High-charge heavy-ion high-energy laser

Abstract

The invention discloses a high-charge heavy ion high-energy laser. A high-intensity single-charge heavy ion beam is obtained by transversely colliding a single-charge heavy ion beam injection section with a low-speed multi-surface side-by-side correlation surface electron flow containing an unionized atom return channel; a high-intensity single-charge heavy ion beam is converted into a high-intensity high-charge heavy ion beam with the ionization degree of mu by adopting a flat runway-shaped high-speed multi-surface side-by-side correlation surface electron flow transverse collision high-charge heavy ion ionization ring with two high-charge ionization regions; high-charge heavy ion high-energy laser and heavy ion beam emission is realized by adopting a flat runway-shaped high-speed multi-surface side-by-side correlation surface electron flow to transversely collide with a high-charge heavy ion excitation ring. The total intensity of surface electron flow, strong laser and heavy ion beam can be greatly improved by adopting the high-capacity supercapacitor connected in parallel, and the overall weight can be reduced by adopting the electrified guide coil to replace a magnet. According to different laser wavelengths and powers, various practical purposes can be achieved from obtaining of a high-contrast holographic image of an internal atomic structure of a organism to serving as a novel high-energy laser weapon.

Description

Technical Field

[0001] The present invention belongs to large-scale electromechanical products, and particularly relates to a high-charge heavy-ion high-energy laser. Background Art

[0002] Currently, in laboratories, single-beam lasers with wavelengths in the range of... have been obtained by using the longitudinal collision ionization excitation transition of low-charge ions such as hydrogen-like, lithium-like, neon-like, and nickel-like ions, but the monochromatic brightness is small, the power is low, the wavelength is not short enough, and it cannot be practically applied. ... The monochromatic brightness is small, the power is low, the wavelength is not short enough, and it cannot be practically applied.

[0003] On February 7, 2018, after the applicant made the fourth major improvement to the invention patent application "High-speed surface electron flow transverse back-and-forth collision high-charge heavy-ion double-beam laser emission device" (ZL 200910164613.8) announced and authorized on August 26, 2013, the utility model patent application "Multi-faceted cross-opposite surface electron flow transverse collision high-charge heavy-ion high-energy double-beam laser" (ZL 2018 2026 2863.x) was submitted and announced and authorized on April 00, 2020. By using them, it is expected to overcome the above difficulties that cannot be practically applied. The present invention application is a further major improvement to the above invention patent application (ZL2018 20262863.x), and it is expected to achieve more significant effects. Summary of the Invention

[0004] The object of the present invention is to overcome the serious defects of the current laser emission devices, solve the technical problem of how to generate and utilize the high-speed multi-faceted cross-opposite surface electron flow transverse back-and-forth collision ionization excitation transition of high-charge heavy ions to obtain a practical high-energy laser with greater monochromatic brightness, higher power, and shorter wavelength, and at the same time provide a set of emission devices that can generate a higher-intensity high-speed multi-faceted cross-opposite surface electron flow and high-charge heavy-ion beam, and obtain a practical high-charge heavy-ion higher-intensity high-energy laser with greater monochromatic brightness, higher power, and shorter wavelength by the transverse back-and-forth repeated collision excitation of the high-charge heavy-ion beam by the high-speed multi-faceted cross-opposite surface electron flow. Since it is much easier to accelerate electrons than heavy ions, the present invention can greatly miniaturize the device.

[0005] The present invention patent application can open up a new way for the research and application of high-energy lasers.

[0006] The technical problems to be solved by the present invention are as follows:

[0007] 1. In the same isoelectronic series of ions, the heavier the ion and the more its charge, the shorter the wavelength of the same transition. Therefore, to obtain a laser with a shorter wavelength, it is necessary to obtain highly charged heavy ions with a higher degree of ionization and more charge. To obtain a laser beam with a greater monochromatic brightness and higher power, the density or beam current intensity of the highly charged heavy ions used must be greater, and the surface current intensity for ionization and excitation must also be greater. Currently, the method of obtaining highly charged heavy ions is to use large ion sources and giant accelerators to accelerate low-charge ions to a very high speed and then collide them with a target to obtain highly charged heavy ions. These devices are huge and consume a great deal of energy, but the intensity of the highly charged heavy ion beam obtained is very small, and it can only be used for nuclear reaction radiation spectroscopy and atomic spectroscopy analysis experiments and cannot be used for practical laser experiments. How to obtain a higher-intensity highly charged heavy ion beam and a higher-intensity surface electron current using ordinary small and simple electromechanical devices is the first technical problem to be solved by the present invention.

[0008] 2. Although the current intensity for ionization and excitation is very high at present, it is all linear and can only collide longitudinally with the heavy ion beam. Longitudinal collision equipment is simple, but limited by the free path, the energy of electrons during collision cannot be very high, and the energy of each collision has a great deal of uncertainty. The number of electrons whose energy can just excite the heavy ions to a certain laser energy level is very small, and the energy of most electrons is converted into the thermal energy of the heavy ions and wasted, and the efficiency of converting electrical energy into light energy is very low, resulting in a very weak laser intensity and a very small monochromatic brightness. How to make each electron colliding with the heavy ions collide with the heavy ions with a definite energy that can just excite the heavy ions to a certain laser energy level, so that the energy of each electron can be fully converted into the excitation energy of the heavy ions and be converted into the light energy of the laser through spontaneous emission. This is the second technical problem to be solved by the present invention.

[0009] 3. In the patent application for invention "High-energy double-beam laser with multi-faceted cross-opposing surface electron flow for transverse collision of highly charged heavy ions" (ZL 2018 2026 2863.x) submitted by the present applicant after four major improvements, the intensity of the surface electron current that can be generated and the laser intensity that can be obtained are relatively large, but they are still not large enough. How to make the intensity of the surface electron current that can be generated and the laser intensity that can be obtained even greater is the third technical problem to be solved by the present invention.

[0010] Technical solution

[0011] A high-charge heavy-ion high-energy laser is divided into two types due to different partial structures: a four-sided side-by-side opposed electron flow transverse collision high-charge heavy-ion high-energy laser and a five-sided side-by-side opposed electron flow transverse collision high-charge heavy-ion high-energy laser. Its characteristics are as follows: The high-charge heavy-ion high-energy laser consists of a low-speed multi-sided side-by-side opposed electron flow transverse collision single-charge heavy-ion injection section (A) containing an un-ionized heavy atom return channel (1', 1"), a flat runway-shaped high-speed multi-sided side-by-side opposed electron flow transverse collision high-charge heavy-ion ionization ring (B) connected through a single-charge heavy-ion beam output / input channel (7') and the low-speed multi-sided side-by-side opposed electron flow transverse collision single-charge heavy-ion injection section (A), a flat runway-shaped high-speed multi-sided side-by-side opposed electron flow transverse collision high-charge heavy-ion excitation ring (D) connected through a first high-charge heavy-ion beam output / input channel (21.1), a second high-charge heavy-ion beam output / input channel (21.2), and the flat runway-shaped high-speed multi-sided side-by-side opposed electron flow transverse collision high-charge heavy-ion ionization ring (B), which can output both high-energy laser and high-charge heavy ions, and their required power, electrical, vacuum, and cooling auxiliary equipment. The flat runway-shaped high-speed multi-sided side-by-side opposed electron flow transverse collision high-charge heavy-ion ionization ring (B) is installed in a sealed flat cuboid large ionization box (38) evacuated to a vacuum. The flat runway-shaped high-speed multi-sided side-by-side opposed electron flow transverse collision high-charge heavy-ion excitation ring (D) is installed in another sealed flat cuboid large excitation box (39) fixed on top of the flat cuboid large ionization box (38) and evacuated to a vacuum. Their required power, electrical, vacuum, and cooling equipment are all installed in the front part of another flat cuboid large accessory box (40) located below the flat cuboid large ionization box (38). The low-speed multi-sided side-by-side opposed electron flow transverse collision single-charge heavy-ion injection section (A) is installed in the evacuated rear part of the flat cuboid large accessory box (40).

[0012] The low-speed multi-faceted side-by-side opposed electron beam transverse collision single-charge heavy ion injection section (A) consists of a high-temperature atomic furnace (1) equipped with a high-frequency induction heating circuit and located on the left rear side of a flat cuboid large accessory box (40), a low-speed multi-faceted side-by-side opposed electron beam transverse collision single-ionization region (a) connected to the regular octagonal or regular decagonal furnace mouth (2) of the high-temperature atomic furnace (1) and located on the right rear side in the middle of the flat cuboid large accessory box (40), with a slightly higher voltage than the single ionization voltage of heavy atoms applied, a gradient heavy ion acceleration tube (5) connected to the rear of the low-speed multi-faceted side-by-side opposed electron beam transverse collision single-ionization region (a) and consisting of 50 - 100 regular octagonal or regular decagonal metal frames made of copper tubes, silver tubes or gold tubes slightly larger in cross-section than the furnace mouth (2) and with an insulating film wrapped on the outside, and 49 - 99 first high resistors (12.1) connected in series alternately, a quarter-circular negatively charged metal strip (7) bent upward and located on the right side of the single-ionized heavy atom beam (4) and connected to the rear of the gradient heavy ion acceleration tube (5), an electromagnetic velocity selector (13) consisting of a pair of front and rear permanent magnets and a pair of left and right parallel metal plates with equal and opposite charges and connected to the metal strip (7), a single-charge heavy ion output / input channel (7’) vertically upward with a regular octagonal or regular decagonal cross-section and composed of energized guiding coils and connected to the upper end of the electromagnetic velocity selector (13), and an un-ionized heavy atom return channel (1’, 1”) consisting of a high-temperature resistant plastic tube with a gas compressor (1’) at the end and in the same straight line as the gradient heavy ion acceleration tube (5), and another high-temperature resistant plastic tube on the right side of the left end of the high-temperature resistant plastic tube with the gas compressor (1’) and connected to it, with a high-pressure gas compressor (1”) at the end, and the left end of the other high-temperature resistant plastic tube with the high-pressure gas compressor (1”) fixed on the left side of the high-temperature atomic furnace (1). The end of the single-charge heavy ion output / input channel (7’) is connected to the entrance of the first high-charge heavy ion electrostatic separation region (F1) or the first high-charge heavy ion static magnetic separation region (F1’) at the left end in the flat racetrack-shaped high-speed multi-faceted side-by-side opposed electron beam transverse collision high-charge heavy ion ionization ring (B). The outer surface of the gradient heavy ion acceleration tube (5) is sleeved with an energized guiding coil (5’) with a regular octagonal or regular decagonal cross-section.

[0013] The low-speed multi-faceted side-by-side opposed electron flow transverse collision single-charge heavy atom injection section (A) of the low-speed multi-faceted side-by-side opposed electron flow transverse collision single-ionization region (a) is composed of 6-10 identical single-ionization surface electron flow emitters and 5-9 identical first energized guiding coils (a”’) arranged side by side in series at intervals. The single-ionization surface electron flow emitter is composed of a first upper emission cavity (a’) with four or five mutually equidistant and intersecting sides and a first lower emission cavity (a”) that is axially symmetrically distributed in the same plane as the first upper emission cavity (a’). The center of 6-10 identical single-ionization surface electron flow emitters and 5-9 identical first energized guiding coils (a”’) arranged side by side in series with it constitutes the drift orbit of the single-ionization heavy atom. Both the first upper emission cavity (a’) and the first lower emission cavity (a”) are composed of a first energized hot cathode (8.1) made of a flat rectangular tungsten sheet with a width slightly larger than the width of the furnace mouth (2) and a length 3-5 times the width of the furnace mouth (2), coated with Ba0 material on the surface, and located on the upper or lower side of the neutral heavy atom beam (3) directly in front of the furnace mouth (2). It is also composed of a first flat rectangular metal frame (11.1) made of copper pipe, silver pipe, or gold pipe, with an area slightly larger than that of the first energized hot cathode (8.1), and 50-100 of them are connected in series with the second high resistance (12.2) at intervals. The outside of the first flat rectangular metal frame (11.1) is wrapped with a layer of insulating film. Each of the four corners of the first flat rectangular metal frame (11.1) is penetrated by a slender cylindrical insulating rod (11.1’) for fixing the first energized hot cathode (8.1) and the first flat rectangular metal frame (11.1). The upper or lower end of the insulating rod (11.1’) has three notches. The uppermost or lowermost notch can just hold the first energized hot cathode (8.1), and the two notches close to the first energized hot cathode (8.1) can just hold two flat rectangular copper plates with the same length and width as the first energized hot cathode (8.1) and parallel to it. Dielectric is filled between the two flat rectangular copper plates, between the flat rectangular copper plates and the first energized hot cathode (8.1). The slender cylindrical second high resistance (12.2) rod passes through the small round hole in the middle of the short side of the first flat rectangular metal frame (11.1), and the slender cylindrical second high resistance (12.2) rod is in close contact with the first flat rectangular metal frame (11.1). The first flat rectangular metal frames (11.1) are parallel to each other and equally spaced. There is a wire connection between a flat rectangular copper plate close to the first energized hot cathode (8.1) and the first energized hot cathode (8.1). In the middle of a flat rectangular copper plate far from the first energized hot cathode (8.1), or in the middle of a flat rectangular copper plate close to the first energized hot cathode (8.1), a single-pole double-throw switch K is connected 12 or K 22 , the single-pole double-throw switch K 12 or K 22A flat rectangular copper plate far from the first energized hot cathode (8.1) or a flat rectangular copper plate near the first energized hot cathode (8.1) and a high-voltage power supply Ea 41 or Ea 42 are connected to the positive or negative pole. A supercapacitor Ca1 or Ca2 with an extremely large capacitance is connected in parallel at one end of the two flat rectangular copper plates. Between the flat rectangular copper plate near the first energized hot cathode (8.1) and the ground, through a grounding switch K 11 or K 12 they are connected. A first energized guiding coil (a''') is sleeved outside the single-charge heavy ion beam between each first upper emission cavity (a') and each first lower emission cavity (a''). The ratio of the width of the first energized guiding coil (a''') to the width of the first upper emission cavity (a') or the first lower reflection cavity (a'') is 1:2 - 1:4. The voltage applied across the two ends of the first upper emission cavity (a') is slightly greater than the single ionization voltage of heavy atoms measured experimentally or obtained through theoretical calculation, and the direction is downward. The voltage applied across the two ends of the first lower emission cavity (a'') is equal in magnitude and opposite in direction to the voltage applied across the two ends of the first upper emission cavity (a'). A first flat rectangular energized guiding coil (10.1) and a second flat rectangular energized guiding coil (10.2) with a cross-section slightly larger than that of the first upper emission cavity (a') and the first lower emission cavity (a'') are sleeved outside each first upper emission cavity (a') and first lower emission cavity (a''). A layer of thin iron sheet is wrapped on the outer surfaces of the first flat rectangular energized guiding coil (10.1) and the second flat rectangular energized guiding coil (10.2). A cylindrical and slender copper wire mesh (33) with a small amount of positive charge is also installed between each first upper emission cavity (a') or first lower emission cavity (a'') and the single-charge heavy ion beam (4).

[0014] The flat track-shaped high-speed multi-faceted side-by-side counter-propagating electron beam transverse collision high-charge heavy ion ionization ring (B) is composed of a first high-speed multi-faceted side-by-side counter-propagating electron beam transverse repeated collision multi-ionization region (b1), a first high-charge heavy ion electrostatic separation region (F1) or a first high-charge heavy ion magnetostatic separation region (F1'), a second high-speed multi-faceted side-by-side counter-propagating electron beam transverse repeated collision multi-ionization region (b2) and a second high-charge heavy ion electrostatic separation region (F2) or a second high-charge heavy ion magneto-electrostatic separation region (F2') connected in series in sequence to form a flat track and field-shaped loop. The first high-speed multi-faceted side-by-side counter-propagating electron beam transverse collision multi-ionization region (b1) is located on the left side of the flat track and field-shaped loop, and the second high-speed multi-faceted side-by-side counter-propagating electron beam transverse repeated collision multi-ionization region (b2) is located on the right side of the flat track and field-shaped loop.

