Method and system to modify radioactive material

Abstract

A method and system is disclosed which includes irradiating a radioactive substrate having a first atomic composition with a physics spin isolated electromagnetic energy beam at a wavelength, an intensity, an integer energy level, a temperature, and for a period of time sufficient to change at least a portion of the first atomic composition into a second atomic composition over a period of time less than would occur at a natural rate of radioactive decay of the first atomic composition.

Description

PATENT APPLICATION FOR:INVENTOREric Arno VigenATTORNEY DOCKET NUMBER: VIGEN-0018 WOCOOPER & Assoc.4149 Pirates Bch, Ste 115 Galveston, TX 77554 (409) 996-9266Method and System to Modify Radioactive MaterialFIELD

[0001] Embodiments of the present disclosure generally relate to the treatment of radioactive material. More specifically, to the irradiation of radioactive material to modify and change the elemental composition of the material.BACKGROUND

[0002] Nuclear industry accumulated waste is a huge problem, especially in the United States where the reprocessing of spent fuel rods from light water reactors is not currently allowed. Certain atomic isotopes have commercial value for potential power generation, but nuclear wastes currently have residual radioactivity levels that constitute a potential hazard that may last for centuries.

[0003] According to theory presented in this patent, nuclear energy and the radioactivity of the waste are based on a high level of the net of radial electrostatic (rES) energy and other forces trapped in the nucleus of large elements most often commercially with atomic numbers greater than 83.

[0004] There is a need in the art to modify and change the elemental composition of radioactive material to reduce the residual radioactivity levels of the material over a shorter time period than that required by natural processes.SUMMARY

[0005] In embodiments, a method comprises irradiating a radioactive substrate having a first atomic composition with a physics spin isolated electromagnetic energy beam at a wavelength, an intensity, an integer energy level, a temperature, and for a period of time sufficient to change at least a portion of the first atomic composition into a second atomic composition over a period of time less than would occur at a natural rate of radioactive decay of the first atomic composition.

[0006] In embodiments, a system comprises a physics spin isolated electromagnetic energy beam source configured to irradiate a radioactive substrate having a first atomic composition at a wavelength, an intensity, a temperature, and for a period of time sufficient to change at least a portion of the first atomic composition into a second atomic composition over a period of time less than would occur at a natural rate of radioactive decay of the first atomic composition.BRIEF DESCRIPTION OF THE DRAWINGS

[0007] Embodiments of the present disclosure, briefly summarized above and discussed in greater detail below, can be understood by reference to the illustrative embodiments of the disclosure depicted in the appended drawings. However, the appended drawings illustrate only typical embodiments of the disclosure and are therefore not to be considered limiting of scope, for the disclosure may admit to other equally effective embodiments.

[0008] FIG. 1 depicts a stable nucleus of an atom according to the Hemichem model.

[0009] FIG. 2 depicts the calculation of nuclear force required to remove a proton from a stable nucleus of an atom according to embodiments disclosed herein.

[0010] FIG. 3 depicts a radioactive nucleus of an atom having an exterior nuclear structure according to embodiments disclosed herein..

[0011] FIG. 4 depicts a radioactive nucleus of an atom having an exterior nuclear structure interacting with a physics spin isolated electromagnetic energy beam according to the Hemichem model and embodiments disclosed herein.

[0012] FIG. 5 depicts the effects of a radioactive nucleus of an atom having an exterior nuclear structure interacting with a physics spin isolated electromagnetic energy beam according to the Hemichem model and embodiments disclosed herein.

[0013] FIG. 6 depicts a calculation of the required wavelength of a physics spin isolated electromagnetic energy beam for an uranium atom according to the Hemichem model and embodiments disclosed herein.

[0014] FIG. 7 depicts a modified double / single slit filter to produce a physics spin isolated electromagnetic energy beam according to embodiments disclosed herein.

[0015] FIG. 8 depicts a modified Stern Gerlach filter to produce a physics spin isolated electromagnetic energy beam according to embodiments disclosed herein.

[0016] FIG. 9 depicts a modified Aharonov Bohm filter to produce a physics spin isolated electromagnetic energy beam according to embodiments disclosed herein.

[0017] FIG. 10 depicts a physics spin isolated electromagnetic energy beam according to embodiments disclosed herein.

