Quantum mechanical systems and methods for channel stimulation and extraction - Patents.com

Abstract

The present invention includes novel quantum mechanical systems and processes for the stimulation and extraction of certain transition state components. In various embodiments, an intermediate channel can be probability enhanced and components can be extracted from among an infinite number of equally probable states B. The systems and methods implement a quantum mechanical reaction that transitions from an initial state A to a final state C through an infinite number of equally probable intermediate general state B channels. A subset of the state B channels can be probability enhanced via the Ying cell system and method, allowing a specific probability enhanced state B channel to be indicated upon detection.

Description

[Technical field]

[0001] This application claims the benefit under 35 USC §119(e) of U.S. Provisional Patent Application No. 63 / 316,507, filed March 4, 2022, the contents of which are incorporated herein by reference in their entirety.

[0002] The present invention relates to the preparation of a quantum mechanical system and the stimulation and extraction of specific intermediate channels from an infinite number of Feynman Path Integral Formulation channels ("PIFs") or "transition states" for the process of proceeding from state A through an infinite number of intermediate state B channels to state C, where after a view transformation from DView to PView, the extraction of the specific specific state B channels is performed prior to or essentially simultaneously with the display of the extracted states in human sensory space. [Background technology]

[0003] Quantum mechanics was formulated about a century ago and contains substantially different aspects from those of classical mechanics. Quantum mechanics is essentially non-deterministic, while classical mechanics is deterministic. There are many different interpretations of quantum mechanics, the Copenhagen interpretation being the one generally accepted and often taught in schools. Feynman's path integral formulation is an alternative interpretation in which there are infinitely many equiprobable paths, aka intermediate channels, that can lead from state A through transition states to state B (including the creation and annihilation of virtual particles) to state C. Summary of the Invention [Problem to be solved by the invention]

[0004] However, most of these state B channels are not visible or observable due to destructive interference at the observation point. Neither interpretation can explain successful experiments in certain fields, for example, D+D experiments and their daughter particles. Therefore, technological applications and improvements for the stimulation and extraction of such state B channels are needed. [Means for solving the problem]

[0005] The present invention includes a system and method for stimulating and extracting certain transition states. In an exemplary embodiment, the system and method provide a quantum mechanical system ("QM system"). The Ying cell system discussed herein is a QM system. An embodiment includes a system for extracting certain intermediate transition states and / or transition state components, including a sealed container containing an electrolyte, an anode connected to the sealed container, a cathode connected to the sealed container, a power source connected to the anode and the cathode, an alpha source disposed within the sealed container, a gamma (γ) source disposed outside (or alternatively disposed inside) the sealed container, a Faraday cage including the sealed container, an insulating container including the Faraday cage and the sealed container, a first pair of thermocouples disposed within the Faraday cage, and a second pair of thermocouples disposed outside the sealed container.

[0006] In an embodiment, the anode is a platinum rod and the cathode is palladium foil. The power supply may be a reversible 15V direct current (DC) power supply. The Gamma power supply has a current of 1 microcurie. 60 Co disks, etc. 60 The alpha source may be a 0.1 microcurie Co disk. 210 Po disks, etc. 210 The electrolyte may be a Po disk. The embodiment may further include a second pair of thermocouples disposed within the insulating container and a second pair disposed outside the Faraday cage. The electrolyte may be deuterium oxide.

[0007] Embodiments may further include systems and methods for extracting the generated helium and / or excess energy based on the QM Ying cell system described above. Such methods may include providing deuterium oxide in a sealable container, electrolyzing the deuterium oxide via a power source, then stimulating a specific transition state involving helium + gamma, and extracting the generated helium and / or excess energy from the Ying cell. Various embodiments may include applying a reverse voltage to the sealable container to re-stimulate the transition of deuterium oxide to the helium + gamma state. Further embodiments may include applying a reverse voltage to the sealable container to re-stimulate the transition of deuterium oxide to the helium + gamma state. Stop Similarly, the deuterium oxide to helium and gamma states can be converted to hydrogen by removing the alpha source. Stop The gamma source can be removed to allow for the electrolysis to proceed. The temperature can be tracked via a pair of thermocouples, and the power supply can be adjusted based on the temperature to stimulate the desired amount of helium and / or excess production energy for extraction. Additionally, electrolysis can be performed over a period of time, e.g., hours, days, etc.