[0015] The structures of the first high-speed multi-faceted side-by-side counter-propagating electron beam transverse collision multi-ionization region (b1) and the second high-speed multi-faceted side-by-side counter-propagating electron beam transverse repeated collision multi-ionization region (b2) are exactly the same. They are both composed of 16 - 30 identical multi-ionization surface electron beam emitters and 15 - 29 identical fourth energized guiding coils (b”’) arranged side by side in series. The structures of the multi-ionization surface electron beam emitter and the single-ionization surface electron beam emitter are also exactly the same. Only the voltages applied across the second upper emission cavity (b’) and the second lower emission cavity (b”) are slightly greater than the specific voltage required to make the ionization degree of heavy atoms μ, which needs to be measured experimentally or calculated theoretically. This specific voltage is much, much larger than the single-ionization voltage applied across the first upper emission cavity (a’) and the first lower emission cavity (a”).

[0016] The first high-charge heavy-ion electrostatic separation region (F1) consists of a first through electromagnetic focusing coil (15.1) with a regular octagon or decagon at the left end, a narrow rectangle with its long side perpendicular to the horizontal plane at the right end, and the left end connected to the front-end outlet of the first high-speed multi-faceted side-by-side counter-propagating electron beam transverse repeated collision multi-ionization region (b1). A first quarter-circular energized guiding coil (20.1) connected to the right-end outlet of the first through electromagnetic focusing coil (15.1). A first high-charge heavy-ion electrostatic separator (f1) with its front-side outlet connected to the inlet end of the first high-charge heavy-ion beam output / input channel (21.1) at the left end, connected to the right-end outlet of the first quarter-circular energized guiding coil (20.1), and its right-end outlet connected to the second quarter-circular energized guiding coil (20.2). An energized guiding coil with a straight left end and a second quarter-circular energized guiding coil (20.2) at the right end, connected to the first high-charge heavy-ion electrostatic separator (f1), and a first through electromagnetic diffusion coil (15.2) with a narrow rectangle at the inlet and a regular octagon or decagon at the outlet, connected to the rear-end of the second quarter-circular energized guiding coil (20.2) and to the front-end inlet of the second high-speed multi-faceted side-by-side counter-propagating electron beam transverse repeated collision multi-ionization region (b2), are connected in series successively. The second high-charge heavy-ion electrostatic separation region (F2) consists of a third through electromagnetic focusing coil (15.3) with a regular octagon or decagon at the front end, a narrow rectangle with its long side perpendicular to the horizontal plane at the rear end, and the front end connected to the rear-end outlet of the first high-speed multi-faceted side-by-side counter-propagating electron beam transverse repeated collision multi-ionization region (b1). A third quarter-circular energized guiding coil (20.3) connected to the rear-end outlet of the third through electromagnetic focusing coil (15.3). A second high-charge heavy-ion electrostatic separator (f2) with its rear-side outlet connected to the inlet of the second high-charge heavy-ion beam output / input channel (21.2), connected to the third quarter-circular energized guiding coil (20.3). An energized guiding coil with a straight right end and a fourth quarter-circular energized guiding coil (20.4) at the left end, connected to the second high-charge heavy-ion electrostatic separator (f2), and a second through electromagnetic diffusion coil (15.4) with a narrow rectangle at the inlet and a regular octagon or decagon at the outlet, connected to the rear-end of the fourth quarter-circular energized guiding coil (20.4) and to the rear-end inlet of the second high-speed multi-faceted side-by-side counter-propagating electron beam transverse repeated collision multi-ionization region (b2), are connected in series successively.

[0017] The first high-charge heavy-ion electrostatic separator (f1) is composed of four pairs of adjacent parallel metal plates perpendicular to the horizontal plane, with equal but opposite charges. The rear plates of the first pair on the left are positively charged and the front plates are negatively charged. The rear plates of the second and third pairs in the middle are negatively charged and the front plates are positively charged. The rear plates of the fourth pair at the back are positively charged and the front plates are negatively charged. The two plates of the first and fourth pairs are closer to each other, the two plates of the second pair are farther apart, and the distance between the two plates of the third pair is between that of the first and fourth pairs. The front exit of the electrostatic charge separator is connected to the entrance of the fifth quarter-circular energized guiding coil (20.5) at the lower end of the first high-charge heavy-ion beam output / input channel (21.1). The second high-charge heavy-ion electrostatic separator (f2) is composed of four pairs of adjacent parallel metal plates perpendicular to the horizontal plane, with equal but opposite charges. The right plates of the first pair at the back are positively charged and the left plates are negatively charged. The right plates of the second and third pairs in the middle are negatively charged and the left plates are positively charged. The right plates of the fourth pair at the front are positively charged and the left plates are negatively charged. The two plates of the first and fourth pairs are closer to each other, the two plates of the second pair are farther apart, and the distance between the two plates of the third pair is between that of the first and fourth pairs. The front exit of the electrostatic charge separator is connected to the entrance of the seventh quarter-circular energized guiding coil (20.7) at the lower end of the second high-charge heavy-ion beam output / input channel (21.2).

[0018] The first high-charge heavy-ion magnetostatic and electrostatic separation region (F1’) is successively formed by connecting in series a first through electromagnetic focusing coil (15.1) with a narrow rectangular front end having a long side perpendicular to the horizontal plane and a rear end in the shape of a regular octagon or decagon, and the rear end being connected to the front-end outlet of the first high-speed multi-faceted side-by-side counter-propagating electron flow transverse multi-ionization region (b1); a pair of upper and lower opposed first trapezoidal magnets (25.1) connected to the front-end outlet of the first through electromagnetic focusing coil (15.1); and a second quarter-circular energized guiding coil (15.2) with its left side connected to the right side of the first trapezoidal magnet (25.1) and its right side connected to the front-end inlet of the second high-speed multi-faceted side-by-side counter-propagating electron flow transverse multi-ionization region (b2). The rear-side outlet on the right of the first trapezoidal magnet (25.1) is connected to the inlet of the fifth quarter-circular energized guiding coil (20.5) at the lower end of the first high-charge heavy-ion beam output / input channel (21.1). The second high-charge heavy-ion magnetostatic and electrostatic separation region (F2’) is successively formed by connecting in series a second through electromagnetic focusing coil (15.3) with a narrow rectangular rear end having a long side perpendicular to the horizontal plane and a front end in the shape of a regular octagon, and the front end being connected to the rear-end outlet of the first high-speed multi-faceted side-by-side counter-propagating electron flow transverse multi-ionization region (b1); a pair of upper and lower opposed second trapezoidal magnets (25.2) connected to the rear-end outlet of the second through electromagnetic focusing coil (15.3); and a fourth quarter-circular energized guiding coil (15.4) with its right side connected to the left side of the first trapezoidal magnet (25.1) and its left side connected to the rear-end inlet of the first high-speed multi-faceted side-by-side counter-propagating electron flow transverse multi-ionization region (b1). The front-side outlet on the left of the second trapezoidal magnet (25.2) is connected to the inlet of the seventh quarter-circular energized guiding coil (20.7) at the lower end of the second high-charge heavy-ion beam output / input channel (21.2).

[0019] The first high-charge heavy-ion beam output / input channel (21.1) is an energized guiding coil with the same cross-section as the flat rectangular cross-section at the exit of the first energized guiding magnetic focusing coil (15.1). The entrance and exit ends of the first high-charge heavy-ion beam output / input channel (21.1) are both quarter-circular arcs, but the bending directions of the two are opposite. The section between the fifth quarter-circular energized guiding coil (20.5) at the entrance end and the fourth quarter-circular energized guiding coil (20.4) at the exit end is a straight energized guiding coil. The sixth quarter-circular coil (20.6) at the exit end of the first high-charge heavy-ion beam output / input channel (21.1) can just be inserted into the entrance of the third energized guiding coil (19.2) in the flat-racetrack-shaped high-speed multi-faceted side-by-side counter-propagating electron beam transverse collision high-charge heavy-ion excitation ring (D). The second high-charge heavy-ion beam output / input channel (21..2) has the same structure as the first high-charge heavy-ion beam output / input channel (21.1). The eighth quarter-circular coil (20.8) at the exit end of the second high-charge heavy-ion beam output / input channel (21.2) can just be inserted into the entrance of the seventh energized guiding coil (19.4) in the flat-racetrack-shaped high-speed multi-faceted side-by-side counter-propagating electron beam transverse collision high-charge heavy-ion excitation ring (D).

[0020] The flat-racetrack-shaped high-speed multi-faceted side-by-side counter-propagating electron beam transverse collision high-charge heavy-ion excitation ring (D) is a flat track-and-field-shaped loop formed by successively connecting in series a first high-speed multi-faceted side-by-side counter-propagating electron beam transverse repeated collision excitation region (d1), a first high-charge heavy-ion receiving region (G1), a second high-speed multi-faceted side-by-side counter-propagating electron beam transverse repeated collision excitation region (b2), and a second high-charge heavy-ion receiving region (G2). The center of the flat track-and-field-shaped loop is the drift orbit of heavy ions with an ionization degree of μ. The center of the first high-speed multi-faceted side-by-side counter-propagating electron beam transverse collision excitation region (d1) on the right side of the flat track-and-field-shaped loop is the first high-charge heavy-ion horizontal drift straight track (23). The center of the second high-speed multi-faceted side-by-side counter-propagating electron beam transverse collision excitation region (d2) on the left side of the flat track-and-field-shaped loop is the second high-charge heavy-ion horizontal drift straight track (23’). There is an optical resonant cavity composed of a semi-reflecting mirror (34) and a total-reflecting lens (35) on the extension lines before and after the first high-charge heavy-ion horizontal drift straight track (23) and the second high-charge heavy-ion horizontal drift straight track (23’). The upper ends of the two high-charge heavy-ion beam output / input channels (21.1, 21.2) before and after the flat-racetrack-shaped high-speed multi-faceted side-by-side counter-propagating electron beam transverse collision high-charge heavy-ion excitation ring (D) are respectively connected to the entrance of the third energized guiding coil (19.2) in front of the flat-racetrack-shaped high-speed multi-faceted side-by-side counter-propagating electron beam transverse collision high-charge heavy-ion excitation ring (D) and the entrance of the seventh energized guiding coil (19.4) behind it.

[0021] The structures of the first high-speed multi-faceted side-by-side counter-propagating electron beam transverse collision excitation region (d1) and the second high-speed multi-faceted side-by-side counter-propagating electron beam transverse repeated collision excitation region (d2) are exactly the same. Both are formed by 16 - 30 identical excitation surface electron beam emitters and 15 - 29 identical fifth energized guiding coils (d''') arranged side by side in series. The structures of the excitation surface electron beam emitter and the single ionization surface electron beam emitter are also exactly the same. Only the voltages applied across the two ends of the third upper emission cavity (d') and the third lower emission cavity (d'') are slightly greater than the specific voltage required to excite heavy ions with an ionization degree of μ to a certain laser energy level, which is determined by experiment or theoretical calculation. This specific voltage is much, much larger than the single ionization voltage applied across the two ends of the first upper emission cavity (a') and the first lower emission cavity (a''). The numbers of the excitation surface electron beam emitter and the fifth energized guiding coil (d''') are also much larger than those of the single ionization surface electron beam emitter and the first energized guiding coil (a''').

[0022] On the outer edge of each fifth energized guiding coil (d''') on the second high-charge heavy ion horizontal drift straight track (23') on the left side, there is a copper ring (30) sleeved. Each copper ring (30) is successively connected to the intermediate connections of a circuit formed by 16 - 30 eighth high resistors (12.8) connected in series. A high voltage (E is applied across the two ends of the circuit formed by 16 - 30 eighth high resistors (12.8) connected in series. d5) At the front wall of the excitation box (39) on the extension line in front of the first high-charge heavy-ion horizontal drift straight track (23) on the right and the second high-charge heavy-ion horizontal drift straight track (23') on the left, there is a laser emission window respectively. The two laser emission windows are connected to a double-fiber converging tube (29') that can converge two high-energy laser beams (29) emitted from the two laser emission windows into one high-energy laser beam (29). A collimator (29'') is fixed under the double-fiber converging tube (29'). The double-fiber converging tube (29') and the collimator (29'') can rotate up, down, left and right through a control device outside the box. At the middle of the two laser emission windows on the front wall of the excitation box (39), at the place where the fast flying trajectory of high-speed and high-charge heavy ions passes through, there is also a high-charge heavy-ion emission window. The high-charge heavy-ion emission window is equipped with a special glass that can withstand high voltage and allow high-charge heavy ions to pass through. Outside the high-charge heavy-ion emission window, there is also an eighth energized guiding coil (17') that can be controllably bent up, down, left and right. The control device outside the box consists of brackets (36.1, 36.2, 36.3) fixed outside the front wall, a motor fixed at the rear end of the bracket bottom plate (36.1), a connecting rod (36.2) fixed at the middle end of the bracket bottom plate (36.1), with the upper end connected to the middle part of the double-fiber converging tube (29') and the lower gear meshing with the lower gear of the motor, a cylinder (36.3) fixed at the front end of the bracket bottom plate (36.1) that can rotate around the lower rotating shaft, a control rod (42) inserted in the cylinder (36.3) with the upper end connected to the front part of the double-fiber converging tube (29') through a rotating shaft, and a high-pressure gas transmission pipeline connecting the circular hole at the rear side of the cylinder (36.3) between the cylinder (36.3) and the control rod (42) to a high-pressure cylinder.

[0023] The first high-charge heavy-ion receiving area (G1) consists of a first square steering magnet (24.1), a second square steering magnet (24.2) located at the front ends of the first high-charge heavy-ion horizontal drift straight track (23) and the second high-charge heavy-ion horizontal drift straight track (23'), and a second energized guiding coil (19.1) with a cross-section of a regular octagon or a regular decagon, bent at both ends and with a small opening in the middle, and a third energized guiding coil (19.2) with a smaller right end and a larger left end sleeved outside the second energized guiding coil (19.1) with a small opening. There is an entrance at the front side of the left end of the third energized guiding coil (19.2). The end of the sixth quarter-circular coil (20.6) at the outlet end of the first high-charge heavy-ion beam output / input channel (21.1) can just be inserted into the entrance of the third energized guiding coil (19.2).

[0024] The second highest charge heavy ion acceptance region (G2) consists of a third square steering magnet (24.3), a fourth square steering magnet (24.4) located at the front ends of the first highest charge heavy ion horizontal drift linear orbit (23) and the second highest charge heavy ion horizontal drift linear orbit (23'), and a sixth energized guiding coil (19.3) with a small opening in the middle and both ends bent, whose cross-section is a regular octagon or a regular decagon between them, and a seventh energized guiding coil (19.4) with a small left end and a large right end sleeved outside the sixth energized guiding coil (19.3) with a small opening. There is an entrance at the rear side of the right end of the sixth energized guiding coil (19.3). The end of the eighth quarter-circular coil (20.8) at the outlet end of the second highest charge heavy ion beam output / input channel (21.2) can just be inserted into the entrance of the third energized guiding coil (19.2).

[0025] In the high-energy laser with high-charge heavy ions collided transversely by four-sided side-by-side counter-propagating surface electron beams, the number of surface electron beams is four, and the furnace opening (2) is a regular octagon. In the high-energy laser with high-charge heavy ions collided transversely by five-sided side-by-side counter-propagating surface electron beams, the number of surface electron beams is five, and the furnace opening (2) is a regular decagon.

[0026] The three large boxes, namely the flat cuboid large ionization box (38) located below and fixedly connected together, the flat cuboid large excitation box (39) located above, and the flat cuboid large accessory box (40) located below the flat cuboid large ionization box (38), can be installed together on a car, or an airplane, or a warship, or in a laboratory.