[0018] To facilitate understanding, identical reference numerals have been used, where possible, to designate identical elements that are common to the figures. The figures are not drawn to scale and may be simplified for clarity. Elements and features of one embodiment may be beneficially incorporated in other embodiments without further recitation.DETAILED DESCRIPTION

[0019] Embodiments disclosed herein include reference to a hemispherical model, referred to herein as a Hemichem model, which provides physical modelling of the underlying chemistry and subatomic physics using hemispherical coordinates (rz,0z,az,zz=XO=±1 / 2), replacing quantum numbers (n,l,mi,ms). The hemispherical model further utilizes acceleration allocation (aa) always at the system center-of-mass, thereby replacing Newton’s 2nd Law of Motion wherein three core interactions are utilized to generate the fundamental forces, including full integration of gravity.

[0020] For purposes herein, elementary particles are considered to be elementary- event sets of multiple core particles, arranged in three dimensional (3D) engineering stable structures. The Hemichem model provides 3D engineering physical arrangement, along with causation of quantum equations in terms of classical physical understanding and calculations. Current quantum mechanical analysis is based on statistical techniques which remain valid for multiple particles and multiple events. However, current quantum mechanical analysis cannot describe a single event or particle. In contrast, the Hemichem model utilized herein provides a means of obtaining information in terms of 3D engineering of quantum equations known in the art by incorporating an additional frame-of-reference. Various known dilemmas, such as improper infinities and the like are resolved by the Hemichem model, rendering statistical quantum techniques redundant.

[0021] However, the Hemichem method referred to herein does not detract from, and is in overall agreement with the multitude of information readily known to one of skill in the art of quantum mechanics (QM), quantum field theory (QFT), and the like. The Hemichem method utilized herein presents revisions to known relationships which bridge classical single particle-particle events-sets with the multiple-event quantum prediction techniques and experimental evidence.

[0022] A detailed description of the methods and models utilized herein, including the HemiChem model and the application thereof, may be found in the HemiChem IDS series including Vigen, A. (4-17-2024). Hemispherical Atomic Model ISBN 9798870681290, Vigen, A. (12-23-2023). The Nature and Causation of Light, Photons, and EM Waves Amazon-ASIN B0CQWN1 NT4; Vigen, A. (3-1 -2024). First Principles for Subatomic Physics Amazon-ASIN: B0CWTYVX7Q; and the like. Additional references include Vigen, A. (1 -28-2023). HemiQuantum Physics: Resolving Each Quantum Dilemma: Improving Each Quantum Technique from Planck’s Equation to Elementary Particles, Amazon-ASIN B0BTC7PGND; Vigen, A. (1 -19-2019). Understanding Pauli’s1Z> as 3D Hemispheres Fully Links Quantum Theory to Classical Physics, Amazon-ASIN B07MYNTPJ7; Vigen, A. (1 -18-2019). Simple Words to Fully Reconcile Classical Mechanics with Quantum Theory, Amazon-ASIN B07MY9CH4F; Vigen, A. (4-25- 2022). Refining the Schrodinger Wave Function Equation in Hemispherical (r,0,(p,z=XO=±1 / 2) Coordinates Amazon-ASIN B09YWSL1 FR; Vigen, A (10-12- 2016). Gravity is Just That Electrons are a Little Closer; Amazon-ASIN B01 M9B4V4E; Vigen. A (10-13-2016). Electron Shell Chemistry is Just Scrunched Cube Geometry; Amazon-ASIN B01 M7PRGWZ; Vigen. A (1 -19-2019). Revising Planck-Einstein Energy Equation to Add Pauli’s1 / 2 Fully Links Quantum Theory to Classical Physics; Amazon- ASIN(B07MYLTJ67); Vigen. A (1 -18-2018). Postulated Nucleostaticmagnetics Force for Subatomic Particles Resolves Dirac’s 1931 Monopoles as Fully Deterministic Duopoles; Amazon-ASIN B07MY7F289; Vigen. A (3-25-2023).The Mass Equation: My Breakthrough Position-in-Field Approach from Hemispherical (r,6,(p,z=X0=±1 / 2); Amazon- ASIN B0BZN3MGNC; Vigen A. (10-2-2020). Replacement of Bohr’s Angular Momentum with Strong Nuclear Force for Electrons; Amazon-ASIN B08KNMVPB1 ; Vigen, A (6-20- 2020). Nucleostaticmagnetics Vector Equations; Amazon-ASIN B08BKW46GG; Vigen,A. (3-2-2020). Math Integrity Understanding Strong and Weak Force Through the Forces I Fields of Electrostatic, Direct and Axial Nucleostaticmagnetics: 4-Vector in 3D Model Generating Four Quantum Equations (Dirac); Amazon-ASIN B085R99M44; Vigen, A. (1 - 18-2020). Renaissance Physics: Understanding Post-Quantum Novo-Classical Subatomic Particle Engineering Textbook Chapter 1 -4 Amazon ISBN 1659185777; Vigen, A. (3-31 -2019). 3D Visual Chemistry Textbook; Amazon-ASIN B07Q3PY8GV; Vigen, A. (1 -18-2018). Quantum Entanglement, Wave Functions, and Spectrum Given the 3D Arno Vigen Scrunched Cube (AVSC) Atomic Model; Amazon-ASIN B07MY7Y5ZW; Vigen, A. (10-8-2017). Fixing Einstein’s E=mc-squared: Replacing Observed Mass (‘m’) with the ‘M’ Nucleus Magnetic Force Divided by the Volume of the Electron Shell Radius Separation; Amazon-ASIN B0769ZJK9K; Vigen, A. (10-29-2016). Why Does a Nucleus Stay Together When Protons (+) Repel Each Other?: A Nucleus is Just . . . a Magnetic Chain-Ring; Amazon-ASIN B01 M73KXNQ; The full disclosures of each are fully incorporated by reference herein.