[0008] Thus, a QM system can be a) displayed in a Probability View (“PView”) and then b) an agent (e.g., a stimulus) can be applied to increase the probability of a particular channel (e.g., a particular intermediate state) from an infinite number of previously equally probable channels. The intermediate states can now be described herein as states B. A particular intermediate state is a channel out of the original infinite number of channels in Feynman probability space that, when appropriately stimulated, is extracted into “real space” out of the infinite number of Feynman Path Integral Formulation (“PIF”) channels, and these particular channels are then added to the HSS as particular states B. display These displayed / extracted channels are then unavailable for destructive interference when observed, where observation is generally a destruction or annihilation event. HSS stands for Human Sensory Space (i.e., Frame of Reality).

[0009] The system and method also provide the necessary conditions for a QM system initially in a direct particle view ("DView") to be transformed into a stochastic wave view ("PView"). Thus, embodiments of the present invention enable a QM system to be displayed in a PView.

[0010] In an additional embodiment, once the QM system is configured in PView, agents or stimuli can be applied to increase the probability of extracting one or more specific channels from an infinite number of previously equally probable Feynman PIF channels.

[0011] In various embodiments, if the extraction is performed contemporaneously with or prior to the observation or event, the observation or event can demonstrate that the extracted state is one of the State B transition states. [Brief description of the drawings]

[0012] The drawings are not necessarily drawn to scale, but like numerals may refer to like components in different figures. For example, numerals with different letter suffixes may represent different instances of a similar component. The drawings generally illustrate, by way of example, and not by way of limitation, various aspects discussed in the present document. In this drawing: [Figure 1] FIG. 1 illustrates an exemplary Ying cell system according to embodiments discussed herein. [Diagram 2] FIG. 2 shows a flow chart for channel component extraction according to the embodiments discussed herein. [Diagram 3] FIG. 3 shows a flow chart for channel stimulation according to embodiments discussed herein. DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS

[0013] The claimed invention is supplemented below by a particular sequence of process steps, which have been demonstrated by previous experimentation by the inventors.

[0014] The terms used herein are for the purpose of describing particular embodiments only and are not intended to be limiting of the invention. As used herein, "and / or" includes any and all combinations of one or more of the associated listed items. As used herein, the singular forms "a" and "the" are intended to include the plural as well as the singular, unless the context clearly indicates otherwise. Furthermore, as used herein, it will be understood that the terms "comprise" and / or "comprises" specify the presence of features, steps, operations, elements, and / or components of a state, but do not exclude the presence or addition of one or more other features, steps, operations, elements, components, and / or groups thereof.

[0015] Unless otherwise defined, all terms used herein (including technical and scientific terms) have the same meaning as commonly understood by those skilled in the art to which the present invention belongs. Furthermore, terms as defined in commonly used dictionaries should be interpreted as having a meaning consistent with their meaning in the context of the relevant art and this disclosure, and will not be interpreted in an idealized or overly formal sense unless expressly defined in this specification.

[0016] It will be understood that in the description of the present invention, many techniques and steps are disclosed. Each of these has its own advantages, and each can also be used in combination with one or more, or in some cases, all of the other disclosed techniques. Thus, for the sake of clarity, the description refrains from unnecessarily repeating all possible combinations of the individual steps. Nevertheless, the specification and claims should be read with the understanding that such combinations are fully within the scope of the present invention and claims.

[0017] New aspects of quantum mechanics, their interpretation, and their applications are discussed herein. In the following description, for purposes of explanation, numerous specific details are set forth in order to provide a thorough understanding of the present invention. However, it will be apparent to one skilled in the art that the present invention may be practiced without some of these specific details or with the substitution of certain details.

[0018] Aspects of the invention include a) converting a QM system from a DView to a PView, and then b) extracting a particular class of intermediate channels from an infinite number of Feynman path integral formulated channels. It will be appreciated that embodiments are not limited by the processes, process geometries, or settings used herein as experiments or examples.

[0019] The disclosed aspects are to be considered as illustrative of the invention and are not intended to limit the invention to the specific embodiments illustrated in the following figures or description.

[0020] Various embodiments discussed herein describe a quantum mechanical system for demonstrating probability enhancement of a state B channel between state A and state C. State A is demonstrated herein as an initial D+D state, a particular state B channel is He+γ, and state C is a D+D final state. Thus, it can be demonstrated that within a transformation (e.g., state A to state C), there may be an infinite number of equiprobable paths or channels, but a particular channel (e.g., a particular state B channel) can be extracted.

[0021] Starting with the basics, it has been shown that when a stream of electrons (a "quantum system" or "QS") is beamed onto a target, a shadow pattern can be produced. But when the experimental setup sends these electrons through one or more very small slits, you get a diffraction or interference pattern, even when only one electron is emitted at a time.