[0027] The beneficial effects of the present invention are as follows:

[0028] 1. A set of high-energy lasers that can generate higher-intensity high-speed multi-sided cross side-by-side counter-propagating surface electron beams and high-intensity high-charge heavy ion beams, and excite high-intensity high-charge heavy ion beams through the transverse back-and-forth collision of higher-intensity high-speed surface currents, to obtain high-charge heavy ions with higher intensity, higher monochromatic brightness, higher power, and shorter wavelength. The present invention overcomes the serious defects of current lasers, opens up a new way for the research and application of lasers, enables high-power emission devices to potentially become new high-energy laser weapons or the ignition light source for thermonuclear fusion devices, and enables small-power laser emission devices to potentially be made into the light source of an ultra-short wavelength laser microscope for observing the atomic structure and activities within organic molecules.

[0029] 2. Only ordinary small and simple electromechanical devices are used, without using large heavy ion sources and giant accelerators, and the conversion efficiency of electrical energy into light energy is very high. Description of the Drawings

[0030] Figure 1 Front view of the low-speed four-sided side-by-side counter-propagating surface electron beam transverse collision single-charge heavy ion injection section (A)

[0031] Figure 2 Top view of the low-speed four-sided side-by-side opposed electron beam transverse collision single-charge heavy ion injection section (A)

[0032] Figure 3 Side view of the low-speed four-sided side-by-side opposed electron beam transverse collision single-charge heavy ion injection section (A)

[0033] Figure 4 Front view of the flat racetrack-shaped high-speed four-sided side-by-side opposed electron beam transverse collision high-charge heavy ion ionization ring (B)

[0034] Figure 5 Top view of the flat racetrack-shaped high-speed four-sided side-by-side opposed electron beam transverse collision high-charge heavy ion ionization ring (B) (equipped with a high-charge heavy ion electrostatic separator)

[0035] Figure 6 Top view of the flat racetrack-shaped high-speed four-sided side-by-side opposed electron beam transverse collision high-charge heavy ion ionization ring (B) (equipped with a high-charge heavy ion static magnetic separator)

[0036] Figure 7 Side view of the flat racetrack-shaped high-speed four-sided side-by-side opposed electron beam transverse collision high-charge heavy ion ionization ring (B)

[0037] Figure 8 Front view of the flat racetrack-shaped high-speed four-sided side-by-side opposed electron beam transverse collision high-charge heavy ion excitation ring (D)

[0038] Figure 9 Top view of the flat racetrack-shaped high-speed four-sided side-by-side opposed electron beam transverse collision high-charge heavy ion excitation ring (D)

[0039] Figure 10 Side view of the flat racetrack-shaped high-speed four-sided side-by-side opposed electron beam transverse collision high-charge heavy ion excitation ring (D)

[0040] Figure 11 Side view of the flat racetrack-shaped high-speed four-sided side-by-side opposed electron beam transverse collision high-charge heavy ion ionization ring (B) and the flat racetrack-shaped high-speed four-sided side-by-side opposed electron beam transverse collision high-charge heavy ion excitation ring (D) overlapping each other

[0041] Figure 12 Side view of the four-sided side-by-side opposed flat cuboid large ionization ring (B), the four-sided side-by-side opposed flat cuboid large excitation ring (D), and the four-sided side-by-side opposed flat cuboid large accessory box (40) stacked on top of each other and installed on a vehicle

[0042] Figure 13Front view of the low-speed five-sided side-by-side opposed electron beam transverse collision single-charge heavy ion injection section (A)

[0043] Figure 14 Top view of the low-speed five-sided side-by-side opposed electron beam transverse collision single-charge heavy ion injection section (A)

[0044] Figure 15 Side view of the low-speed five-sided side-by-side opposed electron beam transverse collision single-charge heavy ion injection section (A)

[0045] Figure 16 Front view of the flat racetrack-shaped high-speed five-sided side-by-side opposed electron beam transverse collision high-charge heavy ion ionization ring (B)

[0046] Figure 17 Top view of the flat racetrack-shaped high-speed five-sided side-by-side opposed electron beam transverse collision high-charge heavy ion ionization ring (B) (equipped with a high-charge heavy ion electrostatic separator)

[0047] Figure 18 Top view of the flat racetrack-shaped high-speed five-sided side-by-side opposed electron beam transverse collision high-charge heavy ion ionization ring (B) (equipped with a high-charge heavy ion magnetostatic separator)

[0048] Figure 19 Side view of the flat racetrack-shaped high-speed five-sided side-by-side opposed electron beam transverse collision high-charge heavy ion ionization ring (B)

[0049] Figure 20 Front view of the flat racetrack-shaped high-speed five-sided side-by-side opposed electron beam transverse collision high-charge heavy ion excitation ring (D)

[0050] Figure 21 Top view of the flat racetrack-shaped high-speed five-sided side-by-side opposed electron beam transverse collision high-charge heavy ion excitation ring (D)

[0051] Figure 22 Side view of the flat racetrack-shaped high-speed five-sided side-by-side opposed electron beam transverse collision high-charge heavy ion excitation ring (D) Figures 23 - 25 Front view, top view and side view of the emission cavity

[0052] Figures 26 - 28 Front view, top view and side view of the high-charge heavy ion beam output / input channel (21.1)

[0053] Names of each serial number in the figure

[0054] 1 - High-temperature atomic furnace, 1' - Gas compressor at the inlet of the non-ionized heavy atom return channel, 1'' - High-pressure gas compressor (1'') at the outlet of the non-ionized heavy atom return channel, 2 - Regular octagonal or regular decagonal furnace opening of the high-temperature atomic furnace, 3 - Heavy atom beam, 4 - Singly charged heavy ion beam, 5 - Gradient heavy ion acceleration tube, 5' - Energized guiding coil sleeved outside the gradient heavy ion acceleration tube, 7 - Negatively charged metal strip on the left, 7' - Input / output channel of the singly charged heavy ion beam, 8 - Energized hot cathode made of tungsten sheet, 10,1, 10,2,... - First flat rectangular energized guiding coil, second flat rectangular energized guiding coil,..., 11,1, 11,2,... - First flat rectangular metal frame, second parallel flat rectangular metal frame,..., 12.1 - First high resistance in the gradient ion acceleration tube, 12,2, 12,3,... - Second high resistance, third high resistance,... in the emission cavity, 13 - Electromagnetic velocity selector, 14 - Mixed heavy ion beam, 15 - Energized guiding and magnetic focusing coil, 17 - Highly charged heavy ion beam with ionization degree μ, 17' - Eighth energized guiding coil, 18 - Insulating plate, a''' - First energized guiding coil, 19.1 - Second energized guiding coil 19.2 - Third energized guiding coil, b''' - Fourth energized guiding coil, d''' - Fifth energized guiding coil, 19.3 - Sixth energized guiding coil, 19.4 - Seventh energized guiding coil, 20 - Quarter-circular energized guiding coil, 21.1 - First input / output channel of the highly charged heavy ion beam, 21.2 - Second input / output channel of the highly charged heavy ion beam., 23 - First horizontal drift straight track of the highly charged heavy ion beam, 23' - Second horizontal drift straight track of the highly charged heavy ion beam, 24 - Square magnet, 25 - Trapezoidal magnet, 29 - High-energy laser beam, 29' - Double fiber optic converging tube, 29'' - Aiming device, 30 - Copper ring, 33 - Tubular fine copper wire mesh with a little positive charge, 34 - Total reflection mirror, 35 - Semi-reflective lens, 36 - Toothed steel strip fixed on the bottom plate, 38 - Flat cuboid large ionization box, 39 - Flat cuboid large excitation box, 40 - Flat cuboid large accessory box, 41 - Automobile chassis, 41' - Automobile carriage floor, 42 - Hydraulic telescopic rod, 43 - Rotating shaft fixed at the upper rear corner of the flat cuboid large ionization box (38), 43' - Bearing fixed at the lower rear corner of the flat cuboid large excitation box (39), 44 - Circular turntable installed on the outer bottom surface of the flat cuboid large accessory box (40), 45 - Two semi-circular card slots with gears engraved on the automobile carriage floor (41'), 46 - Motor installed at the lower rear corner of the middle bottom surface of the flat cuboid large accessory box (40), 47 - Transmission gear on the motor.

[0055] A - Low - speed two - side side - by - side surface electron flow transverse back - and - forth collision single - charge heavy ion beam injection section, B - Flat - racetrack - shaped high - speed two - side side - by - side surface electron flow transverse back - and - forth collision high - charge heavy ion ionization ring, D - Flat - racetrack - shaped high - speed two - side side - by - side surface electron flow transverse back - and - forth collision high - charge heavy ion excitation ring, a - Low - speed two - side side - by - side surface electron flow transverse back - and - forth collision single - ionization region, a’ - The first upper emission cavity in (a), a” - The first lower emission cavity in (a), b - High - speed two - side side - by - side surface electron flow transverse back - and - forth collision multi - ionization region, b’ - The second upper emission cavity in (b), b” - The second lower emission cavity in (b), d - High - speed two - side side - by - side surface electron flow transverse back - and - forth collision excitation region, d’ - The third upper emission cavity in (d), d” - The third lower emission cavity in (d), Ca, Cb, Cd - Ultra - large - capacity supercapacitors, Ea, Eb, Ed - Power supplies. Detailed implementation mode

[0056] The technical solution of the present invention will be further described in combination with the above - mentioned drawings:

[0057] Figures 1 - 3It is a structural diagram of the injection section (A) of a low-speed four-sided side-by-side counter-propagating electron flow for transverse back-and-forth collision of a single-charge ion beam. The high-temperature atomic furnace (1) of the high-frequency induction heating circuit installed on the left side of the injection section (A) of the low-speed four-sided side-by-side counter-propagating electron flow for transverse back-and-forth collision of a single-charge heavy ion beam melts and vaporizes the heavy-atom metal or non-metal laser material, or heats the heavy-atom gas laser material, turning it into a high-temperature single-atom gas. The high-temperature single-atom gas jets out from the regular octagon furnace opening (2) to form a high-intensity heavy-atom beam (3) with a regular octagon cross-section. After the high-intensity heavy-atom beam (3) enters the low-speed four-sided side-by-side counter-propagating electron flow transverse back-and-forth collision single-ionization region (a) where the voltage is slightly higher than the atomic ionization potential, most of it will be ionized to form a high-intensity single-charge heavy ion beam (4), and then enters a gradient acceleration tube (5) with a cross-section slightly larger than the furnace opening area. After acceleration, it obtains a certain kinetic energy. In order to inject the accelerated single-charge heavy ion beam (4) into the flat-race-track-shaped high-speed four-sided side-by-side counter-propagating electron flow transverse collision high-charge heavy ion ionization ring (B) without affecting the ion orbits in the original flat-race-track-shaped high-speed four-sided side-by-side counter-propagating electron flow transverse collision high-charge ion ionization ring (B), a negatively charged upward-bent metal strip (7) is added on the left side of the single-charge heavy ion beam (4). The negatively charged upward-bent metal strip (7) on the left side exerts an attractive force to the left on the single-charge heavy ion beam (4). Under the action of this attractive force, after the single-charge heavy ion (4) turns, it can just enter the vertically upward electromagnetic velocity selector (13). Only the heavy ions with a velocity V = E / B can pass through the electromagnetic velocity selector (13). After the single-charge heavy ion (4) passes through the electromagnetic velocity selector (13), it enters the second high-charge heavy ion electrostatic separation region (F2) or the second high-charge heavy ion static magneto-electric separation region (F2’) in the flat-race-track-shaped high-speed three-sided side-by-side counter-propagating electron flow transverse collision high-charge heavy ion ionization ring (B) through the single-charge heavy ion beam input / output channel (7’).

[0058] After the high-intensity heavy-atom beam (3) passes through the low-speed four-sided side-by-side counter-propagating electron flow transverse collision single-ionization region (a), the un-ionized heavy atoms are not affected by the electric field force and will continue to move forward along the original straight line direction. Subsequently, they enter the un-ionized heavy atom return channel (1’, 1”) with a gas compressor (1’) installed at the entrance. Under the action of the high-pressure gas compressor (1”) installed at its exit, they are pressed back into the high-temperature atomic furnace (1).

[0059] The low-speed four-sided side-by-side opposed electron flow transverse collision single-charge heavy ion beam injection section (A). The low-speed four-sided side-by-side opposed electron flow transverse collision single ionization region (a) is composed of 6-10 identical single ionization surface electron flow emitters and 5-9 identical first energized guiding coils (a''') arranged side by side in series at intervals. The single ionization surface electron flow emitter is composed of a first upper emission cavity (a') where four sides intersect at equal intervals and a first lower emission cavity (a'') that is axially symmetrically distributed on the same plane as the first upper emission cavity (a'). The space surrounded by 6-10 identical single ionization surface electron flow emitters and 5-9 identical first energized guiding coils (a''') arranged side by side in series with them is filled with a magnetic field, forming a drift orbit for columnar single ionization heavy ions. The magnetic force generated by the magnetic field on the single-charge heavy ions can make the single-charge heavy ions move along the magnetic force lines, greatly reducing the diffusion of the single-charge heavy ion beam and greatly increasing the intensity of the single-charge heavy ion beam (4). A first flat rectangular energized guiding coil (10.1) with a cross-section slightly larger than that of the first upper emission cavity (a') is sleeved outside each first upper emission cavity (a'), and a second flat rectangular energized guiding coil (10.2) with a cross-section slightly larger than that of each first lower emission cavity (a'') is also sleeved outside each first lower emission cavity (a''). The magnetic fields generated by the first flat rectangular energized guiding coil (10.1) and the second flat rectangular energized guiding coil (10.2) can greatly reduce the diffusion of the surface electron flow and greatly increase the intensity of the surface electron flow. A layer of thin iron sheet wrapped on the outer surfaces of the first flat rectangular energized guiding coil (10.1) and the second flat rectangular energized guiding coil (10.2) can play a role in magnetic shielding for the first flat rectangular energized guiding coil (10.1) and the second flat rectangular energized guiding coil (10.2), and can reduce the influence of the magnetic fields generated by the first flat rectangular energized guiding coil (10.1) and the second flat rectangular energized guiding coil (10.2) on the magnetic field generated by the first energized guiding coil (a''').

[0060] In the middle of a parallel narrow and long copper plate far from the first energized hot cathode (8.1) of the first upper emission cavity (a') or the first lower emission cavity (a''), a single-pole double-throw switch K12 or K22 is connected.

[0061] The side-by-side opposed electron flow is emitted from these first upper emission cavities (a') and first lower emission cavities (a'') that are arranged side by side and axially symmetrically distributed on the same plane.

[0062] After the power supply Ea1 of the first energized hot cathode (8.1) is turned on, electrons on the lower surface of the first energized hot cathode (8.1) escape from the lower surface of the first energized hot cathode (8.1) due to thermal excitation to form a surface electron current, and such a surface electron current can be called a "local surface electron current". After voltages Ea2 and Ea3 are applied to both ends of the first upper emission cavity (a') and the first lower emission cavity (a") simultaneously, the electrons in the escaped surface electron current will be accelerated to move downward or upward to form a locally counter-propagating surface electron current. The electrons in the accelerated local surface electron current, after colliding with the heavy atoms (3), can just knock off an outer electron, making the heavy atoms (3) carry a positive charge and become a single-charge heavy ion (4). The electrons that collide with the heavy atoms (3) will have almost all of their kinetic energy converted into the electrical energy of the single-charge heavy ions (4), become electrons moving at low speeds, and together with the knocked-off outer electrons, are absorbed by the slightly positively charged tubular fine copper wire mesh (33) surrounding the single-charge heavy ions (4). The electrons that do not collide with the heavy atoms (3) will be decelerated to nearly zero under the reverse voltage of the first lower emission cavity (a") or the first upper emission cavity (a') and then absorbed by the first energized hot cathode (8.1) of the first lower emission cavity (a") or the first upper emission cavity (a). After being absorbed, they escape from the lower surface of the first energized hot cathode (8.1) again due to thermal excitation to form a reverse surface electron current, and collide with the heavy atom (3) beam again until they collide with the heavy atoms (3), become electrons moving at low speeds, and are absorbed by the first energized hot cathode (8.1) of the first lower emission cavity (a") or the first upper emission cavity (a). After the power supply Ea1 of the first energized hot cathode (8.1) is turned on, the above process of the locally counter-propagating surface electron current will continue continuously.