[0023] As used herein, radial electrostatic (rES) interaction I force refers to an electrostatic (ES) attribute often referred to as charge in the prior art, having an appropriate sign of positive (+) or negative (-) or zero for neutrons. The operating rules associated with radial electrostatic (rES) interaction is that opposites attract and like-kind repel with no interaction when the value is zero (0).

[0024] Xtrastatic (XS) axis refers to the magnetic axis inherent in every subatomic particle according to the Hemichem model. Axial xtrastatic interaction and / or force refers to the attractive force from a particle (P1 ), or more specifically from its two hemispheres I poles, towards the axis of a second particle (P2). The sign of the interaction being based upon the XS-attribute known as mass in prior art. The operating rules associated with xtrastatic (XS) interaction as like kind zero and difference generating two force vectors rXS isotropic repulsive with aXS as anisotropic attribute to the axis of the other particleset. These also split between portions as linear towards-the-axis and portions as rotational of the axis itself.

[0025] Radial xtrastatic interaction and / or force refers to the repulsive force from a particle (P1 ) from its two differentiated axes / hemispheres away from a second particle(P2). This sign of this interaction is based upon the XS-attribute also referred to as mass according to common understanding in the art.

[0026] In addition, it is understood that like-kind particles do not have xtrastatic interactions. Only the electron-proton, and the electron-nucleon have xtrastatic interactions.

[0027] For purposes herein, consistent with the Hemichem model, particle-edge and maximum field strength occurs at a particle’s physical dimension radius, which corresponds to the Bohr radius, abbreviated herein as (a0). Accordingly, for purposes herein, a proton is assumed to have a radius and position-in-field maximum at (re).

[0028] For purposes herein, calculation of the behavior of each hemisphere is defined from a pole to an equator of the hemisphere by the inherent XS axis over the body of the particle. The body of the particle having a center-of-substance defined in hemispherical coordinates (rz,0z, )z,Zz=XO=±1 / 2) as ((3 / 8)rz,0,0,+1 / 2) for a first hemisphere, and ( (3 / 8) rz,0, 0,- / 2) for the other second hemisphere, which is locked-at-180° relative to the first hemisphere.

[0029] As used herein, radial electrostatic force - (rES) - refers to the interaction between protons and electron based upon the charge attribute with the product as the interactions. Accordingly, “opposites attract” and “like-kind repel” based upon the following table wherein neutrons do not experience interactions with either a proton or an electron.

[0030] Table 1 depicts the interactions for subatomic particles for radial electrostatic (rES) interactions.

[0031] For the radial electrostatic (rES) interactions, the logic table for types is based upon the product of the signs. The rES ‘charge’ attributes are as follows: Proton = (+1 ); Neutrons = 0; and Electrons = (-1 ); which are shown in the Table 1 :TABLE 1 OF ELECTROSTATIC CHARGE INTERACTIONSProton (+) Neutron (0) Electrons (-)wherein the xtrastastic, pre-magnetism subatomic force, the interaction logic table is based upon two force vectors:i) Radial xtrastatic, the outward ‘at the equator; and ii) Axial xtrastatic, the inward towards-the-axis.