[0022] The present invention demonstrates that raw electrons are presented in the human sensory space ("HSS"), (i.e., reality frame), as discrete particles until they have an experience. This is referred to herein as the "discrete view", or alternatively shortened to "DView". In the slit example above, the experience would be that the electron travels through a small slit and, after passing the slit, is given an "opportunity" to "choose" about its path of travel. This process can be described as going from a discrete particle view ("DView") to a probability wave view ("PView") in the human sensory space. This electron beam is then detected on a screen, called an "event", where diffraction or interference patterns are observed, and disappears. Thus, embodiments of the present invention demonstrate that a quantum system ("QS") can a) be re-presented from the DView to the PView via experience; and b) the quantum system ("QS") is manipulated or stimulated while in the PView.

[0023] Thus, when a particular point in that probability space is examined for a particular feature or characteristics, an interaction is required and a value is determined. However, examining different points will return different values. Interactions can in principle be measured, and those involving quantum objects can also give definite values, regardless of whether they are actually observed.

[0024] An embodiment of the invention includes the application of transition state stimulation and extraction, incorporating aspects of the quantum mechanical system described above. An electrolysis apparatus can include the use of an anode (e.g., platinum anode) and a cathode (e.g., palladium cathode) in heavy water (D2O). An alpha (α) emitter and a gamma (γ) emitter applied to the system generate heat. However, if (i) the α or γ emitter is removed, the heat rise stops; or (ii) if H2O is substituted for D2O, the heat rise stops. The demonstration of heat rise indicates that an "experience" by, for example, application of γ to the D+D system, followed by stimulation by application of α to the D+D system, i.e., an "event" by observation, is sufficient. However, if any of these are removed, the "heat rise stops" indicates that application of α, application of γ, and a deuterium oxide source are all required.

[0025] Deuterium particles directed at the cathode are referred to herein as being in the DView. The term DView is used for purposes of clarity and is not meant to limit or restrict any embodiment or application. The DView, when directed at the slit, can be viewed similarly to an electron in a two-slit experiment, but before the choice is given by the experimental setup as to "choose" which slit to pass through. In a two-slit experiment, the PView represents the probability of infinite paths that an electron can take. Experience (e.g., an electron passing through two slit membranes and / or an electron having the option to choose to pass through two slit membranes) is required to transition the DView particle to the PView.

[0026] The systems and methods of the present invention require, at a minimum, the creation or annihilation of particles or quasiparticles without the need for a quantum mechanical system for "experience." In various embodiments, 60The CO can act as a gamma source for pair creation (aka "experience"), and thus transition from DView to PView. However, various kinds of gamma sources are available. The applicable gamma source provides sufficient energy for pair creation. Then, in PView, 210 Alpha sources such as Po stimulate and increase the probability of emission of alpha particles of various corresponding energies, thus Previously As with gamma sources, alternative alpha sources may be utilized, and in general any source may be utilized to obtain the boson-boson interactions and stimulation described herein.

[0027] As such, the embodiments of the Ying cell described herein further represent experimental validation of quantum mechanical particle generation and an improvement of the Copenhagen interpretation. In particular, the Ying cell provides a light emission stimulus, allowing the extraction of a specific transition state (a certain state B) between states A and C.

[0028] Ying Cell Systems, Processes, and Experiments Aspects of the invention will now be described by reference to the accompanying figures, which represent preferred embodiments. In various embodiments and experiments, a quantum mechanical system was considered in which the initial state A of the system is D+D and its final state C is also D+D, with deuterium being produced by electrolysis of DO.

[0029] FIG. 1 shows an exploded perspective view of a device including a Ying cell 19, a Faraday cage 20, and an insulating container 23 according to various embodiments of the present invention. In various embodiments, the device can be configured with at least one power source 11. In embodiments, the power source can include a switchable and reversible 15V DC power source. Power can go to a first wire leading to an anode 12, such as a platinum (Pt) anode, and a second wire leading to a cathode 15, such as a palladium (Pd) cathode. The first and second wires can be connected to the anode and cathode, respectively, and then connected to the Ying cell 19. In various aspects, the Ying cell can be a container such as a sealable container, a beaker with a stopper, etc. The first and second wires can be connected to the Ying cell 19, for example, via a stopper or seal on the Ying cell 19. The Ying cell 19 may further comprise holes for the anode and cathode or their connecting wires (e.g., first and second wires), and an attachment for holding a thread or wire that can be used to hold the alpha source 17. In an embodiment, the alpha source is 210 It can be a Po disk.

[0030] The gamma source 13 may be mounted outside the Ying cell 19. In an embodiment, the gamma source is 60 It may be a radioactive source such as a CO disk.

