerator system, the parts that require a vacuum may use the vacuum environment in space. <0063><Automation of replacement of movable muon target> As an example of replacement after proton irradiation and activation of a wedge-shaped rotating muon target for muon generation, an alternative system, and when replacing the target with one fixed muon target extraction port, FIG. 10 discloses a system capable of replacing the muon target.<0064>For example, in a device such as a jukebox, a record disk (wedge-shaped rotating muon target MU-WEDGE-DISK-TGT) can be replaced by a robot arm or the like. The device is a robot part (TGT EXCANGE ROBOT / ARM (JUKE BOX MACHINE LIKE)). The wedge-shaped rotating muon target MU-WEDGE-DISK-TGT is mounted on a shaft (2TGT-EXCHANGE-AXIS) that can be rotated by a plurality of motors (such as a rotary magazine of a rotary pistol or revolver) (2TGT-EXCHANGE-MOT) and a magazine part, disk holder, or arm (2TGT-EXCHANGE-ARM) that can be rotated by the rotating means 2TGT-EXCHANGE-MOT. The arm can be rotated to replace the wedge-shaped rotating muon target. Automation of the replacement may be performed. <0065>FIG. 12 describes the replacement, alternate system, (when two muon extraction ports and solenoids are arranged, and one extraction port is stopped and its target is replaced) after proton irradiation activation of the wedge-shaped rotating target for muon generation. Two systems of muon extraction ports, solenoids, and muon irradiation systems for nuclear fusion fuel are required. However, without the above-described replacement rotating mechanism, and the targets T1 of the irradiation system and the nuclear fusion reaction part can also be made into two systems, with the intention of reducing the downtime during which power cannot be generated. (In FIG. 12, there are two systems, but a plurality of systems may also be used.) In FIG. 12, the wedge-shaped rotating target part and the solenoid for muon capture and muon extraction part are provided with two or more, and the movable muon target part and wedge-shaped rotating target part MU-WEDGE-DISK-TGT can be moved in and out, moved back and forth, and inserted (at the MOVE part in FIG. 12) from the outer periphery to the inner periphery of the accelerator. The movable target part is moved (MOVE), pushed out, inserted, pulled out, and pulled back into the MERIT ring, and whether the proton beam collides with the wedge-shaped rotating target part is controlled by the MOVE step and the insertion / removal step. The generation of pion muons at one extraction port can be controlled on and off. When replacing the target part in FIG. 12, it is completely pulled out and pulled back from the MERIT ring for maintenance and replacement. Replacement and the like may be automated using a machine or robot (TGT EXCANGE ROBOT / ARM).<0066><Problem><Miniaturization of a muon-generating device, necessity of a small accelerator and a small muon generator>It is preferable to miniaturize a system (accelerator, accelerating cavity, deflection magnet) for generating muons. When it is desired to mount the fusion system on transportation equipment, spacecraft, spaceships, aircraft, vehicles, ships, submarines, various facilities, and robots, it is preferable that the size of the system including the accelerator and the muon generation device can be reduced.<0067><Solution>Means for solving the problem, mode for carrying out the invention 〇Regarding the muon generation unit, as a high-intensity muon source, a multiplex energy recovery internal target method (MERIT method) using a fixed magnetic field strong focusing accelerator (FFAG accelerator, FFAG: Fixed Field Alternating Gradient, an accelerator having a gradient magnetic field shape with a constant magnetic field (static magnetic field) and alternating the gradient direction) which is a circular accelerator is known. A wedge-shaped target is installed on the beam orbit such as protons inside the ring, the beam is circulated, stored, accumulated, and accelerated, and at the same time, the beam is irradiated onto the target to generate secondary particles. And among the beams that have been irradiated onto the target once, those that have not reacted with the target can also be (re-accelerated and) energy recovered, and by continuously hitting the target multiple times, it is possible to generate secondary particles with high efficiency. This method may be used for the muon generation unit M1 and the particle accelerator of the present application.<0068>In the MERIT method, protons incident on the center of the MERIT ring transition to an outer orbit while accelerating and rotating inside, and enter a muon target section that protrudes outward in a wedge shape and in a thin plate shape, generating pions and muons while being re-accelerated and energy recovered, and then colliding with the target again to generate pions and muons.The generated pions and muons are introduced into the solenoid for muon capture and transport (MUON CAPTURE TRANSPORT SOLENOID in FIGS. 10, 11, 12, and 13), and then those containing muons are irradiated and introduced into the target section T1 (selected isotopes, lithium hydride (lithium deuteride 6), boron hydride, hydrogen nitride, hydrogen oxide, hydrogen fluoride, etc., hydrocarbons, etc., raw material substances) and the nuclear fusion reaction section FP of the muon fusion system 1F-SYS from the said section (optionally passing through