[0032] These operate by ‘like-kind zero’ and both operating in different directions with an overall sign opposite to rES. That is the formula is (SIGN)(product) wherein both protons and neutrons have this ‘mass’ attribute as (+1 ).

[0033] For the XS ‘mass’ attribute the assigned attributes are:Proton = (+1 ), Neutrons = (+1 ) and Electrons = (-1 ), wherein the radial xtrastatic (rXS), using sign = (-1 ), is shown in Table 2:TABLE 2 OF XTRASTATI C CH ARG E I NTE RACTIONSProton (+) Neutron (0) Electrons (-)PROTON same = (0) same = (0) (-)((+)(-)) = (+) NEUTRON same = (0) same = (0) (-)((+)(-)) = (+) ELECTRONS (-)((+)(-)) = (+) (-)((+)(-)) = (+) same = (0)Axial xtrastatic (aXR) (using sign = (+1 )) as shown in Table 3:TAB LE 3 OF N U C L EOSTATI C CHARGE I NTE RACTI O N SProton (+) Neutron (0) Electrons (-)PROTON same = (0) same = (0) (+)((+)(-)) = (-) NEUTRON same = (0) same = (0) (+)((+)(-)) = (-) ELECTRONS (+)((+)(-)) = (-) (+)((+)(-)) = (-) same = (0)

[0034] The combination two static force vectors of the axial xtrastatic force is out- at-equator, inward-towards-axis of pre-magnetism, and the electron subshells, which relates to the inclination ring-spring physics underlying Bose proof of quantum mechanics (QM).

[0035] Elemental Ionization Energy - (Ei,N) refers to the energy to remove an electron of a chosen element and molecular state. For example, the energy required to remove an electron from a hydrogen atom to isolate a proton, wherein N = 1 for hydrogen.

[0036] Molecular Ionization Energy - (Ei,AB-) refers to the energy to remove an electron of a chosen elements and molecular state. For example, the energy required to ionize water to produce a hydronium or hydrogen ion (H2O)+. In this example, the AB notation above is H2O.

[0037] As used herein, a physics spin isolated electromagnetic energy beam, also referred to simply as a spin isolated electromagnetic energy beam, refers to amonochromatic electromagnetic beam consisting essentially of a plurality of physics spin isolated photons, wherein the physics spin isolated photons are only observable within a plurality of first discrete ranges along a path of the monochromatic electromagnetic beam, each of the first discrete ranges centered at a corresponding distance from a source of the monochromatic electromagnetic beam, wherein essentially no photons are observable within a plurality of second discrete ranges located in-between each of the first discrete ranges, as described in the Applicant’s corresponding US Patent Application No. 18 / 674,995, filed May 27, 2024, the disclosure of which is incorporated by reference herein.

[0038] As used herein, a natural rate of radioactive decay of an atomic composition refers to the generally accepted rate of decay for a particular element, typically referred to as a half-life, determined according to the equation:wherein:N(t) is the quantity of the substance remaining;No is the initial quantity of the substance; t is the time elapsed; and ti / 2 is the half life of the substance which is a accepted, fixed value for every Element.

[0039] For example, the accepted half-life of238U is 4.51 x 109years, wherein the atomic composition decays along the following decay chain to206Pb: 238U^234Th^234pa^234U^230Th^226Ra^222Fin^218po^214pb^214Bi^214po^210pb^ 210Bj^210po^206pb (stab|e)

[0040] An example, according to embodiments disclosed herein, of changing a portion of a substrate wherein the first atomic composition has a particular amount of238U, into a second atomic composition over a period of time which is less than would occur at a natural rate of radioactive decay of the first atomic composition, would result in the same portion of the substrate having less238U over that period of time than would be predicted according to the half-life of238U. However, unless otherwise indicated, the second atomiccomposition is not necessarily the end stable element e.g.,238U -^206Pb, but may be any intermediate decay product in the decay chain of the particular element.

[0041] In embodiments, a method of accelerating a radioactive decay rate of a radioactive substrate material, comprises irradiating a radioactive substrate having a first atomic composition with a monochromatic physics spin isolated electromagnetic energy beam at a wavelength, an intensity, an integer energy level, a temperature (within a temperature range),, and for a period of time sufficient to change at least a portion of the first atomic composition into a second atomic composition over a period of time less than would occur at a natural rate of radioactive decay of the first atomic composition.