[0031] In various embodiments, the Ying cell can be filled with an electrolyte 14, such as deuterium oxide (DO). Other electrolytes that provide a source of deuterium during electrolysis can also be utilized in the various embodiments discussed herein. At least two internal thermocouples 16, 18 can be disposed outside the Ying cell. The Ying cell and internal thermocouples 16, 18 can be disposed inside a Faraday cage 20, and two or more external thermocouples 21, 22 can be disposed outside the Faraday cage 20. The Faraday cage 20 blocks electromagnetic fields, and various examples can include a coating of conductive material and / or a mesh coating of conductive material.

[0032] The Faraday cage 20 may then be placed inside an insulating enclosure 23 .

[0033] In various experiments performed, the QM Ying cell system includes an initial state, state A, an infinite number of intermediate states B, and a final state C. In an embodiment, state A is "D+D" and final state C is also "D+D", where deuterons are produced by electrolysis of DO, which along with all other moieties produces excess heat.

[0034] In various embodiments of the Ying cell system, the Pt anode and Pd cathode have D2O as the electrolyte and are connected to a 15V DC battery power supply. In various configurations, Pd foils can be used, for example, 2.5 cm x cm, 0.025 mm thick Pd foils. In various experiments, both Johnson Matthey and Wilkinson foils have been successfully tested in various Ying cell configurations and embodiments. Applicable geometries can include a 1.0 mm diameter straight Pt as the anode. Four thermocouples can also be used. In one example, two thermocouples were taped to the outside of the Ying cell at different heights, and the other two thermocouples were placed outside the Faraday cage 20 but within the insulating container. This placement of the thermocouples prevents inaccurate readings due to potential hot spots.

[0035] In another example, gamma source 13 is a 1 microcurie Gamma source manufactured by Sargent & Welch. 60The gamma source 13 was a Co disk. The gamma source 13 can be taped to the outside of the beaker used in the Ying cell system. The alpha source 17 was a 0.1 microcurie disk placed inside the Ying cell beaker, positioned as close as possible to the Pd cathode without blocking the flow of deuterium (hereafter "D") to the cathode. The components were placed inside a Faraday cage, and then the entire apparatus including the Faraday cage was placed inside an insulated container. After overnight "seasoning" during which "loading" of D occurs at the Pd interstitial sites, an increase in heat was noted. In various embodiments, deuterium oxide can be electrolyzed for a period of time (e.g., 1 hour, 2 hours, 4 hours, 6 hours, 8 hours, 10 hours, etc.). Once the increase in heat has ceased, it has been found that applying a reverse voltage to the cell for a short period of time and allowing it to reset overnight will cause the cell to begin to react again. Such a reaction is easily achieved by swapping the anode and cathode leads. A 10 second reversal and optimal overnight reset is usually sufficient to make the cell operational again.

[0036] No additional electrolyte salt was required to add to the heavy water. The characteristic heat rise in the Ying cell was 60 Co or 210 It is stopped by either removal of Po or substitution of H2O for D2O. It will be understood that the present invention is not limited by the device, the shape of the device, or its configuration.

[0037] State B channels, also referred to here as Feynman infinite equiprobable paths or channels, have been determined to lie between the initial state A, the D+D state, and state C, a common final D+D state. A subset of state B channels includes the intermediate channel "D+D → He+γ → D+D", where this different nature of the channel has different energies for He and γ. Ds emitted by electrolysis of D2O are particles in DVView. DVView is a one-slit or two-slit experiment in which photons or electron beams are emitted and they are then redistributed. settingThis is similar to the case of photon or electron beams when the slits are not at the same wavelength, especially when no opportunity is given to reach the slits later in a one-slit or two-slit experiment.

[0038] Furthermore, it was pointed out that in order to move from DVView to PView, if the QM system is not already in PView, an experience is required. The experience can be, at least, the creation or annihilation of a particle (or quasiparticle) that (i) is within the order of the de Broglie wavelength of the initial or final QM system and (ii) does not originate from and / or involve this QM system.

[0039] If the experiment is set up for D+D→X→D+D, where X is the state B transition state, the inclusion of a gamma-ray emitter is sufficient to produce "pair production" when in the region of an atomic nucleus (e.g., a Pd nucleus), providing a necessary and sufficient condition for "experience" as discussed herein. Experience can be what transforms a D+D QM system from a DVView to a PView. Such a DVView to PView transition can occur without the gamma-ray emitter (e.g., 60 The heat generation in the Ying cell is shown upon removal of the CO2 disk. Stop To make.