an acceleration section, a deflection section, or various devices, etc., and may remain as muons, may become a neutral particle beam, or may be made into muonic atoms). Note that in the present application, as described above, a movable muon target section MU-MOVABLE-TGT and a wedge-rotating target section MU-WEDGE-DISK-TGT may be used for the muon target. By using the wedge-rotating target section, the target can potentially have a longer lifespan than a fixed wedge target. By adopting the configurations shown in FIGS. 10, 11, 12, and 13, it is intended to miniaturize the muon generation device and extend the lifespan of the target and the device (by increasing the time of radioactivity). <0069><Acceleration Cavity>Regarding the synchrotron and circular accelerator that generate muons, it may include an acceleration cavity for acceleration and deflection magnets (such as quadrupole magnets) for controlling, converging, and bending the orbits of the accelerated particles and protons. Regarding the acceleration cavity, it is known that a niobium plating and coating can be applied to a copper cavity to make it a superconductor, and a superconducting acceleration cavity can be used, and it can be used because it can reduce power consumption. Also, the proton, ion, and particle acceleration methods using plasma by high-intensity lasers (ion and electron acceleration by laser plasma drive, Laser Wake Field Acceleration (LWFA), those using the ponderomotive force of the laser) are known, and by using a cavity capable of laser particle acceleration, the acceleration cavity part can be miniaturized. (When used for the acceleration cavity part of the muon generation section of a muon fusion reactor mounted on a device that can move, such as a transport device, spacecraft, aircraft, vehicle, ship, submarine, exploration robot, etc., and is preferably miniaturizable, it is considered preferable.) Therefore, the proton acceleration method using plasma by the said laser, LWFA, etc. can be used to configure a laser-utilization type accelerator or a muon generation section.<0070><Deflection Magnet><Muon Capture Transport Solenoid, Conductor, and Electric Wire within the System of this Application>〇For the deflection magnet, quadrupole electromagnet, and muon capture solenoid section, a superconductor may be used. For the deflection magnet, quadrupole electromagnet, and muon capture solenoid section, a superconductor may be used.●For the wire section, deflection magnet, quadrupole electromagnet, and muon capture solenoid section of the system of this application, (for the purpose of avoiding the problem of using an electrically conductive wire while enhancing the conductivity of a carbon material or the like, or making the wire lighter by changing the conductor from copper to a carbon-based material, reducing the amount of copper used, eliminating the cooling procedure and cooling equipment for superconductivity, and refraining from using substances with a long half-life such as niobium in the superconductor), a 1WIRE conductor that can charge the capacitor portion composed of the insulator, material portion, and gate electrode of the transistor by the voltage applied to the gate electrode disclosed in Japanese Patent Application No. 2022-123161. A carrier introduction portion (104) is formed in the material portion (101) by applying a voltage (VGS) between the first electrode (106) and the second electrode (102). It is an element capable of changing the conductivity of the material portion (101) including the carrier introduction portion (104). The material portion (101) of the element includes the channel portion of the transistor, and the carrier introduction portion (104) is the channel portion. includes minutes, and the first electrode (106) of the element is the gate electrode (106) of the transistor, the second electrode (102) of the element is the source electrode (102) of the transistor, and the element has a feature that a capacitor portion composed of the insulator (105) of the transistor, the material portion (101), and the gate electrode (106) can be charged by the voltage (VGS) applied to the gate electrode (106). A 1WIRE conductor using the element, or a conductor in which a capacitor portion composed of the insulator of the transistor, the material portion, and the gate electrode can be charged by the voltage applied to the gate electrode, and the material portion is a porous film or has a space that becomes a gap with respect to the total volume of the material portion, or the surface area of the interface where the material portion contacts the insulator is larger than the total surface area of the material portion. A deflection electromagnet including the 1WIRE conductor may be used in the muon generation unit and particle accelerator of the present application. The particle accelerator, muon generation unit, and fusion system of the present application may include an electric circuit including the 1WIRE. <Magnetic levitation method of bearing> Known bearing and supporting means may be used as a supporting portion when moving the movable muon target portion. Or a magnetic levitation type bearing may be used to increase the lifespan. The system of the present application is also considering utilization in space, spacecraft, and spaceships. In space, there may be a vacuum and zero gravity. While utilizing zero gravity (or while utilizing zero gravity in space but