[0063] If, after the power supply Ea1 of the first energized hot cathode (8.1) is turned on, the single-pole double-throw switch K 21 and K 22While simultaneously connecting the negative electrodes of power supplies Ea41 and Ea42, the upper and lower surfaces of a parallel narrow and long copper plate of the first energized hot cathode (8.1) far from the first upper emission cavity (a') and / or the first lower emission cavity (a") and the upper and lower surfaces of the upper plates of ultra-large-capacity supercapacitors Ca1 and Ca2 connected in parallel with it are all negatively charged (-Q). The upper and lower surfaces will each carry a negative charge (-Q / 2). The upper or lower surface of a parallel narrow and long copper plate of the first energized hot cathode (8.1) close to the first upper emission cavity (a') or the first lower emission cavity (a") and the lower or upper plate of the ultra-large-capacity supercapacitors Ca1 and Ca2 connected in parallel with it will carry a positive charge Q / 2 due to the induction of the negatively charged plate. The lower or upper surface of a parallel narrow and long copper plate of the first energized hot cathode (8.1) close to the first upper emission cavity (a') or the first lower emission cavity (a") and the lower or upper plate of the ultra-large-capacity supercapacitors Ca1 and Ca2 connected in parallel with it will carry a negative charge (-Q / 2) due to the induction of the negatively charged plate. Since the first energized hot cathode (8.1) is connected to a parallel narrow and long copper plate close to it, it will carry a part of the negative charge (-Q / 2). Therefore, the lower or upper surface of the two first energized hot cathodes (8.1) will induce a certain amount of negative charge when the single-pole double-throw switches K12 and K22 simultaneously connect the negative electrodes of power supplies Ea41 and Ea42. This induced part of the negative charge greatly increases the number of electrons that can be thermally excited and escape from the lower or upper surface of the two first energized hot cathodes (8.1). Since these electrons are also repelled by the negative charge -(-Q) on the upper and lower surfaces of a parallel narrow and long copper plate of the first energized hot cathode (8.1) far from the first upper emission cavity (a') or the first lower emission cavity (a"), they will escape from the surface or upper surface of the first energized hot cathode (8.1) faster, which greatly increases the intensity of the surface electron current emitted from the lower or surface of the two first energized hot cathodes (8.1). The surface electron current emitted from the lower surface of the first energized hot cathode (8.1) of the first upper emission cavity (a') moves downward, and the surface electron current emitted from the upper surface of the first energized hot cathode (8.1) of the first lower emission cavity (a") moves upward, and they form a simultaneous counter-propagating surface electron current. The simultaneous counter-propagating surface electron current increased due to induction can be called the induced surface electron current. The induced surface electron current is several times larger than the simultaneous counter-propagating local surface electron current formed without induction. It makes the probability of single ionization of heavy atoms several times larger, and the intensity of the single-ionized heavy ions that can be generated is also several times larger. The greater the electromotive force of power supplies Ea41 and Ea42 and the greater the capacitance of the ultra-large-capacity supercapacitors Ca1 and Ca2, the more charge Q can be stored, the greater the induced surface electron current that can be generated, and the greater the intensity of the single-ionized heavy ions.The total electric charge of the electrons that can escape from the lower surface of the first energized hot cathode (8.1), a parallel narrow and long copper plate close to the first energized hot cathode (8.1), and the lower plates of the ultra-large-capacity supercapacitors Ca1 and Ca2 connected in parallel with it due to the induction of the negatively charged plate is (-Q). These electrons with a total electric charge of (-Q) continuously escape and collide with the heavy atom (3) beam. After becoming low-speed moving electrons, they will be absorbed by the tubular fine copper wire mesh (33) with a little positive charge outside the single-charged heavy ion (4). The above process of the opposed induction surface electron flow will completely stop. At this time, the upper surfaces of the first energized hot cathode (8.1), a parallel narrow and long copper plate close to the first energized hot cathode (8.1), and the lower plates of the ultra-large-capacity supercapacitors Ca1 and Ca2 connected in parallel with it will carry an induced positive charge with a total electric charge of Q. These induced positive charges with a total electric charge of Q and the negative charge (-Q) on the lower surface of a parallel narrow and long copper plate of the first energized hot cathode (8.1) far from the first upper emission cavity (a') or the first lower emission cavity (a") and the lower surface of the upper plates of the ultra-large-capacity supercapacitors Ca1 and Ca2 connected in parallel with it maintain static balance.

[0064] Due to the large capacitance of the ultra-large-capacity supercapacitors Ca1 and Ca2, the amount of electric charge Q that can be stored is very large. Therefore, the process of the opposed induction surface electron flow will last for a quite long time. If it is necessary to carry out the process of the opposed induction surface electron flow again, the grounding switch K 11 and K 12 . Connect the grounding switch K 11 and K 12After that, the induced positive charge with a stored electric quantity of Q will attract electrons on the ground to enter. When the total electric quantity of the entering electrons reaches (-Q), the upper surfaces of the first energized hot cathode (8.1), a parallel narrow and long copper plate close to the first energized hot cathode (8.1), and the lower plates of the ultra-large-capacity supercapacitors Ca1 and Ca2 connected in parallel with it will carry a total electric quantity of Q / 2, and the lower surfaces of the first energized hot cathode (8.1), a parallel narrow and long copper plate close to the first energized hot cathode (8.1), and the lower plates of the ultra-large-capacity supercapacitors Ca1 and Ca2 connected in parallel with it will carry a total electric quantity of (-Q / 2), and the system reaches a quasi-electrostatic equilibrium state, and electrons on the ground will no longer enter. The electrons on the lower surfaces of the first energized hot cathode (8.1), a parallel narrow and long copper plate close to the first energized hot cathode (8.1), and the lower plates of the ultra-large-capacity supercapacitors Ca1 and Ca2 connected in parallel with it, under the repulsive force of the negative charges on the upper and lower surfaces of a parallel narrow and long copper plate of the first energized hot cathode (8.1) far from the first upper emission cavity (a') or the first lower emission cavity (a") with a total negative charge of (-Q) and the upper plates of the ultra-large-capacity supercapacitors Ca1 and Ca2 connected in parallel with it, continuously escape from the lower surface due to heat, forming a surface electron flow, and continuously colliding with heavy atoms to singly ionize them. Since the electrons on the lower surface continuously escape from the lower surface due to heat, the negative charge on the lower surface decreases, and the quasi-electrostatic equilibrium state is destroyed, and electrons on the ground will be continuously sucked in to maintain the quasi-electrostatic equilibrium state. If the grounding switch K 11 and K 12 are closed, the first upper emission cavity (a') and / or the first lower emission cavity (a") will continuously emit surface electron flows simultaneously and continuously collide with heavy atoms to singly ionize them. This continuously ongoing process is called the simultaneous counter-emission process.

[0065] When the single-pole double-throw switch K21 connects to the negative pole of the power supply Ea41 and the single-pole double-throw switch K22 connects to the positive pole of the power supply Ea42, due to the above reasons, the first upper emission cavity (a’) will emit surface electron flow to the first lower emission cavity (a”). When the grounding switches K11 and K12 are not connected, the total electric charge of the electrons that can be emitted is (-Q). However, the upper and lower surfaces of a parallel flat rectangular copper plate far from the first lower emission cavity (a”) and the upper and lower surfaces of the upper plates of the ultra-large-capacity supercapacitors Ca1 and Ca2 connected in parallel with it will each carry a positive charge of (Q / 2), and the upper and lower surfaces together carry a positive charge of Q. The lower surface of a parallel flat rectangular copper plate close to the first lower emission cavity (a”) and the first energized hot cathode (8.1) and the lower surfaces of the lower plates of the ultra-large-capacity supercapacitors Ca1 and Ca2 connected in parallel with it will carry a negative charge (-Q / 2) due to the induction of the positively charged plates. The upper surface of a parallel flat rectangular copper plate far from the first lower emission cavity (a”) and the first energized hot cathode (8.1) and the upper surface of the lower plate of the ultra-large-capacity supercapacitor Ca2 connected in parallel with it will carry an equal amount of positive charge Q / 2 due to the induction of the negatively charged plates. Since the first energized hot cathode (8.1) is connected to the upper surface of a parallel flat rectangular copper plate close to the first energized hot cathode (8.1), they will carry a part of the positive charge Q / 2. Therefore, a certain amount of positive charge will be induced on the upper surface of the first energized hot cathode (8.1) when the single-pole double-throw switch K22 connects to the positive pole of the power supply Ea42. Since the positive charge is induced on the upper surface of the first energized hot cathode (8.1), it will not emit induced surface electron flow to the first upper emission cavity (a’). However, it can absorb the induced surface electron flow with a total electric charge of (-Q) emitted from the first upper emission cavity (a’) to the first lower emission cavity (a”). Half of the absorbed induced surface electron flow neutralizes the positive charge Q / 2 on the upper surface of the first energized hot cathode (8.1), and the remaining (-Q / 2) and the induced negative charge (-Q / 2) already carried on the lower surface together carry a total induced negative charge of (-Q), while the upper and lower surfaces of a parallel flat rectangular copper plate far from the first lower emission cavity (a”) and the upper and lower surfaces of the upper plates of the ultra-large-capacity supercapacitors Ca1 and Ca2 connected in parallel with it carry a total positive charge of Q, reaching a quasi-electrostatic equilibrium state.

[0066] If, when just reaching the quasi-electrostatic equilibrium state, the single-pole double-throw switch K 21 connects to the positive pole of the power supply Ea 41 and the single-pole double-throw switch K 22 connects to the positive pole of the power supply Ea 42For the negative electrode, a process opposite to the above process will occur: the first lower emission cavity (a') will emit a surface electron flow towards the first upper emission cavity (a"), and it will be absorbed by the first upper emission cavity (a"). Single-pole double-throw switch K 21 and the single-pole double-throw switch K 22 In this way, the power supplies Ea 41 and the power supply Ea 42 are alternately connected to the negative and positive electrodes. The first upper emission cavity (a') and the first lower emission cavity (a") will continuously and alternately emit counter-propagating surface electron flows towards the symmetric first lower emission cavity (a') or the first upper emission cavity (a") until the power supply energy is exhausted. Such a counter-propagating process is called an alternating counter-propagating process.

[0067] This alternating counter-propagating process of alternately emitting counter-propagating surface electron flows can avoid occasional collisions of electrons in the counter-propagating surface electron flow at the same time, avoiding additional losses of the energy of the surface electron flow, but it will reduce the intensity of singly ionized heavy ions.

[0068] In the high-speed four-sided side-by-side counter-propagating surface electron flow transversely colliding with the singly ionized region (a), the single-pole double-throw switch K 21 or K22 can also be connected in the middle of a parallel flat rectangular copper plate of the first energized hot cathode (8.1) adjacent to the first upper emission cavity (a') or the first lower emission cavity (a"). Therefore, after connecting the power supply Ea1 of the first energized hot cathode (8.1), then use the single-pole double-throw switch K 21 and K 22 to simultaneously connect the power supplies Ea 41 and Ea 42The negative electrode, the upper and lower surfaces of the first energized hot cathode (8.1) and a parallel narrow and long copper plate of the first energized hot cathode (8.1) adjacent to the first upper emission cavity (a') or the first lower emission cavity (a"), and the upper and lower surfaces of the upper plates of the ultra-large-capacity supercapacitors Ca1 and Ca2 connected in parallel with it will carry a negative charge Q. The upper surface of a parallel flat rectangular copper plate far from the first upper emission cavity (a') or the first lower emission cavity (a") of the first energized hot cathode (8.1) and the upper plates of the ultra-large-capacity supercapacitors Ca1 and Ca2 connected in parallel with it will carry a negative charge (-Q / 2) due to the induction of the charged negative plate. The lower surface of a parallel narrow and long copper plate of the first energized hot cathode (8.1) adjacent to the first upper emission cavity (a') or the first lower emission cavity (a") and the lower plates of the ultra-large-capacity supercapacitors Ca1 and Ca2 connected in parallel with it will carry an equal amount of positive charge Q / 2 due to the induction of the charged negative plate. Since the first energized hot cathode (8.1) is connected to the lower surface of the adjacent parallel flat rectangular copper plate, they will carry a part of the negative charge Q. This increased part of the negative charge greatly increases the number of electrons that can be thermally excited and escape from the lower surface of the first energized hot cathode (8.1) on the lower surfaces of the two first energized hot cathodes (8.1), and greatly increases the surface electron current intensity emitted from the lower surfaces of the two first energized hot cathodes (8.1). This surface electron current can be called the "charged surface electron current". The charged surface electron current emitted from the lower surface of the first energized hot cathode (8.1) of the first upper emission cavity (a') is downward, and the charged surface electron current emitted from the upper surface of the first energized hot cathode (8.1) of the first lower emission cavity (a") is upward, and they form a simultaneous counter-propagating charged surface electron current. The simultaneous counter-propagating charged surface electron current increased due to charging is several times larger than the simultaneous counter-propagating local surface electron current formed without charging. It makes the probability of single ionization of heavy atoms several times larger, and the intensity of the single-ionized heavy ion beam that can be generated is also several times larger. The greater the electromotive force of the power supplies Ea41 and Ea42, and the greater the capacitance of the ultra-large-capacity supercapacitors Ca1 and Ca2, the greater the intensity of the single-ionized heavy ion beam that can be generated. As long as the power supplies Ea41 and Ea42 are not powered off, the above process of the simultaneous counter-propagating charged surface electron current will continue.

[0069] After turning on the power supply Ea1 of the first energized hot cathode (8.1) of the first upper emission cavity (a'), then use the single-pole double-throw switch K 12 Connect to the negative electrode of the power supply Ea41. After simultaneously turning on the power supply Ea1 of the first energized hot cathode (8.1) of the first upper emission cavity (a'), then simultaneously use the single-pole double-throw switch K 22 Connect to the power supply Ea of the first lower emission cavity (a") 42The upper surface and lower surface of the positive electrode, the first energized hot cathode (8.1) of the first upper emission cavity (a'), a parallel flat rectangular copper plate adjacent to the first energized hot cathode (8.1) of the first upper emission cavity (a'), and the upper surface and lower surface of the upper plate of the ultra-large-capacity supercapacitor Ca1 connected in parallel with it will carry negative charges (-Q). The upper surface of a parallel flat rectangular copper plate far from the first energized hot cathode (8.1) of the first upper emission cavity (a') or the first lower emission cavity (a") and the lower plate of the ultra-large-capacity supercapacitor Cal connected in parallel with it will carry negative charges (-Q / 2) due to the induction of the negatively charged plate. The lower surface of a parallel flat rectangular copper plate adjacent to the first energized hot cathode (8.1) of the first upper emission cavity (a') or the first lower emission cavity (a") and the lower plates of the ultra-large-capacity supercapacitors Cal and Ca2 connected in parallel with it will carry positive charges Q / 2 of equal amount due to the induction of the negatively charged plate. Since the first energized hot cathode (8.1) is connected to the lower surface of the adjacent parallel flat rectangular copper plate, they will carry a part of the negative charge Q. This increased part of the negative charge greatly increases the number of electrons that can be thermally excited and escape from the lower surface of the two first energized hot cathodes (8.1), and greatly increases the surface electron current intensity emitted from the lower surfaces of the two first energized hot cathodes (8.1). This surface electron current can be called the "charged surface electron current". The charged surface electron current emitted from the lower surface of the first energized hot cathode (8.1) of the first upper emission cavity (a') is downward.