[0040] When the QM system is in PView, "D+D→He+γ→D+D" is part of an equiprobability path or channel. In one embodiment, to reduce the collision loss of alpha, 210 An alpha emitter such as a Po disk was placed in D2O close to the cathode. 210 Po decay alpha results in the emission of stimulated alpha extracted from the D+D→He+γ paths, thereby removing these channels from the infinite equiprobability paths. Such extracted channels from state B are no longer available to participate in destructive interference (aka "events") at the observation / destruction point.

[0041] Furthermore, once this stimulated alpha is realized, the response also realizes gamma. Therefore, an initial alpha is needed to stimulate the extraction of this response. This is because the alpha emitters (e.g. 210 Heat generation in a Ying cell upon removal of a Po disk. stops It's also the reason.

[0042] Therefore, the above experiments indicate that D is involved in heat production. を In a similar experiment, the Ying Cell system stopped producing heat when replaced with H2O. Therefore, the heat rise in the Ying Cell system can be reduced by removing the alpha or gamma source, or by replacing electrolytes, e.g., by replacing D2O with H2O. Stop .

[0043] Similar to the extraction of He and γ from the state A→B reaction, (i.e., D+D→He+γ) involves the production of He and γ. Therefore, the D+DQM system Includes Two particles have been generated. Thus, embodiments of the present invention generate an "event" that indicates the transformation of state A (D+D) to a specific state B (He+γ) and allows for the extraction of at least one of He or γ, or the excess energy generated.

[0044] In the above example, the neutron does not need to conserve momentum because the Pd and γ systems serve to balance the momentum of the stimulated alpha (as explained further below).

[0045] In metals, the positive ions are in a sea of ​​electrons and there is no Coulomb repulsion between the positive ions. However, there is metallic bonding, which is the electrostatic attraction between the metal atoms or ions and the delocalized electrons. Thus, there is no repulsion between the positive ions or between the interstitial atom D and the incident D. Therefore, the Coulomb repulsion of D and D may not be relevant in metals.

[0046] 2 shows a flow chart for application of the systems and methods discussed herein. The embodiment allows for the extraction of components of the electrolyte provided in the Ying cell system of FIG.

[0047] In an example, deuterium oxide (heavy water, also known as D2O) can be provided in the Ying cell system 210. The deuterium oxide acts as an electrolyte from which deuterium can be extracted.

[0048] In block 220, the deuterium oxide undergoes electrolysis to produce deuterium, which (i) first reaches and enters the interstitial sites of the Pd cathode, and then (ii) is transported by later arriving projectile D to (iii) produce an initial transition state A=D+D (and the original final state C is also =D+D).

[0049] In an example, given an electrolyte containing deuterium oxide, after electrolysis, when the resulting Ds enters the Pd cathode, there can be an infinite number of intermediate states B (between states A and C) and can contain the specific channel He+γ. The electrolysis can be carried out for a period of time, e.g., overnight, hours, days, etc., to produce Ds. When Ds reaches the Pd cathode, it produces the initial transition state A=D+D as described above, and the initial final state C is also =D+D. In the example, 60 After moving from DVView to PView through the "experience" provided by Co, and 210 After "boson-boson interaction / stimulated extraction by alpha from Po", the desired or targeted amount of a component such as helium and / or excess energy is produced.

[0050] In block 225, electrolysis can be performed to obtain deuterium. In block 227, such an action (PO 210 The inflow alpha from PO 210 A particular desired transition state corresponding to the inflow alpha from can be stimulated / created / extracted, thus providing He+γ and / or excess energy. Such excess energy can be partially or fully utilized in the electrolysis in block 220, if desired. The flow chart continues at block 230 with the unused He and / or excess energy.

[0051] At block 230, the generated He+γ and / or excess energy can be extracted from the system. The helium and / or excess energy generated can be extracted from the system in any of a number of ways known to those skilled in the art. For example, an extraction tube can be connected to a sealable container to extract the helium as it is produced. As discussed herein, the volume of helium and / or excess energy produced can be adjusted based on changes to one or more of the power source, alpha source, and gamma source.

[0052] In one example, after electrolysis of heavy water with Pd as the cathode and Pt as the anode, D reaches the Pd cathode and occupies the interstitial sites of Pd. When heavy water is further electrolyzed, the system also produces D, λ de Broglie At a rate of about A°, the gamma from CO is incident on Pd (whose interstitial sites are now mostly filled with initial D), leading to the state A=D+D. The incident gamma from CO with energies of 1.173 or 1.332 MeV is sufficient for pair production that does not require the quantum object to be involved. This pair production creation can occur outside the Heisenberg cut of the quantum object, but within a distance that is the de Broglie wavelength of the quantum object, or the de Broglie wavelength of the particle created or destroyed (e.g. a quasiparticle). This is referred to here as an "experience". So, with this "experience", within the HSS where the behavior of the quantum object is projected, the system exhibits thereby transitioning from a DVView to a PView. Thus, a probability distribution is mapped for each of the attribute sets that can be displayed in the HSS reality domain.