[0042] In embodiments, the wavelength (A) is determined from formula I:A = RE,Q# (1 / (Ni)2- 1 / (N2)2) (I); wherein: A is a wavelength of the physics spin isolated monochromatic electromagnetic beam; 0# is a second quantum number of the subshell of an electron of an atom of element E of the source of the electromagnetic beam, RE,O# is a Rydberg constant for the subshell of the electron of the atom of the element E of the source of the electromagnetic beam; Nx is an integer subset energy level starting at x=1 determined by formula (II) Nx+i = Nx +1 (II); wherein each N and x are determined independently, as integers greater than or equal to 1 ; and wherein RE,O# is determined by formula (III):RE,S# = 6re((DeN / (6 re))2-1 ) (III); wherein: reis the radius of an electron; DeN is a distance between a center of a nucleus and a center of an electron of the atom of the source of the electromagnetic beam. In embodiments, |Ni- N2| > 6.

[0043] In embodiments, the irradiation of the radioactive substrate with the physics spin isolated electromagnetic energy beam comprises delivering the physics spin isolated electromagnetic energy beam to a plurality of locations, each of the plurality of locations positioned an incremental distance apart, based on a starting position, wherein the incremental distance is less than one wavelength of the physics spin isolated electromagnetic energy beam.

[0044] In embodiments, the irradiation of the substrate with the physics spin isolated electromagnetic energy beam in pulsed on for a first period of time, followed byoff for a recovery period of time sufficient to allow equilibration of a subatomic particle B- field. In embodiments, both the recovery period of time Trand the incremental distance Di are determined by:Tr = (DeN / C) / NxDi = (DeN ) / Nx wherein DeN is the distance between an electron and a nucleus of a target atom; c is the speed of light; and Nxis the integer energy level of photons of the physics spin isolated electromagnetic energy beam, wherein Nx is a larger of a value determined by (1 / Ni)2- ( N2)2, and wherein N1 is a starting integer energy level and N2 is an ending integer energy level of the nucleus of the target atom. In embodiments, Di is greater than or equal to about 3 / 8*re, wherein reis a radius of an electron equal to 2.8179*1015m.

[0045] In embodiments, the physics spin isolated electromagnetic energy beam is polarized.

[0046] In embodiments, the physics spin isolated electromagnetic energy beam is produced using a modified double slit / single slit filter comprising a single slit from which the physics spin isolated electromagnetic energy beam is produced, positioned within an interference pattern produced by a double slit.

[0047] In embodiments, the physics spin isolated electromagnetic energy beam is produced using a modified Stern Gerlach filter.

[0048] In embodiments, the physics spin isolated electromagnetic energy beam is produced using a modified Aharonov Bohm filter.

[0049] In embodiments, the radioactive substrate having the first atomic composition comprises a naturally occurring radioactive material, a spent radioactive waste material, an intermediate radioactive fuel material, and / or a radioactive fuel material.

[0050] In embodiments, the second atomic composition is essentially nonradioactive.

[0051] In embodiments, the irradiating of the radioactive substrate with a physics spin isolated electromagnetic energy beam comprises changing a distance between a source of the electromagnetic energy beam and the substrate over a range configured toirradiate the portion of the substrate at intervals of greater than or equal to about 3 / 8 re, wherein reis a radius of an electron equal to about 2.8179*10-15m.

[0052] In embodiments, the radioactive substrate is disposed within a magnetic field sufficient to orient at least a portion of an xtrastatic axis of the atoms with the magnetic field, wherein the magnetic field is oriented essentially perpendicular to a direction of the monochromatic physics spin isolated electromagnetic energy beam.

[0053] In embodiments, the radioactive substrate is disposed between two electrodes having a difference in electric potential sufficient to produce an electrostatic field sufficient to orient at least a portion of the xtrastatic axis of the atoms with the electrostatic field, wherein the electrostatic field is oriented essentially perpendicular to a direction of the monochromatic physics spin isolated electromagnetic energy beam.