equipped with magnetic levitation, magnetic conveyance, movement, levitation control, and levitation mechanism), a rotating muon target portion that rotates in a vacuum may be configured in a spacecraft in space. As shown in FIG. 10, it may be inserted so as to pass through a part of the cross section obtained by cutting the outer periphery of the MERIT ring in the poloidal direction, and the rotating muon target portion may rotate. <Utilization of vacuum and zero gravity in space> The system of the present application, the muon generation unit of the present application, the MERIT ring type particle accelerator from FIGS. 10 to 13, the movable muon target, the muon capture solenoid, and the fusion system unit 1F - SYS may utilize the vacuum and zero gravity environment in space for operation. For example, the acceleration tube and cavity inside the accelerator can be evacuated and constructed to have strength to withstand the force pushed by atmospheric pressure. As a result, it may become a heavy accelerator used to ensure strength such as steel.In the other cosmic space, it is pre-evacuated to a high vacuum without air and atmospheric pressure. Therefore, there are fewer components for ensuring the strength to keep the accelerator in a vacuum and fewer vacuum pumps, resulting in a smaller number of components, lower strength, and lighter weight. This can reduce the number of components and the launch weight when lifting members from the Earth into space, thereby reducing costs. Therefore, devices and systems such as the nuclear fusion system, particle accelerator, and pion and muon generation system of the present application may be used in cosmic space. In addition, the system of the present application may be installed for power sources and power sources for the movement and operation of transportation equipment, spacecraft, space bases, spaceships, and exploration robots in cosmic space, as well as for particle experiments using particles. <0072><Another form of the rotatable and movable muon target part>In FIGS. 10-12, the rotating muon target is in the shape of a disk, but the shape is not limited thereto. For example, as shown in FIG. 13, a target part is attached to the rotating chip part and the saw chain part of a chain saw to form a movable muon target part. The saw chain part is inserted into and circulated through the accelerator so as to pass through a part of the cross-section obtained by cutting the outer peripheral part of the MERIT ring in the poloidal direction as shown in FIG. 10 and return to the chain catcher part. The muon target part may rotate, and the muon target part on the chip may generate pions and muons by the collision of ions, protons, and particles having energy. From the perspective of activation, it is preferable that the target part is a light element, and elements with a low Z such as lithium and carbon are used. (When using an element with a large Z, there are concerns about management costs due to a long half-life during activation.) The chip part may be removed before the degree of activation becomes strong when it is activated and replaced with a new wedge-shaped or thin chip-shaped muon target. The muon target may be able to pass through and be movable through the particle irradiation part in the particle accelerator, FFAG, and MERIT ring of the present application. <6><0073>. <mt1>FIG. 10, FIG. 11, FIG. 12, and FIG. 13 are explanatory diagrams of a particle accelerator (MERIT ring) that generates, captures, and irradiates muons to a muon utilization system and a muon fusion system, a movable protruding / inserted wedge-shaped thin movable muon target, a rotating muon target, and a generation section of pion muons generated by the collision of particles / particle beams having energy with the target, a pion muon generation section, and a muon capture solenoid that captures pion muons and transports them toward a target section. ● In the present application, it is considered desirable to miniaturize the size of the fusion system using muons so that it can be mounted on the above-described transport equipment, and the acceleration cavities of the circular accelerator may use superconducting, laser wakefield acceleration type acceleration cavities, or acceleration cavities using lasers. ● Further, the movable muon target and the rotating muon target may be replaced by unmanned machinery so that humans do not approach highly radioactive targets and members by machinery or a robot arm. ● The muon target is movable so as not to stop the particle accelerator, the fusion system, or the power generation system (so as to reduce the above-described downtime) due to the replacement of the muon target caused by the activation and deterioration of the target, and to avoid continuous irradiation of the particle beam to one point for a long time. Irradiation of the particle beam is performed on other surfaces of the target, and the irradiation portions are dispersed so that the target can be used for a long time. <mt2>Figure 12 shows a system equipped with two movable targets and two muon capture solenoid - muon extraction ports, and then injecting muons into two sets of two nuclear fusion systems - nuclear fusion reactors, irradiating the targets T1 and the nuclear fusion reaction points FP in the nuclear fusion systems to promote muon - nuclear fusion (or various muon - related experiments and irradiating muons on substances for nuclear