[0070] Since the first lower emission cavity (a”) is connected to the positive pole of the power supply Ea42, the upper and lower surfaces of the first energized hot cathode (8.1) of the first lower emission cavity (a’) and a parallel flat rectangular copper plate adjacent to the first energized hot cathode (8.1) of the first lower emission cavity (a’), as well as the upper and lower surfaces of the upper plate of the ultra-large-capacity supercapacitor Ca2 connected in parallel with it, will carry a positive charge Q. The upper surface of a parallel flat rectangular copper plate far from the first energized hot cathode (8.1) of the first lower emission cavity (a”) and the lower plate of the ultra-large-capacity supercapacitor Ca2 connected in parallel with it will carry a positive charge Q / 2 due to the induction of the negatively charged plate. The lower surface of a parallel flat rectangular copper plate adjacent to the first energized hot cathode (8.1) of the first lower emission cavity (a”) and the lower plates of the ultra-large-capacity supercapacitors Ca1 and Ca2 connected in parallel with it will carry an equal amount (-Q / 2) due to the induction of the positively charged plate. Since the first energized hot cathode (8.1) is connected to the upper surface of the adjacent parallel flat rectangular copper plate, a part of the positive charge Q will be carried on the upper surface of the first energized hot cathode (8.1) of the first lower emission cavity (a”). Because the upper surface of the first energized hot cathode (8.1) of the first lower emission cavity (a”) carries a positive charge Q, it will not emit a charging surface electron flow. However, it can absorb the downward charging surface electron flow emitted from the lower surface of the first energized hot cathode (8.1) of the first upper emission cavity (a’) and neutralize it.

[0071] If the single-pole double-throw switch K 21 is used to connect to the positive pole of the power supply Ea41, and at the same time the single-pole double-throw switch K 22 is used to connect to the negative pole of the power supply Ea42 of the first lower emission cavity (a”), then the upper surface of the first energized hot cathode (8.1) of the first lower emission cavity (a”) will emit an upward charging surface electron flow, and the lower surface of the first energized hot cathode (8.1) of the first upper emission cavity (a’) will absorb the upward charging surface electron flow emitted from the upper surface of the first energized hot cathode (8.1) of the first lower emission cavity (a’) and neutralize it. In this way, by continuously and alternately connecting the positive and negative poles of the power supplies Ea41 and Ea42, the first upper emission cavity (a’) and the first lower emission cavity (a”) can alternately emit and oppose each other with charging surface electron flows. The alternately opposing charging surface electron flows can avoid the collision between electrons in the surface electron flow and avoid the energy loss caused by the collision and deflection of the surface electron flow. However, it reduces the total intensity of the surface electron flow and the intensity of single-ionized heavy ions. As long as the power supplies Ea41 and Ea42 are not powered off, the above process of alternately opposing charging surface electron flows will continue.

[0072] The gradient heavy ion acceleration tube (5) is formed by serially connecting 50 - 100 regular octagonal metal frames (11') with a cross-section slightly larger than that of the heavy ion beam (4) and each wrapped with an insulating film, and the second high resistor (12.2). A certain voltage is applied at both ends to form an accelerating electric field for heavy ions in the tube, so that the single-charge heavy ions (4) are accelerated after passing through the gradient ion acceleration tube (5), obtaining a certain speed and a certain kinetic energy. This speed cannot be too large to avoid an overly large deflection magnet, nor can it be too small to avoid excessive diffusion during transmission. An energized guiding coil (5') is sleeved on the outer wall of the gradient heavy ion acceleration tube (5). The magnetic field generated by the energized guiding coil (5') in the gradient heavy ion acceleration tube (5) can greatly reduce the diffusion of the single-charge heavy ions (4) and greatly increase the intensity of the single-charge heavy ion beam (4).

[0073] Figures 4 - 7 It is a structural diagram of a flat racetrack-shaped high-speed four-sided side-by-side opposing electron flow for transverse collision with a high-charge heavy ion ionization ring (B).

[0074] As can be seen from the figure, after the single-charge heavy ion beam (4) enters the second high-charge heavy ion electrostatic separation region (F2) or the second high-charge heavy ion magnetoelectrostatic separation region (F2') at the rear end of the flat racetrack-shaped high-speed four-sided side-by-side opposing electron flow for transverse back-and-forth collision with the high-charge ion ionization ring (B), it then enters the rear end of the first high-speed four-sided side-by-side opposing electron flow for transverse collision with the multi-ionization region (b1) on the left, exits from the front end, then enters the left entrance of the first high-charge heavy ion electrostatic separation region (F1) or the first high-charge heavy ion magnetoelectrostatic separation region (F1') at the front end, exits from the right exit, then enters the front entrance of the second high-speed multi-sided side-by-side opposing electron flow for transverse repeated collision with the multi-ionization region (b2) on the right, exits from the rear exit, and then enters the right entrance of the second high-charge heavy ion electrostatic separation region (F2) or the second high-charge heavy ion magnetoelectrostatic separation region (F2') at the rear end, forming a flat racetrack-shaped circular orbit.

[0075] The structures of the first high-speed multi-faceted side-by-side counter-propagating electron flow transverse collision multi-ionization region (b1) and the second high-speed multi-faceted side-by-side counter-propagating electron flow transverse repeated collision multi-ionization region (b2) are exactly the same. They are both composed of 16 - 30 identical multi-ionization surface electron flow emitters and 15 - 29 identical fourth energized guiding coils (b''') arranged side by side in series. The structures of the multi-ionization surface electron flow emitter and the single-ionization surface electron flow emitter are also exactly the same. Only the voltage applied across the second upper emission cavity (b') and the second lower emission cavity (b'') is slightly greater than the voltage required to make the ionization degree of heavy atoms μ, which can be measured experimentally or obtained through theoretical calculation. This voltage is much greater than the single-ionization voltage applied across the first upper emission cavity (a') and the first lower emission cavity (a''). The speed of the electrons in the high-speed surface electron flow emitted is also much greater than the speed of the electrons in the low-speed surface electron flow of the first upper emission cavity (a') and the first lower emission cavity (a'').

[0076] The high-speed surface electron flow emitted from the second upper emission cavity (b') and the second lower emission cavity (b'') collides transversely back and forth with the single-charge heavy ion beam (4), which can multi-charge ionize the single-charge heavy ion (4) again, turning the single-charge ion beam (4) into a mixed heavy ion beam (14) with different intensities and a higher ionization degree. Among them, there is a high-charge heavy ion beam (17) with an ionization degree of μ, and there are also low-charge heavy ion beams (22, 22',...) with a smaller ionization degree. A fourth energized guiding coil (b''') is sleeved outside the mixed heavy ion beam (14) between each second upper emission cavity (b') and each second lower emission cavity (b''). The flat racetrack-shaped annular columnar magnetic field space formed by the magnetic fields generated by all the fourth energized guiding coil tubes (b''') can greatly reduce the diffusion of the mixed heavy ion beam (14) and greatly improve the intensity of the mixed heavy ion beam (14). A third flat rectangular energized guiding coil (10.3) with a cross-section slightly larger than that of the first upper emission cavity (b') is sleeved outside each first upper emission cavity (b'), and a fourth flat rectangular energized guiding coil (10.4) with a cross-section slightly larger than that of the first reflection cavity (b'') is sleeved outside each first lower emission cavity (b''). The magnetic fields generated by the third flat rectangular energized guiding coil (10.3) and the fourth flat rectangular energized guiding coil (10.4) can greatly reduce the diffusion of the surface electron flow therein and greatly improve the intensity of the high-speed surface electron flow therein. A layer of thin iron sheet is wrapped on the outer surfaces of the third flat rectangular energized guiding coil (10.3) and the fourth flat rectangular energized guiding coil (10.4), and the thin iron sheet can reduce the influence of the magnetic fields generated by the third flat rectangular energized guiding coil (10.3) and the fourth flat rectangular energized guiding coil (10.4) on the magnetic field generated by the fourth energized guiding coil (b''').

[0077] The mixed heavy ion beam (14) exits from the first high-speed four-sided side-by-side counter-propagating electron beam transverse collision multi-ionization region (b1) and enters the first through electromagnetic focusing coil (15.1). Since the entrance of the first through electromagnetic focusing coil (15.1) is large and the exit is small, it has a focusing effect on the mixed heavy ion beam (14). After the mixed heavy ion beam (14) exits from the first through electromagnetic focusing coil (15.1), it becomes a ribbon-shaped mixed heavy ion beam (14) with a narrow rectangular cross-section whose long side is perpendicular to the horizontal plane. The ribbon-shaped mixed heavy ion beam (14) with a narrow rectangular cross-section then enters the first high-charge heavy ion electrostatic separator (f1) in the first high-charge heavy ion electrostatic separation region (F1). In the first high-charge heavy ion electrostatic separator (f1), since the high-charge heavy ions with an ionization degree of μ have the largest charge amount and the largest transverse deflection distance, they can fly out from the exit on the front side of the high-charge heavy ion separator and enter the entrance of the fifth quarter-circular energized guiding coil (20.5) at the lower end of the first high-charge heavy ion input / output channel (21), and enter the flat racetrack-shaped high-speed four-sided cross side-by-side electron beam transverse collision high-charge heavy ion excitation ring (D) through the exit of the sixth quarter-circular energized guiding coil (20.6) at the upper end of the first high-charge heavy ion input / output channel (21). The remaining low-charge heavy ion beams (22, 22',...) with smaller ionization degrees cannot fly out from the exit on the front side of the high-charge heavy ion separator due to their smaller charge amounts and smaller transverse deflection distances, but fly out from the right exit of the high-charge heavy ion separator and enter the second quarter-circular energized guiding coil (20.2) in front of it, and then enter the first through electromagnetic diffusion coil (15.2) through the second quarter-circular energized guiding coil (20.2). Through the diffusion effect of the first through electromagnetic diffusion coil (15.2), they become low-charge heavy ion beams (22, 22',...) with a regular octagon cross-section. The low-charge heavy ion beams (22, 22',...) with a regular octagon cross-section then enter the second high-speed four-sided side-by-side counter-propagating electron beam transverse collision multi-ionization region (b2). The low-charge heavy ion beams (22, 22',...) with smaller ionization degrees are re-ionized in the second high-speed four-sided side-by-side counter-propagating electron beam transverse collision multi-ionization region (b2) by the high-speed electrons emitted from the second upper emission cavity (b') and the second lower emission cavity (b"), increasing their ionization degree and becoming a new mixed heavy ion beam (14), which contains some new high-charge heavy ions (17) with an ionization degree of μ. The new mixed heavy ion beam (14) exits from the second high-speed four-sided side-by-side counter-propagating electron beam transverse collision multi-ionization region (b2) and enters the second through electromagnetic focusing coil (15.2). Since the entrance of the second through electromagnetic focusing coil (15.2) is large and the exit is small, it has a focusing effect on the new mixed heavy ion beam (14). The new mixed heavy ion beam (14) exits from the second through electromagnetic focusing coil (15.2) After coming out, it becomes a strip-shaped high-charge ion flow with a narrow rectangular cross-section whose long side is perpendicular to the horizontal plane. The strip-shaped high-charge ion flow with a narrow rectangular cross-section then enters the second high-charge heavy-ion separator (f2) in the second high-charge heavy-ion electrostatic separation zone (F2). In the second high-charge heavy-ion separator (f2), since the high-charge heavy ions with an ionization degree of μ have the largest charge amount and the largest lateral deflection distance, they can fly out from the outlet on the front side of the high-charge heavy-ion separator and enter the inlet of the seventh quarter-circular energized guiding coil (20.7) at the lower end of the second high-charge heavy-ion output / input channel (21'), and then enter the flat-raceway-shaped high-speed four-sided side-by-side counter-stream electron flow transverse collision high-charge heavy-ion excitation ring (D) through the outlet of the eighth quarter-energized guiding circular coil (20.8) at the upper end of the second high-charge heavy-ion output / input channel (21'). The other low-charge heavy-ion beams (22, 22',...) with smaller ionization degrees cannot fly out from the outlet on the front side of the high-charge heavy-ion separator because of their smaller charge amounts and smaller lateral deflection distances. Instead, they fly out from the left-end outlet of the high-charge heavy-ion separator and enter the fourth quarter-circular energized guiding coil (20.4) in front of it, and then enter the second electromagnetic diffusion coil (15.2) through the fourth quarter-circular energized guiding coil (20.4). Through the diffusion effect of the second electromagnetic diffusion coil (15.2), they become low-charge heavy-ion beams (22, 22',...) with a regular octagon cross-section. The low-charge heavy-ion beams (22, 22',...) with a regular octagon cross-section then enter the first high-speed four-sided side-by-side counter-stream electron flow transverse collision multi-ionization zone (b1) again for ionization, so that the number of high-charge heavy ions with an ionization degree of μ increases again. By continuously cycling like this, the number of high-charge heavy ions with an ionization degree of μ entering the flat-raceway-shaped high-speed four-sided side-by-side counter-stream electron flow transverse collision high-charge heavy-ion excitation ring (D) becomes more and more.

[0078] The first high-charge heavy-ion electrostatic separation region (F1) can also be replaced by the first high-charge heavy-ion magnetoelectrostatic separation region (F1'), and the second high-charge heavy-ion electrostatic separation region (F2) can also be replaced by the second high-charge heavy-ion magnetoelectrostatic separation region (F2'). That is, a pair of upper and lower opposed first trapezoidal magnets (25.1) and a pair of upper and lower opposed second trapezoidal magnets (25.2) are used to replace the first high-charge heavy-ion electrostatic separator (f1) and the second high-charge heavy-ion electrostatic separator (f2). Since the high-charge heavy ions with an ionization degree of μ have the largest charge amount and the smallest deflection radius in the magnetic field, they can fly out from the inner outlet of the first high-charge heavy-ion magnetostatic separator or the second high-charge heavy-ion magnetostatic separator and enter the seventh quarter-circular energized guiding coil (20.7) or the eighth quarter-circular energized guiding coil (20.8) at the lower end of the first high-charge heavy-ion output / input channel (21.1) or the second high-charge heavy-ion output / input channel (21.2), and then enter the flat-raceway-shaped high-speed four-sided side-by-side counter-propagating electron beam transverse collision high-charge heavy-ion excitation ring (D) from the outlet of the seventh quarter-circular energized guiding coil (20.7) or the eighth quarter-circular energized guiding coil (20.8).

[0079] The structure and the process of emitting the counter-propagating electron beam of the flat-raceway-shaped high-speed four-sided side-by-side counter-propagating electron beam that laterally collides back and forth with the high-charge heavy-ion ionization ring (B) to make the ionization degree of the heavy atom μ are the same as those of the flat-raceway-shaped low-speed four-sided side-by-side counter-propagating electron beam that laterally collides with the first upper emission cavity (a') and the first lower emission cavity (a") in the single-ionization region (a). The functions are also the same. Only the total width of the second upper emission cavity (b') and the second lower emission cavity (b") is much wider, and the voltages Eb2 and Eb3 applied at both ends are much larger, so that the ability to ionize heavy ions is much stronger.

[0080] The voltage required to be applied at both ends of the second upper emission cavity (b') and the second lower emission cavity (b") to generate high-charge heavy ions (17) with an ionization degree of μ needs to be accurately calculated theoretically, such as by using the fully relativistic multi-configuration self-consistent field method with Breit correction and QED correction, and can only be determined after experimental verification.

[0081] The above-mentioned first high-charge heavy ion separator (f1) is composed of four pairs of parallel metal plates with equal amounts of opposite charges. For the first pair and the fourth pair, the front plates are negatively charged and the rear plates are positively charged. For the second pair and the third pair, the front plates are positively charged and the rear plates are negatively charged. When the strip-shaped mixed heavy ion stream enters the space between the first pair of parallel metal plates at an appropriate speed along a straight track, it will be subject to a forward electric field force and move along a forward-curved parabolic track. After entering the space between the second pair and the third pair of parallel metal plates, it will be subject to a backward electric field force and move along a backward-curved parabolic track. After entering the space between the fourth pair of parallel metal plates, it will be subject to a forward electric field force again and move along a forward-curved parabolic track. When leaving the fourth pair of parallel metal plates, all ions return to the straight track when they first entered the space between the first pair of parallel metal plates while maintaining their original speed. Since there are heavy ions with different amounts of charge in the strip-shaped mixed heavy ion stream, the heavy ions with a larger charge amount will have a larger forward deviation displacement after entering the space between the second pair and the third pair of parallel metal plates, and the heavy ions with a smaller charge amount will have a smaller forward deviation displacement after entering the space between the second pair and the third pair of parallel metal plates. The high-charge heavy ions (17) with the largest charge amount and an ionization degree of μ will have the largest forward deviation displacement after entering the space between the second pair and the third pair of parallel metal plates. Therefore, they can fly out from the outlet between the third pair of parallel metal plates and the fourth pair of parallel metal plates and enter the inlet of the seventh quarter-circular energized guiding coil (20.7) at the lower end of the second high-charge heavy ion output / input channel (21’). Then, they enter the high-charge heavy ion excitation ring (D) of the flat-raceway-shaped high-speed four-sided side-by-side opposed electron beam transverse collision through the outlet of the eighth quarter-circular energized guiding coil (20.8) at the upper end of the second high-charge heavy ion output / input channel (21’). The remaining low-charge heavy ion beams (22, 22’,...) with a smaller ionization degree cannot fly out from the outlet on the front side of the high-charge heavy ion separator due to their smaller charge amount and smaller lateral deflection distance. Instead, they return to the straight track when they first entered the space between the first pair of parallel metal plates while maintaining their original speed.