[0054] In embodiments, the radioactive substrate is disposed between two electrodes having a difference in electric potential sufficient to produce an electrostatic field sufficient to orient at least a portion of the xtrastatic axis of the atoms with the electrostatic field, wherein the electrostatic field is oriented essentially perpendicular to a direction of the monochromatic physics spin isolated electromagnetic energy beam; and a magnetic field sufficient to orient at least a portion of the xtrastatic axis of the atoms with the magnetic field, wherein the magnetic field is oriented essentially perpendicular to a direction of the monochromatic physics spin isolated electromagnetic energy beam.

[0055] In embodiments, a system comprises a monochromatic physics spin isolated electromagnetic energy beam source configured to irradiate a radioactive substrate having a first atomic composition at a wavelength, an intensity, a temperature, and for a period of time sufficient to change at least a portion of the first atomic composition into a second atomic composition over a period of time less than would occur at a natural rate of radioactive decay of the first atomic composition.

[0056] In embodiments, the system is configured to irradiate the radioactive substrate with a physics spin isolated electromagnetic energy beam at a plurality of distances between a source of the electromagnetic energy beam and the substrate over a range configured to irradiate the portion of the substrate at intervals of at a minimum spacing of about 3 / 8 re, wherein reis a radius of an electron equal to 2.8179*1015m anda maximum sequence spacing and a maximum interval of intervals less than the chosen wavelength which has ranges from 10-14to 1 O05m.

[0057] In embodiments, the system further comprises a source of a magnetic field oriented about at least a portion of the radioactive substrate, configured to produce a magnetic field sufficient to orient at least a portion of an xtrastatic axis of atoms present within the radioactive substrate with the magnetic field, wherein the magnetic field is oriented essentially perpendicular to a direction of the monochromatic physics spin isolated electromagnetic energy beam; further comprising two electrodes oriented about at least a portion of the radioactive substrate, having a difference in electric potential sufficient to produce an electrostatic field sufficient to orient at least a portion of the xtrastatic axis of the atoms with the electrostatic field, wherein the electrostatic field is oriented essentially perpendicular to a direction of the monochromatic physics spin isolated electromagnetic energy beam; or a combination thereof.

[0058] In embodiments, the radioactive substrate is a free flowing material flowing through a treatment cell in which the physics spin isolated electromagnetic energy beam source is directed into contact with the radioactive substrate.

[0059] FIG. 1 depicts a nucleus (101 ) for a non-radioactive element having multiple protons (102, 104). The protons repel each other by radial electrostatic (rES) force (105). However, when a neutron (103) having a structure, based upon the strong nuclear force, overcomes the proton to proton rES force 105 to keep the nucleus with multiple protons together as a unit. Specifically, the neutron is both a separator and binds by strong nuclear force between proton and neutron more than the p-p rES force 105. There is always at least one neutron for and between every proton pair. In larger elements, more neutrons than protons are required to maintain a stable structure.

[0060] As depicted in FIG. 2, the net forces between subatomic particles are the combination of rES with basic strength from Planck’s constant version (hca) for 1 / distance-squared offset the ‘extra 1 / r’ counter force which finds equilibrium at the Bohr- H radius (ao), wherein Planck’s constant per particle is used, not per kilogram. As a result, we have the fixed (hca) for 1 / d2for (1 +d / ao). However, that calculation is moving the particle to 2d, the protons touching. At that point, the (re / aO) ratio becomes material to both segments. That would be (18,778 / 2) = (9,389) or for the (-1 ) segment (9,388). Assuch, the rES absorbed by strong nuclear forces is (9,389)(9,389)(9,388) = 827 million stronger than the typical electron-proton Hydrogen strength. Further, that interaction proton-proton rES is repulsive.

[0061] FIG. 3 depicts a radioactive nucleus having exterior nuclear structure 312 comprising weakly held protons and neutrons outside of the core nucleus structure (301 ) wherein neutrons (303) (only one is shown for clarity) are disposed between protons (302, 304). The more loosely held protons (306 and 308), and neutrons (305 and 307) are present within the extension structures. In addition, the element may include different exterior sets e.g., proton 310 and two neutrons 309 and 311 . The inventor has observed that radioactive elements have multiple excess particle-sets of weakly held nuclear particles.

[0062] Radioactivity is the decay of these exterior structures that are excess and are weakly held. Non-radioactivity is when the nucleus structure has little or no weak stability exterior protons, which occurs below 209 atomic weight. Separation, usually by p-p rES repulsion, of the protons present in these exterior structures become the radioactive events present during radioactive decay via these protons repelling one- another to eject the proton form the nucleus structure.