conversion such as radioactive waste, nuclear fusion, and muon application experiments are possible). One of the two extraction ports is put on hold to replace and maintain the movable target at that location. In Figure 13, the movable target can be replaced and maintained at the part that catches the movable target. <0074>Symbols etc. <Figure 10>MU - MOVABLE - TGT: The part receiving the particle beam is movable (muon) target part. MU - DISK - TGT: The part receiving the particle beam can be rotatable and movable, and can be a disk - type target part. Muon target part. MU - WEDGE - DISK - TGT: A muon target part that is movable and can be of the disk - type, where the thickness of the part receiving the beam irradiation is thin, and the cross - sectional shape becomes thinner towards the outer periphery of the disk, being wedge - shaped. MU - TGT - BRG: Support means such as bearings for supporting the movable part during movement and rotation. AXIS - TGT - BRG: When moving and in the case of rotational movement, its rotation axis. 2MU - GEN - ROT - TGT: Means for making the muon target part and the muon target movable, a target unit part equipped with a motor and bearings. 2MU: An example of the muon generation part M1. (It may include a target, an accelerator, a charged - conversion beam incident part, a part for adjusting the charge, a proton particle beam incident part, a proton particle beam accelerator part, a muon capture solenoid, etc.). Muons at M1 can be combined with protons and atomic nuclei to generate (neutral particle beam) muonic atoms MP1. 2MU - ACC - RING: Circular accelerator, particle accelerator. 2MU - FFAG: FFAG accelerator. 2MU - MERIT - RING: MERIT ring - type accelerator (The target of the wedge - shaped part can be movable and inserted. A movable muon target that becomes thinner towards the inserted tip can be inserted. The muon target part can be formed on the outer periphery of a rotatable disk or the tip of a chain saw and be movable).Irradiate the inner circumferential side of the circumference of a circle with a proton particle beam, and then perform circular acceleration and spiral acceleration by the accelerator and the ring, so that it becomes high-energy and high-speed on the outer circumferential side and transitions. Then, while colliding with the movable muon target, it may decelerate and still recover energy and be able to collide with the target again. (The particle may decelerate due to target collision, move in the inner circumferential direction, be accelerated again, transition to the outer circumference, and collide again. It is an accelerator in which particles are stored, accumulated, and re-accelerated in the ring.) 2MU-FFAG-CS·2MU-ACC-RING-CS·2MU-MERIT-RING-CS: When the accelerator is regarded as a donut, it is a cross-section perpendicular to the toroidal direction and a cross-section cut in the poloidal direction, which is the cross-section of the accelerator when cut between point CSP1 and point CSP2. A movable target (for example, a thin disk-shaped muon target) into which a particle beam accelerated to high energy on the outer circumferential side of the circular accelerator and the MERIT ring is inserted can be inserted and moved in the outer circumferential direction of the circle of the accelerator cross-section. CS: The cross-section CS between point CSP1 and point CSP2 <Figure 12>·Replacement after proton irradiation and activation of the rotating target for muon generation, an alternating system at two locations, with a movable muon target section, a muon extraction port, and a muon capture solenoid that can be inserted, removed, and moved inside the accelerator. An explanatory diagram when one extraction port is put on hold, the muon target section is removed from the accelerator and replaced, and the muon target section is replaced. 2MU-GEN-ROT-TGT: A movable muon target section unit / system that can be moved, inserted, and ejected inside the accelerator. MUON CAPTURE TRANSPORT SOLENOID: Muon capture transport solenoid <Figure 11> 2TGT-EXCHANGE: A device for replacing the movable muon target with a mechanical robot, the target exchange unit 2TGT-EXCHANGE-ARM: The arm part of the exchange unit·Robot arm 2TGT-EXCHANGE-AXIS: The rotating axis of the exchange unit 2TGT-EXCHANGE-MOT: The motor of the exchange unit * It may be a device like the record replacement part of a jukebox. TGT EXCANGE ROBOT / ARM: (JUKE BOX MACHINE LIKE) <Figure 13> An example of a movable muon target, an example having a part that makes a chain-saw-like (or cableway-like and lift-like) target movable.CHAIN-CATCHER: It is also the chain catcher part of the chainsaw, and it is a part where the muon target part MU-MOVABLE-TGT on the saw chain can be replaced by a machine such as a robotic arm. Chain-Sow-and-TGT: The guide bar part that guides the saw chain part to which the muon target TGT of the chainsaw is attached. (In FIG. 13, the muon may be decelerated by the muon decelerator MUDECE.) <0075><>. <mt1>A rotatable disk-shaped muon target, or a muon generation unit, muon target unit, muon target, or target provided with a rotatable and movable target part MU-MOVABLE-TGT · MU-WEDGE-DISK-TGT, wherein (for example, in the cross-sectional part from the inner peripheral part to the outer peripheral part of the disk, the outer peripheral part is thick and wide, the outer peripheral part is thin, narrow, and sharp, or with respect to the thickness