[0082] Since the first high-charge heavy ion electrostatic separation region (F1), the second high-charge heavy ion electrostatic separation region (F2), the first high-charge heavy ion magneto-electrostatic separation region (F1’), and the second high-charge heavy ion magneto-electrostatic separation region (F2’) are all arranged at both ends of the flat-raceway-shaped high-speed four-sided side-by-side opposed electron beam transverse collision high-charge heavy ion ionization ring (B), replacing the previous large magnets, the weight of the flat-raceway-shaped high-speed four-sided side-by-side opposed electron beam transverse collision high-charge heavy ion ionization ring (B) is reduced. Moreover, it enables the low-charge return channel to be changed to the added second high-speed four-sided side-by-side opposed electron beam transverse collision multi-ionization region (b2). This not only replaces the low-charge return channel but also increases the intensity of the high-charge heavy ions (17) with an ionization degree of μ by 1.4 times compared to the previous situation (ZL 2018 2026 2863.x) where there was only the first high-speed four-sided side-by-side opposed electron beam transverse collision multi-ionization region (b1).

[0083] Figures 8 - 10 It is a structural diagram of a flat racetrack-shaped high-speed four-sided side-by-side opposed electron beam transverse collision high-charge heavy ion excitation ring (D).

[0084] As can be seen from the figure, high-charge heavy ions (17) with an ionization degree of μ in the ionization ring enter through the sixth quarter-circular energized guiding coil (20.6) at the upper end of the first high-charge heavy ion beam output / input channel (21.1) at the front end and then enter the entrance between the fifth energized guiding coil (d''') and the third energized guiding coil (19.2) at the front end of the flat racetrack-shaped high-speed four-sided side-by-side opposed electron beam transverse collision high-charge heavy ion excitation ring (D). Then they enter the middle of a second 90° turning energized guiding coil (24.2) with a regular octagon cross-section. Under the magnetic field generated by the second 90° turning energized guiding coil (24.2) with a regular octagon cross-section, they enter the first high-charge heavy ion horizontal drift straight track (23) on the right side of the flat racetrack-shaped high-speed four-sided side-by-side opposed electron beam transverse collision high-charge heavy ion excitation ring (D), drift backward along the first high-charge heavy ion horizontal drift straight track (23) on the right side and enter a third 90° turning energized guiding coil (24.3) with a regular octagon cross-section. Under the magnetic field generated by the third 90° turning energized guiding coil (24.3) with a regular octagon cross-section, they enter the rear-end sixth energized guiding coil (19.3) and the sixth energized guiding coil (19.4) perpendicular to the first high-charge heavy ion horizontal drift straight track (23), then drift into a fourth 90° turning energized guiding coil (24.4) with a regular octagon cross-section. Under the magnetic field generated by the fourth 90° turning energized guiding coil (24.4) with a regular octagon cross-section, they enter the second high-charge heavy ion horizontal drift straight track (23') on the left side, drift through the second high-charge heavy ion horizontal drift straight track (23') on the left side and then enter a first 90° turning energized guiding coil (24.1) with a regular octagon cross-section. Under the magnetic field generated by the first 90° turning energized guiding coil (24.1) with a regular octagon cross-section, they enter the front-end fifth energized guiding coil (d''') and the third energized guiding coil (19.2) perpendicular to the second high-charge heavy ion horizontal drift straight track (23') on the left side.

[0085] A horizontal flat racetrack-shaped loop is formed by the second highest charge heavy ion horizontal drift straight track (23') on the left, the first 90° turning energized guiding coil (24.1) with a regular octagon cross-section, the fifth energized guiding coil (d'''), the third energized guiding coil (19.2), the second 90° turning energized guiding coil (24.2) with a regular octagon cross-section, the third 90° turning energized guiding coil (24.3) with a regular octagon cross-section, the sixth energized guiding coil (19.3), the seventh energized guiding coil (19.4), and the second highest charge heavy ion horizontal drift straight track (23'). The highly charged heavy ions (17) with an ionization degree of μ that enter the flat racetrack-shaped high-speed four-sided side-by-side electron beam transverse collision high charge heavy ion excitation ring (D) through the sixth quarter-circular energized guiding coil (20.6) at the upper end of the first high charge heavy ion beam output / input channel (21.1) will all continuously orbit along this horizontal flat racetrack-shaped loop.

[0086] The highly charged heavy ions (17) with an ionization degree of μ in the ionization ring can also enter through the eighth quarter-circular energized guiding coil (20.8) at the upper end of the second high charge heavy ion beam output / input channel (21.2) at the rear end, enter the entrance between the sixth energized guiding coil (19.3) and the fifth energized guiding coil (d''') at the rear end of the excitation ring (D), and then immediately enter a fourth 90° turning energized guiding coil (24.4) with a regular octagon cross-section. Under the magnetic field generated by the fourth 90° turning energized guiding coil (24.4) with a regular octagon cross-section, it enters the second highest charge heavy ion horizontal drift straight track (23') on the left side of the excitation ring (D), and then will also continuously orbit along this horizontal flat racetrack-shaped loop.

[0087] The highly charged heavy ion beam (17) with an ionization degree of μ that enters the flat racetrack-shaped loop must be selectively excited by the high-speed electron beam before it can emit high-energy laser (29).

[0088] The high-speed surface electron flow is emitted from the first high-speed multi-faceted side-by-side counter-propagating surface electron flow transverse collision excitation region (d1) and the second high-speed multi-faceted side-by-side counter-propagating surface electron flow transverse repeated collision excitation region (d2). The first high-speed multi-faceted side-by-side counter-propagating surface electron flow transverse collision excitation region (d1) and the second high-speed multi-faceted side-by-side counter-propagating surface electron flow transverse repeated collision excitation region (d2) are located on the left and right sides or the upper and lower sides of the first high-charge heavy ion horizontal drifting straight orbit (23) and the second high-charge heavy ion horizontal drifting straight orbit (23'). The structures of the first high-speed multi-faceted side-by-side counter-propagating surface electron flow transverse collision excitation region (d1) and the second high-speed multi-faceted side-by-side counter-propagating surface electron flow transverse repeated collision excitation region (d2) are completely the same, and both are composed of 16 - 30 identical excitation surface electron flow emitters and 15 - 29 identical fifth energized guiding coils (d''') arranged side by side in series. The structures of the excitation surface electron flow emitter and the single ionization surface electron flow emitter are also completely the same. Only the total width of the third upper emission cavity (d') and the third lower emission cavity (d'') is much wider, and the voltages Ed2 and Ed3 applied at both ends are also much larger. The speed of the electrons in the emitted high-speed surface electron flow is also much, much larger than that of the first upper emission cavity (a') and the first lower emission cavity (a'').

[0089] The voltages Ed2 and Ed3 applied at both ends of the third upper emission cavity (d') and the third lower emission cavity (d'') are equal in magnitude and opposite in direction, and their values are slightly greater than the voltage required to excite the selected high-charge heavy ion with an ionization degree of μ to a certain laser energy level. The value of this certain laser energy level needs to be determined through accurate theoretical calculations, such as calculations using the fully relativistic multi-configuration self-consistent field method with Breit correction and QED correction, and verified through experiments.

[0090] A highly charged heavy ion beam with an ionization degree of μ between each third upper emission cavity (d') and each third lower emission cavity (d") is sheathed with a fifth energized guiding coil (d'''). The fifth energized guiding coil (d''') can greatly reduce the diffusion of the highly charged heavy ion beam and greatly increase the intensity of the highly charged heavy ion beam (17) with an ionization degree of μ. A fifth flat rectangular energized guiding coil (10.5) with a cross-section slightly larger than that of the third emission cavity (d') is sleeved outside each third upper emission cavity (d'), and a sixth flat rectangular energized guiding coil (10.6) with a cross-section slightly larger than that of the third reflection cavity (d") is sleeved outside each third lower emission cavity (d"). The magnetic fields generated by the fifth flat rectangular energized guiding coil (10.5) and the sixth flat rectangular energized guiding coil (10.6) can greatly reduce the diffusion of the mid-plane electron flow therein and greatly increase the intensity of the high-speed mid-plane electron flow therein. A thin iron sheet wrapped on the outer surfaces of the fifth flat rectangular energized guiding coil (10.5) and the sixth flat rectangular energized guiding coil (10.6) can act as a magnetic shield for the fifth flat rectangular energized guiding coil (10.5) and the sixth flat rectangular energized guiding coil (10.6), and can reduce the influence of the magnetic fields generated by the fifth flat rectangular energized guiding coil (10.5) and the sixth flat rectangular energized guiding coil (10.6) on the magnetic field generated by the fifth energized guiding coil (d''').

[0091] Because when the electrons emitted from the third electrically heated cathode (8.3) pass through the high-charge heavy ion beam (17) with an ionization degree of μ in the first high-charge heavy ion horizontal drift straight track (23) and the second high-charge heavy ion horizontal drift straight track (23') after being accelerated by the third upper emission cavity (d') or the third lower emission cavity (d''), if they do not collide with the high-charge heavy ions (17) with an ionization degree of μ, they will keep moving back and forth between the third upper emission cavity (d') and the third lower emission cavity (d'') at the original speed until they encounter the high-charge heavy ions (17) with an ionization degree of μ, excite the high-charge heavy ions (17) with an ionization degree of μ to a selected laser energy level, and their kinetic energy is almost reduced to zero and then is absorbed by a slender copper wire mesh (33) with a small amount of positive charge surrounding the first high-charge heavy ion horizontal drift straight track (23) on the right and the second high-charge heavy ion horizontal drift straight track (23') on the left. In this way, it can not only avoid the slow electrons being captured by the high-charge heavy ions (17) with an ionization degree of μ, reducing the ionization degree of the high-charge heavy ions (17) with an ionization degree of μ and reducing the intensity of the high-charge heavy ion beam (17) with an ionization degree of μ and the high-energy laser (29), but also ensure that each electron encountering the high-charge heavy ions (17) with an ionization degree of μ has a definite kinetic energy that can exactly excite the high-charge heavy ions (17) with an ionization degree of μ to a certain laser energy level, and all the electron kinetic energy can be almost completely converted into the excitation energy of the high-charge heavy ions (17) with an ionization degree of μ, and then is converted into the light energy of the radiated high-energy laser (29) through spontaneous emission. Such an excitation method has a much higher energy conversion efficiency than the general longitudinal excitation method.

[0092] On the rear extension line of the first high-charge heavy ion horizontal drift straight track (23) and the second high-charge heavy ion horizontal drift straight track (23') of the flat racetrack-shaped high-speed four-sided cross-parallel surface electron flow lateral collision high-charge heavy ion excitation ring (D), there is a total reflection mirror (34) fixed on the bottom plate, and on the front extension line there is a half reflection mirror (35) that can move slightly back and forth on the bottom plate, and the front and rear mirrors (34, 35) form an optical resonance cavity. The high-energy laser (29) radiated by the high-charge heavy ions (17) with an ionization degree of μ can emit high-intensity high-energy laser (29) after being reflected back and forth and amplified in the optical resonance cavity. Because the high-charge heavy ion beam (17) with an ionization degree of μ in each horizontal drift linear track can emit a high-intensity high-energy laser (29), a laser emission window is respectively provided on the front box wall of the excitation box (39) on the front extension line of the first high-charge heavy ion horizontal drift linear track (23) and the second high-charge heavy ion horizontal drift linear track (23'). The two laser emission windows can emit lasers respectively at the same time, or the two beams of high-energy lasers emitted from the two laser emission windows can be converged into a beam of high-energy laser (29) through a double optical fiber convergence tube (29') that can be controllably bent up, down, left, and right, and then emitted. In this way, the energy of the high-energy laser (29) will be more concentrated and the intensity of the high-energy laser (29) will be greater.

[0093] By using the high-pressure gas in the control device on the front outer wall of the excitation box (D) to push the control rod (42) upward or downward, the dual-fiber convergence tube (29') and the aiming device (19") fixed on the dual-fiber convergence tube (29') can be flexibly slid up and down. By using the rotation of the motor to rotate the connecting rod (36.2) left and right, the dual-fiber convergence tube (29') and the aiming device (19") fixed on the dual-fiber convergence tube (29') can be rotated right and left. In this way, the dual-fiber convergence tube (29') and the aiming device (19") fixed on the dual-fiber convergence tube (29') can be flexibly rotated up and down, left and right, and the time for aiming at the target and emitting the laser can be greatly shortened. The highly charged heavy ions flying out of the highly charged heavy ion emission window can be used for spectral analysis of highly charged heavy ions, and can also be used for nuclear reaction experiments between highly charged heavy ions and atomic molecules.

[0094] If the intensity of the high-charge heavy ion beam (17) with an ionization degree of μ is large enough and the intensity of the high-speed surface electron flow (30) used for excitation is also large enough, the power of the high-energy laser (29) that can be emitted will also be large enough. Depending on the wavelength and power of the laser, there can be various practical uses: from obtaining high-contrast holographic images of the internal structure of organisms to being used as a new type of high-energy laser weapon.

[0095] Since very light steering energized guide coils and deflection magnets are used to replace the heavier deflection magnets used before (ZL 201820262863.x), the weight of the flat racetrack-shaped high-speed four-sided cross-parallel surface electron flow transverse collision high-charge heavy ion ionization ring (B) and the flat racetrack-shaped high-speed four-sided cross-parallel surface electron flow transverse collision high-charge heavy ion excitation ring (D) is greatly reduced.

[0096] A thin and long copper wire mesh (33) with a small amount of positive charge is sheathed around the first high-charge heavy ion horizontal drift straight track (23) and the second high-charge heavy ion horizontal drift straight track (23') in the flat racetrack-shaped high-speed four-sided cross-parallel surface electron flow transverse collision high-charge heavy ion excitation ring (D). The thin and long copper wire mesh (33) with a small amount of positive charge will hardly have any effect on the movement of high-speed electrons accelerated by the emission cavity, but can capture low-speed electrons whose kinetic energy is almost reduced to zero after encountering high-charge heavy ions (17) with an ionization degree of μ, thereby preventing low-speed electrons from being captured by high-charge heavy ions (17) with an ionization degree of μ, reducing the intensity of high-charge ion beams (17) with an ionization degree of μ and high-energy lasers, and playing the role of an electrostatic speed selector (33).

[0097] exist Figure 11 —— Figure 12 The side view of the flat runway-shaped high-speed four-sided side-by-side facing surface electron flow transverse collision high-charge heavy ion ionization ring (B) and the flat runway-shaped high-speed four-sided side-by-side facing surface electron flow transverse collision high-charge heavy ion excitation ring (D) and the side view of the flat rectangular large ionization ring (B), the flat rectangular large excitation ring (D) and the flat rectangular large accessory box (40) installed on the car are overlapped up and down. The flat runway-shaped high-speed four-sided side-by-side facing surface electron flow transverse collision high-charge heavy ion ionization ring (B) and the flat runway-shaped high-speed four-sided side-by-side facing surface electron flow transverse collision high-charge heavy ion excitation ring (D) can also be installed on high-speed trains, ships or airplanes.