[0063] In embodiments, a spacing between two or more of these external protons are manipulated by interaction with a physics spin isolated electromagnetic energy beam which results in the movement of the proton an subsequent rejection of the proton via rES repulsion, thereby increasing the conversion rate of the first atomic composition to the second atomic composition over a period of time less than would be required to effect the same transition at a natural rate of radioactive decay of the first atomic composition.

[0064] FIG. 4 depicts the remote electron’s behavior the relative to the structure of the nucleus according to the Hemichem model, wherein the nucleus has a stable nuclear structure 401 and an external nuclear structure 410, which interacts over a distance 403 with an electron 406. That electron 406 has its inherent axis 408 which can rotate. Yet, anisotropic force changing with rotation 404 of the electron 406 causes cycles of linear movements 407 relative to the nucleus structure 401. As the electron 406 rotates 404, linear movement 407 results in rotation of 402 and linear movement 405 of the corresponding nucleus structures 401 and the proton 408 of the external nuclear structure410. Accordingly, inducing rotation and linear acceleration of electron 806 by application of an external force 412 i.e., via irradiating the radioactive substrate having a first atomic composition with a physics spin isolated electromagnetic energy beam at a wavelength, an intensity, an integer energy level, a temperature, and for a period of time, will rotate a particle present in the external structure 408 of the nucleus into a decay position wherein the proton is ejected, thereby sufficient changing at least a portion of the first atomic composition into a second atomic composition over a period of time less than would occur at a natural rate of radioactive decay of the first atomic composition.

[0065] Each electron present in an atom has a base movement and rotation rate specific to each element as adjusted for each molecular configuration. However, the application of 3D engineering according to the Hemichem model to radioactive materials allows for effecting a change in the electron energy level (‘wave’ anisotropic behavior) and related linear acceleration (ring-electron) counter behavior. In embodiments, the wavelength of the physics spin isolated electromagnetic energy beam is selected for the exterior particles of the nucleus by choice of rotation rate intervals of wavelengths at the edge or slightly below the Lamb shift wavelength for the target element. Using energy jumps e.g., 1 / 2 levels of infrared or 2 / 3 or visible light, or higher to produce rotation and / or linear acceleration sufficient to increase the decay cascade for the target nucleus.

[0066] In embodiments, the physics spin isolated electromagnetic energy beam has been isolated for same-polarity, same-spin and is delivered an energy level sufficient to produce a jump of at least nine (9) levels (1 / 9, 2 / 10, 1 / 10, 2 / 1 1 , 2 / 12, and so on), which may involve utilizing ultraviolet light or shorter wavelengths, which are selected for a particular element or elemental composition.

[0067] In embodiments, a slightly shorter wavelength than the Lamb shift is utilized to target the weakly held protons on the exterior. That is at wavelength not as (d)2, but instead calculated as (d2-((6)(2re))2) for a Shell-6 or Shell-7 Element.

[0068] The rotations of the electrons are not continuous. That is because molecules, other than Hydrogen, have multiple electrons organized in subshells sets such that movement results from all the electrons in the subshells. The electrons are generally at the same distance and at the same inclination (longitude) angle relative to the nucleusaxis of symmetry. Only when those electron rotations and ring-electron movements settle into integer units can the nucleus be stable.

[0069] Utilizing the Hemichem model, movement harmonics are in offsetting axial directions. A subshell-hemisphere set of electrons generally settle around a corresponding longitudinal ring relative to the axis of the nucleus. Each electron has a rotational wave and a linear movement dynamic, which is generally spaced evenly at latitudes angles of (2n7# in subshell-hemisphere set, wherein # represents the maximum number of subshells, defined by theta 2nd Quantum number (6z) including the “0” subshell-s as two electrons at zero inclination angle, so on the axis at the two poles. As such, the combination of forces aggregate to zero overall. The electrons travelling near the speed of light thus form the unit based frequency for the nucleus. Yet, when the nucleus is radioactive, it has an exterior structure that which may be manipulated according to embodiments disclosed herein by irradiating the radioactive substrate having a first atomic composition with a physics spin isolated electromagnetic energy beam at a wavelength, an intensity, an integer energy level, a temperature, and for a period of time, using a targeted wavelength with sufficient energy level the lower Lamb shift and slightly beyond chosen specific to each element such that the rate of radioactive decay increases.