of the disk, the central part of the disk is thick and the outer peripheral part of the disk is thin), a muon generation unit provided with a disk-shaped muon target, (the outer peripheral part of the disk or wheel is thin, pointed, wedge-shaped, or in the shape of a mortar wheel or a circular saw), the disk-shaped muon target is irradiated with a proton beam or particle beam at a point on the outer periphery of the circle of the circular accelerator or in its vicinity, and it is possible to generate pions, pi mesons, and muons. <mt2>The muon generation unit according to MT1, which has a target part using lithium-carbon (a material with a low atomic number Z) capable of generating pion muons. <mt3>A muon generation unit in which the muon target part is dynamic and movable, or a part that becomes a muon target part and is made radioactive is moved, and a muon generation unit (muon target) in which the radioactive part can be dispersed on a disk or a plate. <mtex1>A muon target is a muon generation unit that can be replaced by a mechanical device, and a rotatable disk-shaped muon target, or a rotatable and movable target unit (MU-MOVABLE-TGT·MU-WEDGE-DISK-TGT) is provided to the replaceable accelerator (·muon generation unit·muon nuclear fusion system). <mermt1>The target part of the rotatable and movable target part MU-MOVABLE-TGT described in MT1 is such that a part of the outer peripheral part is perpendicular to the outer circumference of the circle with respect to the circumferential direction and toroidal direction of the MERIT ring, FFAG ring, circular accelerator, and doughnut-shaped accelerator. A cross-section (a cross-section cut in the poloidal direction, a poloidal cross-section) obtained by cutting, and in the part through which the orbit of the proton beam or particle beam passes, an accelerator (target, muon generation part, muon nuclear fusion system, transport equipment equipped with a muon nuclear fusion system) in which the muon target can be inserted, removed, and arranged. <merlsr1>(For the purpose of miniaturizing the acceleration cavities of an accelerator,) a proton acceleration method using plasma by a laser, an ion / electron acceleration by laser plasma driving, a laser wakefield acceleration (LWFA), an accelerator using the ponderomotive force of a laser (· muon generation unit, muon fusion system, transportation equipment equipped with a muon fusion system). <0076><<Addendum to the application claiming priority>> The following items are added to the previous applications, Japanese Patent Application Nos. 2023-150635, 2023-151787, 2023-174791, 2023-196029, and 2023-196327. (This application is a utility model and requires demonstration)<<<Description regarding the raw materials and fuel substances of the muon fusion system and muon conversion system>>><Mode for carrying out the invention><Electronegativity: From the perspective of a relative measure of the strength with which an atom attracts electrons> There is electronegativity as a measure of the scale by which a atomic nucleus attracts electrons and negative charges. According to the electronegativity of arenes, it can be expected that fluorine electrons have a higher electronegativity than helium atoms and are more likely to attract electrons and muons. Therefore, according to the electronegativity of arenes, when muons are irradiated onto hydrogen fluoride and fused to produce helium, from the perspective of electronegativity, muons may be more likely to be attracted to the fluorine in hydrogen fluoride than the helium produced after nuclear fusion. From this perspective, it is also possible to implement the invention of this application by introducing muons into hydrogen fluoride (which may also be a liquid or gaseous fluid of hydrogen fluoride) to promote nuclear fusion. <From the perspective of effective nuclear charge> Regarding the effective nuclear charge, the effective nuclear charge and charge felt by the 1S orbital are [helium He: 1.688, hydrogen H: 1.000, lithium Li: 2.691, beryllium Be: 3.685, boron B: 4.680, carbon C: 5.673, nitrogen N: 6.665, oxygen: 7.658, fluorine F: 8.650, neon Ne: 9.642, sodium Na: 10.626, potassium K: 18.490, rubidium Rb: 36.208, cesium Cs: greater than Rb].In terms of the effective nuclear charge, when a muon is introduced into a system containing boron, nitrogen (and hydrogen) and a nuclear fusion reaction that generates helium occurs, the effective nuclear charges of boron and nitrogen in the nuclear fusion fuel have the characteristic of being larger than the effective nuclear charge of helium in the nuclear fusion product, and since the muon can be expected to be attracted to boron and nitrogen with a larger effective nuclear charge than helium, it can be used in the nuclear fusion system of the present application. Regarding the nuclear fusion reaction system, in the present invention, a nuclear fusion reaction system in which the effective nuclear charge of the atomic nucleus of the nuclear fusion fuel is larger than the effective nuclear charge of the atomic nucleus of the product after nuclear fusion may be used. (A nuclear fusion reaction system having a raw material atom for nuclear fusion having an effective nuclear charge larger than the effective nuclear charge of the atomic nucleus generated by nuclear fusion may be used.) <From the perspective of muon-catalyzed nuclear fusion in molecules having a chain or polymer structure> &l...