[0053] Moreover, the arrival of incident alpha particles from an alpha source at the cathode appears to be sufficient to provide stimulation of the desired transition state by boson-boson interactions. These arriving incident alpha particles have different energies due to the variation of the collision history before reaching the individual quantum objects. When these incident alpha particles with energy states corresponding to the energies of the various possible alpha particles of the series of possible "D+D→He+γ" reactions are within the reaction distance of said corresponding points, said incident alpha particles (of various energies) disturb these corresponding states with these same or similar energies, thus stimulating and increasing the probability of the production of He+γ, resulting in the production of He+γ. These daughter particles can then travel further and further and stimulate the production of further next generation daughters He+γ. Each of these can be called an "event" and is also a necessary condition. And when the alpha source is removed, the production of excess heat is also Stop .

[0054] Neutron production is also not necessary, at least in part, for the solid-state mode of this embodiment. In solids, H, D and He can drift, but such drift speeds are slow and therefore the time is significantly longer than that of state A → B, e.g., D + D → He + γ reaction. The effect may therefore be comparable to the Mossbauer effect fluctuations seen in solids but not in gases. It is also possible to consider here that the entire Pd crystal is involved, and assume that momentum is conserved as the "daughter alpha particle" and the Pd "cathode + daughter γ" move in opposite directions to each other upon the production of daughter He + γ. Under this scenario, neutrons are not required to conserve momentum.

[0055] Moreover, in metals there is no Coulomb repulsion between positive ions since they are in a sea of ​​electrons. There may be metallic bonds between metal atoms / ions and delocalized electrons which are essentially electrostatic attractions. Hence there is no repulsion between positive ions. Also there is no repulsion between interstitial atoms D and incident atoms D. The Coulomb repulsion which is said to keep interstitial atoms D and incident atoms D apart may not be relevant in metals. In other words, positive ions (e.g. interstitial Ds and incident Ds in this case) are in a sea of ​​electrons and therefore are not subject to Coulomb repulsion.

[0056] These above reasons explain why no neutrons have been found in successful experiments producing He, γ, or excess energy, and why the Coulomb repulsion between incident D and interstitial D is negligible. Furthermore, both a gamma emitter and an alpha emitter are needed, since removing either one will stop the reaction. Also, a D source is needed, since replacing it with a H source like water will stop the reaction.

[0057] The experiment further showed that, especially after multiple collisions along the path from the He source and Pd cathode of the experiment, 210 Given the low penetration capability of alpha particles from Po decay, it suggests that the initial reactions above mostly occur at the surface of the cathode. Thus, a cathode with a large surface area may be suitable for this purpose. Increasing the number of incident gammas and alphas may further scale up the resulting products. On the other hand, increasing the electrolysis voltage so that D has higher energy may be counterproductive. However, it may provide an optimal voltage for this type of experiment. Furthermore, by installing a suitable timer-based automatic voltage reversal mechanism, the cathode can be "refreshed" to allow a more continuous production of the resulting products, such as heat.

[0058] In addition, from the Sargent & Welch disc 210It was noted that the alpha particles emitted from Po decay have low energy and therefore long de Broglie wavelengths, especially after the collisions on the way to the Pd cathode. The energy range of the alpha particles that ultimately reach the Pd target will vary, as it depends on the number of collisions of each alpha particle on its way from the disk to the target. However, their energies will all be very low, and there will essentially be no penetration of the Pd target. Thus, the expected interactions will be on the surface of the Pd, as already mentioned.

[0059] We can also assume that the stimulated daughter alpha has the same energy as the incident alpha. Therefore, when the first daughter alpha produced escapes from the Pd, it is likely to go towards the heavy water side due to momentum conservation, but the momentum of the produced / escaped daughter alpha is balanced by the entire Pd cathode and the daughter γ recoiling in the opposite direction. Therefore, as mentioned before, there is no need to produce neutrons at this stage to conserve momentum.

[0060] On the other hand, as mentioned above, gamma is directed in the opposite direction, e.g., towards Pd, so the gamma energy can be dissipated by pair production in Pd, conversion to heat, or escape. Also, there is no need to produce neutrons at this stage to conserve momentum.