[0098] exist Figure 13 —— Figure 22Shown are the structural diagrams of the low-speed five-sided side-by-side opposed electron beam transverse collision single-charge heavy ion injection section (A), the flat racetrack-shaped high-speed five-sided side-by-side opposed electron beam transverse collision high-charge heavy ion ionization ring (B), and the flat racetrack-shaped high-speed five-sided side-by-side opposed electron beam transverse collision high-charge heavy ion excitation ring (D). Except that the number of sides of the surface electron beam in the low-speed five-sided side-by-side opposed electron beam transverse collision single-charge heavy ion injection section (A), the flat racetrack-shaped high-speed five-sided side-by-side opposed electron beam transverse collision high-charge heavy ion ionization ring (B), and the flat racetrack-shaped high-speed five-sided side-by-side opposed electron beam transverse collision high-charge heavy ion excitation ring (D) is five, and the furnace mouth (2) is a regular decagon furnace mouth, the rest of the structure and the action process are exactly the same as those of the low-speed four-sided side-by-side opposed electron beam transverse collision single-charge heavy ion injection section (A), the flat racetrack-shaped high-speed four-sided side-by-side opposed electron beam transverse collision high-charge heavy ion ionization ring (B), and the flat racetrack-shaped high-speed four-sided side-by-side opposed electron beam transverse collision high-charge heavy ion excitation ring (D).

[0099] Due to the low-speed five-sided side-by-side opposed electron beam transverse collision single-charge heavy ion injection section (A), the flat racetrack-shaped high-speed five-sided side-by-side opposed electron beam transverse collision high-charge heavy ion ionization ring (B), and the flat racetrack-shaped high-speed five-sided side-by-side opposed electron beam transverse collision high-charge heavy ion excitation ring (D), which have one more side of the surface electron beam than the low-speed four-sided side-by-side opposed electron beam transverse collision single-charge heavy ion injection section (A), the flat racetrack-shaped high-speed four-sided side-by-side opposed electron beam transverse collision high-charge heavy ion ionization ring (B), and the flat racetrack-shaped high-speed four-sided side-by-side opposed electron beam transverse collision high-charge heavy ion excitation ring (D), the intensity of the single-ionized heavy atom beam (4), the intensity of the high-charge heavy ion beam (17) with an ionization degree of μ, and the intensity of the high-energy laser (29) they generate all need to increase by one-fifth accordingly.

[0100] In Figure 23 —— Figure 25Shown is a schematic structural diagram of the first upper emission cavity (a'). The structures of other emission cavities are the same as it, except for the applied voltages. It consists of a first energized hot cathode (8.1) made of slender tungsten sheets, which is slightly wider than the width of the regular octagon or regular decagon furnace mouth (2) and has a length 3 - 6 times the width of the regular octagon or regular decagon furnace mouth (2), and is located on the upper or lower side of two high-charge heavy ion horizontal drift straight tracks (23, 23'), and a first flat rectangular metal frame (11.1) made of copper tubes or silver tubes or gold tubes with a layer of insulating film wrapped on the outside, which is adjacent to the first energized hot cathode (8.1) in parallel and consists of 50 - 100 units area slightly larger than that of the first energized hot cathode (8.1) and is connected in series with the second high resistance (12.2) at intervals. The width and length of the first flat rectangular metal frame (11.1) with a layer of insulating film wrapped on the outside are the same and parallel to each other. Each of the four corners of the first flat rectangular metal frame (11.1) is penetrated by an insulating rod (11') for fixing the first energized hot cathode (8.1) and the first flat rectangular metal frame (11.1) with a layer of insulating film wrapped on the outside. The upper end of the insulating rod (11') has three clamping openings. The lower clamping opening can just clamp the first energized hot cathode (8.1), and the upper two clamping openings can just clamp two flat rectangular copper plates with the same length and width as the first energized hot cathode (8.1) and parallel to it. Dielectrics are filled between the two flat rectangular copper plates and between the flat rectangular copper plates and the first energized hot cathode (8.1). A slender cylindrical second high resistance (12.2) rod passes through the middle of the short side of the first flat rectangular metal frame (11.1) with a layer of insulating film wrapped on the outside. The slender cylindrical second high resistance (12.2) rod is in close contact with the first flat rectangular metal frame (11.1) with a layer of insulating film wrapped on the outside. The first flat rectangular metal frames (11.1) with a layer of insulating film wrapped on the outside are parallel to each other and equally spaced. At both ends of the second high resistance (12.2) rod, a certain voltage is applied, which makes the electric potential of the first flat rectangular metal frame (11.1) gradually increase downward in turn, forming an accelerating electric field in the first flat rectangular metal frame (11.1) to continuously accelerate the electrons emitted from the first energized hot cathode (8.1). If the voltage applied at both ends of the second high resistance (12.2) rod is high enough, the accelerating electric field formed in the first flat rectangular metal frame (11.1) will be strong enough, and the electrons emitted from the first energized hot cathode (8.1) can reach a high speed close to the speed of light.

[0101] Because it is easy to apply a very high voltage to both ends of the second high resistance (12.2) rod with a small-sized high-voltage transformer, and it is also easy to accelerate electrons to a very high speed without the need for large equipment. Using high-speed electrons to highly ionize heavy atoms requires much smaller equipment than accelerating low-ionization heavy atoms to a very high speed with a giant accelerator and then colliding with a stripping film to obtain highly ionized heavy atoms. Therefore, this device can be miniaturized.

[0102] In Figure 26 —— Figure 28 is a schematic structural diagram of the first high-charge heavy ion beam output / input channel (21.1). The first high-charge heavy ion beam output / input channel (21.1) is an energized guiding coil with a flat rectangular cross-section. In the middle is a straight energized guiding coil, and at both ends are the first quarter-circular energized guiding coil (20.1) and the second quarter-circular energized guiding coil (20.2), but the bending directions of the coils at both ends are opposite. An important feature of the first high-charge heavy ion beam output / input channel (21.1) is that its inner surface is coated with a highly efficient insulating layer, the current passing through the coil is particularly strong, and the magnetic field in the coil is sufficient to guide the high-charge heavy ions to flow along the magnetic field lines in the coil. Other various energized guiding coils also have this important feature. The structure of the second high-charge heavy ion beam output / input channel (21.2) is the same as that of the first high-charge heavy ion beam output / input channel (21.1).

Claims

1. A high-charge heavy-ion high-energy laser is divided into two types due to different partial structures: a four-sided side-by-side opposed surface electron flow transverse collision high-charge heavy-ion high-energy laser and a five-sided side-by-side opposed surface electron flow transverse collision high-charge heavy-ion high-energy laser, and its characteristics are as follows: A high-charge heavy-ion high-energy laser is composed of a low-speed multi-faceted side-by-side electron flow transverse collision counter-jet single-charge heavy-ion injection section (A) containing an un-ionized heavy atom return channel (1', 1"), a flat-raceway-shaped high-speed multi-faceted side-by-side counter-jet electron flow transverse collision high-charge heavy-ion ionization ring (B) connected through a single-charge heavy-ion beam output / input channel (7') and the low-speed multi-faceted side-by-side electron flow transverse collision counter-jet single-charge heavy-ion injection section (A), a flat-raceway-shaped high-speed multi-faceted side-by-side counter-jet electron flow transverse collision high-charge heavy-ion excitation ring (D) connected through a first high-charge heavy-ion beam output / input channel (21.1), a second high-charge heavy-ion beam output / input channel (21.2) and the flat-raceway-shaped high-speed multi-faceted side-by-side counter-jet electron flow transverse collision high-charge heavy-ion ionization ring (B), and their required power, electrical, vacuum, and cooling auxiliary equipment. The flat-raceway-shaped high-speed multi-faceted side-by-side counter-jet electron flow transverse collision high-charge heavy-ion ionization ring (B) is installed in a sealed flat cuboid large ionization box (38) evacuated to a vacuum, and the flat-raceway-shaped high-speed multi-faceted side-by-side counter-jet electron flow transverse collision high-charge heavy-ion excitation ring (D) is installed in another sealed flat cuboid large excitation box (39) fixed on top of the flat cuboid large ionization box (38) and evacuated to a vacuum. Their required power, electrical, vacuum, and cooling equipment are all installed in the front part of another flat cuboid large accessory box (40) located below the flat cuboid large ionization box (38), and the low-speed multi-faceted side-by-side counter-jet electron flow transverse collision single-charge heavy-ion injection section (A) is installed in the evacuated rear part of the flat cuboid large accessory box (40). The low-speed multi-faceted side-by-side counter-propagating electron flow transverse collision single-charge heavy ion injection section (A) consists of a high-temperature atomic furnace (1) equipped with a high-frequency induction heating circuit and located on the left rear of a flat cuboid large accessory box (40), a low-speed multi-faceted side-by-side counter-propagating electron flow transverse collision single-ionization region (a) that is connected to the regular octagon or regular decagon furnace opening (2) of the high-temperature atomic furnace (1) and is located on the right rear of the middle part of the flat cuboid large accessory box (40) and is applied with a voltage slightly higher than the single ionization voltage of heavy atoms, a gradient heavy ion acceleration tube (5) that is connected to the rear of the low-speed multi-faceted side-by-side counter-propagating electron flow transverse collision single-ionization region (a) and is applied with a certain low voltage and consists of 50 - 100 regular octagon or regular decagon metal frames made of copper tubes, silver tubes or gold tubes that are slightly larger in cross-section than the furnace opening (2) and are wrapped with an insulating film on the outside and 49 - 99 first high resistors (12.1) connected in series alternately, an upward-bending quarter-circular negatively charged metal strip (7) that is connected to the rear of the gradient heavy ion acceleration tube (5) and is on the right side of the single-ionized heavy atom beam (4), an electromagnetic velocity selector (13) composed of a pair of front and rear permanent magnets and a pair of left and right parallel metal plates with equal amounts of opposite charges and connected to the metal strip (7), a single-charge heavy ion output / input channel (7’) that is vertically upward and has a regular octagon or regular decagon cross-section and is composed of energized guiding coils and is connected to the upper end of the electromagnetic velocity selector (13), and an un-ionized heavy atom return channel (1’, 1”) which consists of a high-temperature resistant plastic tube with a gas compressor (1’) at the end and is on the same straight line as the gradient heavy ion acceleration tube (5), and another high-temperature resistant plastic tube that is connected to the right side of the left end of the high-temperature resistant plastic tube with the gas compressor (1’) and has a high-pressure gas compressor (1”) at the end, and the left end of the other high-temperature resistant plastic tube with the high-pressure gas compressor (1”) is fixedly installed on the left side of the high-temperature atomic furnace (1), and the end of the single-charge heavy ion output / input channel (7’) is connected to the entrance of the first high-charge heavy ion electrostatic separation region (F1) or the first high-charge heavy ion magnetostatic separation region (F1’) at the left end of the flat racetrack-shaped high-speed multi-faceted side-by-side counter-propagating electron flow transverse collision high-charge heavy ion ionization ring (B). The outer surface of the gradient heavy ion acceleration tube (5) is sleeved with an energized guiding coil (5’) with a regular octagon or regular decagon cross-section. The low-speed multi-faceted side-by-side counter-propagating electron flow transverse collision single-charge heavy atom injection section (A) in the low-speed multi-faceted side-by-side counter-propagating electron flow transverse collision single-ionization region (a) is composed of 6-10 identical single-ionization surface electron flow emitters and 5-9 identical first energized guiding coils (a''') arranged side by side in series at intervals. The single-ionization surface electron flow emitter is composed of a first upper emission cavity (a') with four or five mutually equally spaced intersecting surfaces and a first lower emission cavity (a'') that is axially symmetrically distributed on the same plane as the first upper emission cavity (a'). The centers of 6-10 identical single-ionization surface electron flow emitters and 5-9 identical first energized guiding coils (a''') arranged side by side in series with them form the drift orbit of single-ionized heavy atoms. Both the first upper emission cavity (a') and the first lower emission cavity (a'') are composed of a first energized hot cathode (8.1) made of a flat rectangular tungsten sheet with a width slightly larger than the width of the furnace mouth (2) and a length 3-5 times the width of the furnace mouth (2), coated with Ba0 material, on the upper or lower side of the neutral heavy atom beam (3) directly in front of the furnace mouth (2), and a first flat rectangular metal frame (11.1) made of copper pipe, silver pipe or gold pipe, with an area slightly larger than that of the first energized hot cathode (8.1), and 50-100 of them are connected in series with the second high resistance (12.2) at intervals, and are wrapped with an insulating film on the outside. Each of the four corners of the first flat rectangular metal frame (11.1) is penetrated by a slender cylindrical insulating rod (11.1') for fixing the first energized hot cathode (8.1) and the first flat rectangular metal frame (11.1). There are three bayonets at the upper or lower end of the insulating rod (11.1'). The uppermost or lowermost bayonet can just hold the first energized hot cathode (8.1), and the two bayonets close to the first energized hot cathode (8.1) can just hold two flat rectangular copper plates with the same length and width as the first energized hot cathode (8.1) and parallel to it. Dielectric is filled between the two flat rectangular copper plates, between the flat rectangular copper plates and the first energized hot cathode (8.1). A slender cylindrical second high resistance (12.2) rod passes through a small round hole in the middle of the short side of the first flat rectangular metal frame (11.1), and the slender cylindrical second high resistance (12.2) rod is in close contact with the first flat rectangular metal frame (11.1). The first flat rectangular metal frames (11.1) are parallel to each other and equally spaced. There is a wire connection between a flat rectangular copper plate close to the first energized hot cathode (8.1) and the first energized hot cathode (8.1). In the middle of a flat rectangular copper plate far from the first energized hot cathode (8.1), or in the middle of a flat rectangular copper plate close to the first energized hot cathode (8.1), a single-pole double-throw switch K 12 or K 22 , the single-pole double-throw switch K 12 or K 22 A flat rectangular copper plate far from the first energized hot cathode (8.1) or a flat rectangular copper plate close to the first energized hot cathode (8.1) and a high-voltage power supply Ea 41 or Ea 42 are connected to the positive or negative electrode. A supercapacitor Ca1 or Ca2 with an extremely large capacitance is connected in parallel at one end of the two flat rectangular copper plates. Between the flat rectangular copper plate close to the first energized hot cathode (8.1) and the ground, there is a connection through a grounding switch K 11 or K 12 Each single-charge heavy ion beam between each first upper emission cavity (a') and each first lower emission cavity (a") is surrounded by a first energized guiding coil (a'''). The ratio of the width of the first energized guiding coil (a''') to the width of the first upper emission cavity (a') or the first lower reflection cavity (a") is 1:2 - 1:

4. The voltage applied across the two ends of the first upper emission cavity (a') is slightly greater than the single ionization voltage of heavy atoms measured experimentally or obtained through theoretical calculation, and the direction is downward. The voltage applied across the two ends of the first lower emission cavity (a") is equal in magnitude and opposite in direction to the voltage applied across the two ends of the first upper emission cavity (a'). A first flat rectangular energized guiding coil (10.1) and a second flat rectangular energized guiding coil (10.2) with a cross-section slightly larger than that of the first upper emission cavity (a') and the first lower emission cavity (a") are respectively surrounded outside each first upper emission cavity (a') and each first lower emission cavity (a"). A thin iron sheet is wrapped on the outer surfaces of the first flat rectangular energized guiding coil (10.1) and the second flat rectangular energized guiding coil (10.2). A cylindrical slender copper wire mesh (33) with a small amount of positive charge is also installed between each first upper emission cavity (a') or each first lower emission cavity (a") and the single-charge heavy ion beam (4). The flat-race-track-shaped high-speed multi-faceted side-by-side counter-propagating electron beam transverse back-collision high-charge heavy-ion ionization ring (B) is a flat track-and-field-shaped loop formed by successively connecting in series a first high-speed multi-faceted side-by-side counter-propagating electron beam transverse multi-ionization region (b1), a first high-charge heavy-ion electrostatic separation region (F1) or a first high-charge heavy-ion magnetostatic separation region (F1'), a second high-speed multi-faceted side-by-side counter-propagating electron beam transverse multi-ionization region (b2), and a second high-charge heavy-ion electrostatic separation region (F2) or a second high-charge heavy-ion magnetoelectrostatic separation region (F2'). The first high-speed multi-faceted side-by-side counter-propagating electron beam transverse multi-ionization region (b1) is on the left side of the flat track-and-field-shaped loop, and the second high-speed multi-faceted side-by-side counter-propagating electron beam transverse multi-ionization region (b2) is on the right side of the flat track-and-field-shaped loop. The structures of the first high-speed multi-faceted side-by-side counter-propagating electron beam transverse multi-ionization region (b1) and the second high-speed multi-faceted side-by-side counter-propagating electron beam transverse multi-ionization region (b2) are exactly the same, and both are formed by alternately connecting in series 16 - 30 identical multi-ionization surface electron beam emitters and 15 - 29 identical fourth energized guiding coils (b'''). The structures of the multi-ionization surface electron beam emitter and the single-ionization surface electron beam emitter are also exactly the same, except that the voltages applied across the two ends of the second upper emission cavity (b') and the second lower emission cavity (b'') are slightly greater than the specific voltage required to achieve an ionization degree of μ for heavy atoms, which is determined by experiment or theoretical calculation. This specific voltage is much, much larger than the single-ionization voltage applied across the two ends of the first upper emission cavity (a') and the first lower emission cavity (a''). The first high-charge heavy-ion electrostatic separation region (F1) consists of a first through electromagnetic focusing coil (15.1) with a regular octagon or decagon at the left end, a narrow rectangle with its long side perpendicular to the horizontal plane at the right end, and the left end connected to the front-end exit of the first multi-ionization region (b1) where high-speed multi-faceted counter-propagating electron beams collide transversely and repeatedly; a first quarter-circular energized guiding coil (20.1) connected to the right-end exit of the first through electromagnetic focusing coil (15.1); a first high-charge heavy-ion electrostatic separator (f1) with its front-side exit connected to the entrance end of the first high-charge heavy-ion beam output / input channel (21.1), its left end connected to the right-end exit of the first quarter-circular energized guiding coil (20.1), and its right-end exit connected to the second quarter-circular energized guiding coil (20.2); an energized guiding coil connected to the first high-charge heavy-ion electrostatic separator (f1) with a straight left end and a second quarter-circular energized guiding coil (20.2) at the right end; and a first through electromagnetic diffusion coil (15.2) with a narrow rectangle at the entrance, a regular octagon or decagon at the exit, and connected to the front-end entrance of the second high-speed multi-faceted counter-propagating electron beam transverse repeated collision multi-ionization region (b2), which are successively connected in series. The second high-charge heavy-ion electrostatic separation region (F2) consists of a third through electromagnetic focusing coil (15.3) with a regular octagon or decagon at the front end, a narrow rectangle with its long side perpendicular to the horizontal plane at the back end, and the front end connected to the back-end exit of the first high-speed multi-faceted counter-propagating electron beam transverse repeated collision multi-ionization region (b1); a third quarter-circular energized guiding coil (20.3) connected to the back-end exit of the third through electromagnetic focusing coil (15.3); a second high-charge heavy-ion electrostatic separator (f2) with its back-side exit connected to the entrance of the second high-charge heavy-ion beam output / input channel (21.2); an energized guiding coil connected to the second high-charge heavy-ion electrostatic separator (f2) with a straight right end and a fourth quarter-circular energized guiding coil (20.4) at the left end; and a second through electromagnetic diffusion coil (15.4) with a narrow rectangle at the entrance, a regular octagon or decagon at the exit, and connected to the back-end entrance of the second high-speed multi-faceted counter-propagating electron beam transverse repeated collision multi-ionization region (b2), which are successively connected in series. The first high-charge heavy-ion electrostatic separator (f1) is composed of four pairs of adjacent parallel metal plates with equal amounts of opposite charges perpendicular to the horizontal plane. The rear plate of the first pair on the left is positively charged, and the front plate is negatively charged. The rear plates of the second and third pairs in the middle are negatively charged, and the front plates are positively charged. The rear plate of the fourth pair at the back is positively charged, and the front plate is negatively charged. The two plates of the first and fourth pairs are relatively close, the two plates of the second pair are relatively far apart, and the distance between the two plates of the third pair is between that of the first and fourth pairs. The front outlet of the electrostatic charge separator is connected to the inlet of the fifth quarter-circular energized guiding coil (20.5) at the lower end of the first high-charge heavy-ion beam output / input channel (21.1). The second high-charge heavy-ion electrostatic separator (f2) is composed of four pairs of adjacent parallel metal plates with equal amounts of opposite charges perpendicular to the horizontal plane. The right plate of the first pair at the back is positively charged, and the left plate is negatively charged. The right plates of the second and third pairs in the middle are negatively charged, and the left plates are positively charged. The right plate of the fourth pair at the front is positively charged, and the left plate is negatively charged. The two plates of the first and fourth pairs are relatively close, the two plates of the second pair are relatively far apart, and the distance between the two plates of the third pair is between that of the first and fourth pairs. The front outlet of the electrostatic charge separator is connected to the inlet of the seventh quarter-circular energized guiding coil (20.7) at the lower end of the second high-charge heavy-ion beam output / input channel (21.2). The first high-charge heavy-ion magnetostatic and electrostatic separation region (F1') is successively formed by connecting in series a first electromagnetic focusing coil (15.1) with a regular octagon or decagon at the rear end, a narrow rectangle with the long side perpendicular to the horizontal plane at the front end, and the rear end connected to the front-end outlet of the first high-speed multi-faceted side-by-side counter-propagating electron beam transverse repeated collision multi-ionization region (b1), a pair of upper and lower opposite first trapezoidal magnets (25.1) connected to the front-end outlet of the first electromagnetic focusing coil (15.1), and a second quarter-circular energized guiding coil (15.2) with the left side connected to the right side of the first trapezoidal magnet (25.1) and the right side connected to the front-end inlet of the second high-speed multi-faceted side-by-side counter-propagating electron beam transverse repeated collision multi-ionization region (b2). The rear-side outlet on the right side of the first trapezoidal magnet (25.1) is connected to the inlet of the fifth quarter-circular energized guiding coil (20.5) at the lower end of the first high-charge heavy-ion beam output / input channel (21.1). The second high-charge heavy-ion magnetostatic and electrostatic separation region (F2') is successively formed by connecting in series a second electromagnetic focusing coil (15.3) with a regular octagon at the front end and a narrow rectangle with the long side perpendicular to the horizontal plane at the rear end, and the front end connected to the rear-end outlet of the first high-speed multi-faceted side-by-side counter-propagating electron beam transverse repeated collision multi-ionization region (b1), a pair of upper and lower opposite second trapezoidal magnets (25.2) connected to the rear-end outlet of the second electromagnetic focusing coil (15.3), and a fourth quarter-circular energized guiding coil (15.4) with the right side connected to the left side of the first trapezoidal magnet (25.1) and the left side connected to the rear-end inlet of the first high-speed multi-faceted side-by-side counter-propagating electron beam transverse repeated collision multi-ionization region (b1). The front-side outlet on the left side of the second trapezoidal magnet (25.2) is connected to the inlet of the seventh quarter-circular energized guiding coil (20.7) at the lower end of the second high-charge heavy-ion beam output / input channel (21.2). The first high-charge heavy-ion beam output / input channel (21.1) is a current-carrying guiding coil with the same cross-section as the flat rectangular cross-section at the exit of the first current-carrying guiding magnetic focusing coil (15.1). The entrance and exit ends of the first high-charge heavy-ion beam output / input channel (21.1) are both quarter-circular arcs, but the bending directions of the two are opposite. The section between the fifth quarter-circular current-carrying guiding coil (20.5) at the entrance end and the fourth quarter-circular current-carrying guiding coil (20.4) at the exit end is a straight current-carrying guiding coil. The sixth quarter-circular coil (20.6) at the exit end of the first high-charge heavy-ion beam output / input channel (21.1) can just be inserted into the entrance of the third current-carrying guiding coil (19.2) in the flat racetrack-shaped high-speed multi-faceted side-by-side counter-propagating electron beam transverse collision high-charge heavy-ion excitation ring (D). The second high-charge heavy-ion beam output / input channel (21.2) has the same structure as the first high-charge heavy-ion beam output / input channel (21.1). The eighth quarter-circular coil (20.8) at the exit end of the second high-charge heavy-ion beam output / input channel (21.2) can just be inserted into the entrance of the seventh current-carrying guiding coil (19.4) in the flat racetrack-shaped high-speed multi-faceted side-by-side counter-propagating electron beam transverse collision high-charge heavy-ion excitation ring (D). The flat racetrack-shaped high-speed multi-faceted side-by-side counter-propagating electron beam transverse collision high-charge heavy-ion excitation ring (D) is a flat track and field-shaped loop formed by successively connecting in series a first high-speed multi-faceted side-by-side counter-propagating electron beam transverse repeated collision excitation region (d1), a first high-charge heavy-ion receiving region (G1), a second high-speed multi-faceted side-by-side counter-propagating electron beam transverse repeated collision excitation region (b2), and a second high-charge heavy-ion receiving region (G2). The center of the flat track and field-shaped loop is the drift orbit of heavy ions with an ionization degree of μ. The center of the first high-speed multi-faceted side-by-side counter-propagating electron beam transverse collision excitation region (d1) on the right side of the flat track and field-shaped loop is the first high-charge heavy-ion horizontal drift straight track (23). The center of the second high-speed multi-faceted side-by-side counter-propagating electron beam transverse collision excitation region (d2) on the left side of the flat track and field-shaped loop is the second high-charge heavy-ion horizontal drift straight track (23'). There is an optical resonance cavity composed of a semi-reflecting mirror (34) and a total reflecting lens (35) on the extension lines before and after the first high-charge heavy-ion horizontal drift straight track (23) and the second high-charge heavy-ion horizontal drift straight track (23'). At the upper ends of the two high-charge heavy-ion beam output / input channels (21.1, 21.2) before and after the flat racetrack-shaped high-speed multi-faceted side-by-side counter-propagating electron beam transverse collision high-charge heavy-ion excitation ring (D), they are respectively connected to the entrance of the third current-carrying guiding coil (19.2) in front of the flat racetrack-shaped high-speed multi-faceted side-by-side counter-propagating electron beam transverse collision high-charge heavy-ion excitation ring (D) and the entrance of the seventh current-carrying guiding coil (19.4) at the back. The structures of the first high-speed multi-faceted side-by-side counter-propagating electron beam transverse collision excitation region (d1) and the second high-speed multi-faceted side-by-side counter-propagating electron beam transverse repeated collision excitation region (d2) are exactly the same. They are both composed of 16 - 30 identical excitation surface electron beam emitters and 15 - 29 identical fifth energized guiding coils (d”’) arranged in series side by side. The structures of the excitation surface electron beam emitter and the single ionization surface electron beam emitter are also exactly the same. Only the voltage applied across the third upper emission cavity (d’) and the third lower emission cavity (d”) is slightly greater than the specific voltage required to excite heavy ions with an ionization degree of μ to a certain laser energy level, which is determined by experiment or theoretical calculation. This specific voltage is much, much larger than the single ionization voltage applied across the first upper emission cavity (a’) and the first lower emission cavity (a”). The number of excitation surface electron beam emitters and fifth energized guiding coils (d”’) is also much larger than the number of single ionization surface electron beam emitters and the first energized guiding coils (a”’). On the outer edge of each fifth energized guiding coil (d''') on the second highest-charge heavy-ion horizontal drift linear orbit (23') on the left side, a copper ring (30) is sleeved. Each copper ring (30) is successively connected to the intermediate connections of a circuit formed by 16 - 30 eighth high resistors (12.8) in series. A high voltage (E d5 ) is applied across the two ends of the circuit formed by 16 - 30 eighth high resistors (12.8) in series. On the front wall of the excitation box (39) on the extension line in front of the first highest-charge heavy-ion horizontal drift linear orbit (23) on the right side and the second highest-charge heavy-ion horizontal drift linear orbit (23') on the left side, a laser emission window is provided respectively. The two laser emission windows are connected to a double-fiber converging tube (29') that can converge the two high-energy laser beams (29) emitted from the two laser emission windows into one high-energy laser beam (29). A collimator (29'') is fixed under the double-fiber converging tube (29'). The double-fiber converging tube (29') and the collimator (29'') can be rotated up, down, left, and right through a control device outside the box. In the middle of the two laser emission windows on the front wall of the excitation box (39), at the position where the trajectory of the high-speed and high-charge heavy ions passes quickly, a high-charge heavy-ion emission window is also provided. The high-charge heavy-ion emission window is equipped with a special glass that can withstand high voltage and allow high-charge heavy ions to pass through. Outside the high-charge heavy-ion emission window, an eighth energized guiding coil (17') that can be controllably bent up, down, left, and right is also installed. The control device outside the box consists of brackets (36.1, 36.2, 36.3) fixed outside the front wall, a motor fixed at the rear end of the bracket base plate (36.1), a connecting rod (36.2) fixed in the middle of the bracket base plate (36.1), with its upper end connected to the middle part of the double-fiber converging tube (29') and its lower gear meshing with the gear at the lower part of the motor, a cylinder (36.3) fixed at the front end of the bracket base plate (36.1) that can rotate around the lower rotating shaft, a control rod (42) inserted into the cylinder (36.3) with its upper end connected to the front part of the double-fiber converging tube (29') through a rotating shaft, and a high-pressure gas transmission pipeline connecting the circular hole at the rear side of the cylinder (36.3) between the cylinder (36.3) and the control rod (42) to a high-pressure cylinder. The first high-charge heavy ion receiving region (G1) consists of the first square steering magnet (24.1), the second square steering magnet (24.2) located at the front ends of the first high-charge heavy ion horizontal drifting straight track (23) and the second high-charge heavy ion horizontal drifting straight track (23’), and the second energized guiding coil (19.1) with a cross-section of a regular octagon or a regular decagon, bent at both ends and with a small opening in the middle therebetween. And there is a third energized guiding coil (19.2) with a small right end and a large left end sleeved outside the second energized guiding coil (19.1) with a small opening. There is an entrance at the front side of the left end of the third energized guiding coil (19.2). The end of the sixth quarter-circular coil (20.6) at the outlet end of the first high-charge heavy ion beam output / input channel (21.1) can just be inserted into the entrance of the third energized guiding coil (19.2). The second high-charge heavy ion receiving region (G2) consists of the third square steering magnet (24.3), the fourth square steering magnet (24.4) located at the front ends of the first high-charge heavy ion horizontal drifting straight track (23) and the second high-charge heavy ion horizontal drifting straight track (23’), and the sixth energized guiding coil (19.3) with a cross-section of a regular octagon or a regular decagon, bent at both ends and with a small opening in the middle therebetween. And there is a seventh energized guiding coil (19.4) with a small left end and a large right end sleeved outside the sixth energized guiding coil (19.3) with a small opening. There is an entrance at the rear side of the right end of the sixth energized guiding coil (19.3). The end of the eighth quarter-circular coil (20.8) at the outlet end of the second high-charge heavy ion beam output / input channel (21.2) can just be inserted into the entrance of the third energized guiding coil (19.2). In the four-sided side-by-side counter-propagating electron beam transverse collision high-charge heavy ion high-energy laser, the number of surface electron beams is four, and the furnace opening (2) is a regular octagon. In the five-sided side-by-side counter-propagating electron beam transverse collision high-charge heavy ion high-energy laser, the number of surface electron beams is five, and the furnace opening (2) is a regular decagon. The three large boxes, namely the flat cuboid large ionization chamber (38) located below and fixedly connected together, the flat cuboid large excitation chamber (39) located above, and the flat cuboid large accessory box (40) located below the flat cuboid large ionization chamber (38), can be installed together in a car, or an airplane, or a warship, or a laboratory.

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