Claims

1. A nuclear conversion system having the characteristic that muon particles, or muon particles generated using cosmic rays, or cosmic ray muon particles can be decelerated using a decelerator, A nuclear conversion system capable of binding the muons decelerated by the decelerator to raw material atoms to be nuclear-converted, The decelerator is, Using a laser wakefield, or using an electric field, or using a magnetic field, Or using an electric field within a material, or using a magnetic field within a material, Or using a plurality of stacked capacitors or a multilayer capacitor, Or using an electric field generated by a capacitor, Or using a material, or using a material containing raw material atoms to which the muons decelerated in muon nuclear conversion are to be bound, or using a dielectric material, or using an insulator material, or using ionization cooling, or using frictional cooling, A nuclear conversion system using a decelerator having the characteristic of being able to decelerate the muon particles, The muons decelerated by the decelerator, Transportable to the raw material atoms, Or connectable to the decelerator and the raw material atoms, Or bindable to the raw material atoms provided in the decelerator, Or bindable to the raw material atoms contained in the decelerator, a nuclear conversion system.

2. The nuclear conversion system according to claim 1, having a step of nuclear-converting to an atom having an atomic number smaller than that of the raw material atoms to be nuclear-converted.

3. The nuclear conversion system according to claim 2, wherein the raw material atoms are atoms of boron, carbon, nitrogen, oxygen, or fluorine, and having a step of irradiating / introducing the decelerated muons to the raw material atoms.

4. A nuclear conversion system provided with a muon particle decelerator having the characteristic that muon particles generated using cosmic rays or cosmic ray muon particles can be decelerated using a decelerator.

5. The nuclear conversion system according to claim 4, capable of binding the muons decelerated by the decelerator to raw material atoms to be nuclear-converted.

6. A compression device that may obtain propulsion using a nuclear conversion system, A pressurizing device that compresses a material using centrifugal force.

7. A compression device that compresses a material using centrifugal force, a pressurizing device that applies centrifugal force to a material arranged in a ring shape and compresses the material arranged in a ring shape by the centrifugal force.

8. The pressurizing device according to claim 7, wherein the material is hydrogen, helium, lanthanum hydride, calcium hydride, a high-pressure-induced superconducting material, or a quantum solid.

9. The material is a high-pressure-induced superconducting material, which, when compressed into a superconductor, conducts a superconducting current to form a coil and a magnet. The pressurizing device according to claim 8.

10. The material is a high-pressure-induced superconducting material, which, when compressed into a superconductor, conducts a superconducting current to form a coil and a magnet. A superconducting magnet including the pressurizing device according to claim 9.

11. A magnetic device capable of bending the trajectory of charged particles using the magnet according to claim 10.

12. A magnetic sail device using the magnet according to claim 10.

13. A nuclear conversion system using the material atoms of the pressurizing device according to claim 7 as raw material atoms, the nuclear conversion system having the feature that muon particles, or muon particles generated using cosmic rays, or cosmic ray muon particles can be decelerated using a decelerator, the nuclear conversion system capable of binding the muons decelerated by the decelerator to the raw material atoms to be nuclear-converted.

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