[0061] In other words, incident alpha, for example, via boson-boson interaction, can stimulate He+γ via D+D→He+γ, bringing it into the HSS reality space. This is essentially a very low probability reaction. However, considering Feynman's PIF, all intermediate channels (aka states B) have equal probability, so the increase in probability of a particular intermediate channel due to boson-boson interaction greatly increases its creation compared to all other intermediate channels. Therefore, other channels similarly stimulated to that channel will no longer be able to participate in destructive interference within the full path of state A→C, for example "D+D→D+D".

[0062] Thus, as mentioned several times herein, "experience" affects the projection of quantum objects onto the PView of the HSS. And when a quantum object is in the PView, a stimulus (e.g., a boson-boson interaction) can sufficiently increase the probability of a particular channel, beyond the previous Feynman equal probability case for all intermediate channels, and thus an "event" (e.g., an observation or measurement) can affect the projection onto a particular state in the DView of the HSS, thereby indicating this increase in probability for a particular desired outcome.

[0063] FIG. 3 illustrates a flow chart for further application of a stimulated transition state 300, according to various examples and embodiments discussed herein.

[0064] In block 310, the transition state (initially including components of the electrolyte) can be stimulated via the Ying cell system. Following the above example, the electrolyte can be deuterium oxide and the stimulated / extracted transition state can be He+γ and / or excess generated energy. The initial and transition states can be manipulated and tuned via modifications to one or more of the power sources, D-source, alpha-source, and gamma-source. In this manner, the various principles and concepts described herein can be used to generate quantities of helium and / or excess generated energy, for example, for extraction or other uses.

[0065] In block 320, the alpha source is removed to control the production of the desired transition state. As described herein, the alpha source is necessary to stimulate the production of the daughter "He+γ and / or excess generated energy." In this manner, a desired or targeted amount can be produced based on application or removal of the alpha source. For example, the alpha source can be removed for a period of time, e.g., to stop the production of a particular transition state, or simply to produce a desired or targeted amount.

[0066] In block 330, the gamma source is removed to control heat production. The gamma source is necessary to generate the "experience" and allow the system to transition from DWF to PView. The "removal" is to reduce heat production. In this manner, a desired or target temperature can be reached based on the application or removal of the gamma source. For example, the gamma source can be removed for a period of time, for example, to stop further production or simply to generate the desired or target temperature of the system.

[0067] In block 340, the temperature can be tracked and the power supply adjusted based on the temperature to produce a target and / or desired amount of a particular transition state component. In various examples, this can initially be state A=D+D, and ultimately the particular transition state component for extraction, e.g., "helium or gamma and / or excess energy produced."

[0068] Any combination of application or removal of one or more of the D source, alpha source, gamma source, and power sources can be implemented to achieve a particular transition state and / or a desired amount of a particular transition state component. In various examples, one or more of the sources can be applied or removed for a period of time to stimulate a desired state. One or more of the state components can be extracted and applied in any of a variety of applications and combinations.

[0069] Aspects The following aspects are illustrative only and do not limit the scope of the disclosure or the appended claims.

[0070] Aspect 1. A system for stimulating production of a transition state component and / or extracting a transition state component, comprising: a sealable container containing an electrolyte; an anode connected to the sealable container; a cathode connected to the sealable container; a power source connected to the anode and the cathode; an alpha source disposed within the sealable container; a gamma source disposed outside or inside the sealable container; a Faraday cage comprising the sealable container; an insulating container comprising the Faraday cage and the sealable container; and a first pair of thermocouples disposed within the Faraday cage and a second pair of thermocouples disposed outside the sealable container.

[0071] Embodiment 2. The system of embodiment 1, wherein the anode is a platinum rod and the cathode is a palladium foil.

[0072] Aspect 3. The system according to any one of aspects 1 to 2, wherein the power source is a reversible 15 V DC power source.

[0073] Aspect 4. Gamma power supply 60 The system according to any one of aspects 1 to 3, wherein the system is a Co disc.

[0074] Aspect 5. 60 The system of embodiment 4, wherein the Co disc is a 1 microCurie disc.

[0075] Aspect 6. Alpha Source 210 The system according to any one of embodiments 1 to 5, wherein the system is a Po disk.

[0076] Aspect 7. 210 The system of embodiment 6, wherein the Po disc is a 0.1 microCurie disc.

[0077] Aspect 8. The system described in any of aspects 1 to 7, further comprising a second pair of thermocouples disposed within the insulating container and outside the Faraday cage.

[0078] Embodiment 9. The system of any one of embodiments 1 to 8, wherein the electrolyte is deuterium oxide.

[0079] Aspect 10. A method of stimulating production of helium and / or excess generated energy via the system of aspect 1, comprising providing deuterium oxide in a sealable container, electrolyzing the deuterium oxide via a power source to generate / provide D+D in a Pd cathode, providing a pathway to transition the system from DWF to PView, and stimulating extraction of one or more of the desired intermediate transition channel states including helium+γ and / or excess generated energy in the PView.

[0080] Aspect 11. The method of aspect 10, further comprising the step of applying a reverse voltage to the sealable container, the cathode and the anode to "clean and reenergize" the system to stimulate at least one of the transition of deuterium oxide to helium + gamma, or excess generated energy.

[0081] Embodiment 12. The method of any of embodiments 10-11, further comprising removing the alpha source to stop transitions of deuterium oxide to D+D, helium+γ, and / or excess generated energy.

[0082] Embodiment 13. The method of any of embodiments 10-12, further comprising removing the gamma source to stop heat production.

[0083] Aspect 14. The method of any of aspects 1-13, further comprising tracking a temperature via said pair of thermocouples, and adjusting said power source based on said temperature to stimulate a target amount of helium and / or excess generated energy for extraction.

[0084] Embodiment 15. The method of any one of embodiments 10 to 15, wherein the electrolysis of deuterium is carried out for a period of time.

[0085] Embodiment 16. The method of any of embodiments 10 to 16, further comprising extracting helium and excess produced energy from the system.

Claims

1. 1. A system for stimulating the production of transition state components and / or extracting transition state components, comprising: a sealable container containing an electrolyte; an anode connected to the sealable container; a cathode connected to the sealable container; a power supply connected to the anode and the cathode; an alpha source disposed within the sealable enclosure; a gamma source located outside or inside the sealable container; a Faraday cage containing the sealable container; an insulating container containing the Faraday cage and the sealable container; a first pair of thermocouples positioned at different heights within the Faraday cage and a second pair of thermocouples positioned outside the sealable enclosure; the power supply adjusts power to the anode and the cathode based on temperatures measured from at least one of the first pair of thermocouples and the second pair of thermocouples to maintain a target temperature for stimulating energy production from the electrolyte; The system wherein the alpha source and the gamma source are removable to control heat production and maintain the target temperature.

2. 10. The system of claim 1, wherein the anode is a platinum rod and the cathode is a palladium foil.

3. 10. The system of claim 1, wherein the power supply is a reversible 15V DC power supply.

4. The gamma power supply ６０ 10. The system of claim 1, wherein the disk is a Co disk.

5. The aforementioned ６０ 5. The system of claim 4, wherein the Co disk is a 1 microcurie disk.

6. the alpha source ２１０ The system of claim 1, wherein the system is a Po disk.

7. The aforementioned ２１０ 7. The system of claim 6, wherein the Po disk is a 0.1 microCurie disk.

8. The system of claim 1 further comprising a second pair of thermocouples disposed within the insulating enclosure and outside the Faraday cage.

9. The system of claim 1 , wherein the electrolyte is deuterium oxide.

10. 10. A method of stimulating the production of helium and / or excess produced energy via the system of claim 1, comprising: providing deuterium oxide into the sealable container; Electrolyzing the deuterium oxide in the Pd cathode via the power source to produce D+D; and / or providing a pathway for transitioning the system from the DView to the PView, and stimulating extraction within the PView of one or more desired intermediate transition channel states including helium + γ and excess generated energy; A method having the following.

11. 11. The method of claim 10, The method further comprises applying a reverse voltage to the sealable container, the cathode, and the anode, "purifying and reenergizing" the system so as to re-stimulate at least one of the deuterium oxide to helium + gamma transition or excess generated energy.

12. 11. The method of claim 10, The method further comprising removing the alpha source to stop the deuterium oxide transitions to D+D, helium+γ, and / or excess generated energy.

13. 11. The method of claim 10, The method further comprising removing the gamma source to stop the production of heat.

14. 11. The method of claim 10, tracking temperature via the pair of thermocouples; adjusting the power supply based on the temperature to stimulate a target amount of helium for extraction and / or excess energy generation; The method further comprises:

15. 11. The method of claim 10, wherein the electrolysis of the deuterium oxide is carried out for a period of time.

16. The method of claim 10 further comprising extracting helium and excess generated energy from the system.

17. A method of stimulating the production of helium and / or excess generated energy via the system of claim 1, the method comprising: Electrolyzing the electrolyte in the Pd cathode via the power source; stimulating at least one of helium plus gamma and excess energy with the alpha source; transitioning the system from DView to PView with the gamma ray source; extracting one or more desired intermediate transition channels while in said PView; A method comprising:

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