[0070] FIG. 5 depicts the nucleus external structure 51 1 in a harmonic coupling with the remote electron 505. There is a stable nucleus structure (501 ) and an electron (505) having a rotation harmonic (506) which also has a linear acceleration harmonic (510) propagating a field which becomes periodic waves for the external structure proton 502 and 507. There exist other weakly held exterior protons 507. Any change in forces for rotation 503 and linear acceleration 504 relayed via linear acceleration harmonic to the weakly-held exterior structure proton 502 results in the distance 509 between the proton 502 and another exterior structure proton 507, such that the radial electrostatic (rES) repulsion becomes overwhelming and the exterior structure proton 502 is ejected as nuclear decay.

[0071] In embodiments, the interaction of the physics spin isolated electromagnetic energy beam with the nucleus external structure increases the rotation rate of the electron, creating a destabilizing rotational and / or linear acceleration on the protons of the nucleus external structure resulting in movement of proton 502 relative to anotherproton 507 which achieves the p-p rES repulsion eject the proton 502 from the nucleus external structure 511 thereby changing the atomic number and thus the atomic composition of the atom and by extension, the substrate in which the atom is located.

[0072] This action is substantially perpendicular to the direction of the strong nuclear force along the exterior structure to the nucleus 501. In embodiments, the wavelength of the physics spin isolated electromagnetic energy beam is selected to be about equal to the overall nucleus to electron distance 508, which is slightly larger than the nucleus-target electron distance 509.

[0073] The overall nucleus to electron distance is calculated based on the three positions which describe the position occupied by the target proton (subatomic particle). The center of the particular particle is applicable to calculate rES. However, the calculation of axial xtrastatic (aXS) forces requires additional calculations involving the angular momentum, Omega elementary particle, magnetic, pre-magnetic and other anisotropic constants of interactions, which may be determined according to two additional positions.

[0074] Utilizing the Hemichem model, a subatomic particle includes a center and two poles. The center-of-structure (mass) for each hemisphere located at (z,r) of ((3 / 8re),0,0) become the effective, estimation for determining the actual position of the electron from the proton, providing a reasonable estimate for the full integral over the entire hemisphere structures. The interaction between the proton and the electron requires a direction of the closer pole of the particular particle with the center of the particular particle, and the vertex defines a relative angle of the two to complete the requirements of the 3D engineering of the Hemichem model.

[0075] Further, variations of structure and count due to the various isotopes present, becomes variance in the wavelength and mass for the various particles by position in the fields of the interacting particles. An example of the calculation for uranium (atomic number 92) is shown in FIG. 6, which is calculated to be about 91 nm. In embodiments, the ranges of wavelengths required are typically in the ultraviolet and higher energy ranges to generate the necessary delivery of rotational energy on the target exterior nucleus structure.

[0076] As these calculations show, the distance of the proton versus neutron is closer by (2re). With two electrons, one present in one hemisphere and the other present in the other hemisphere, produce the effect known as the Lamb shift. The inventor has determined that electrons will always operate with protons that are (d-2re) and (d+2re), and that this combination results in a consistent differentiation of wavelengths based upon the two consistently different distances. Since the proton is not a point but is in-fact a sphere having a radius, the proton interacting with half of the electrons associated with one hemisphere have a slightly shorter interaction distance equal to1 / 2 the proton radius, and thereby the interaction of the closer electrons is characterized by a shorter wavelength than the Bohr-Dirac main line calculation. Likewise, those same protons interacting with electrons, which is generally an equal number, present in the other hemisphere have a slightly longer distance, and thereby are characterized by a slightly longer wavelength than the Bohr-Dirac main line calculation. This results in the observed two spectrum lines of intensity with a fine separation rather than one spectral line.

[0077] In larger atoms, since the target protons of the external structure interact with electrons over 7 layers away from a center of the nucleus on the closer side, the distance calculation required for embodiments disclosed herein results in a wavelength in the range slightly below the lower Lamb Shift wavelength for the particular element.

[0078] The calculation of the wavelength of the physics spin isolated electromagnetic energy beam depends on the number of nucleons (nucleus particles) and requires determining the size of the nuclear structure and the electron shell structure. In embodiments, this calculation utilizes a Rydberg methodology based on the assumption that the volume is consistent per unit using an average radius for X units and the cube-root of (X) applied to the basic unit, i.e., a hydrogen atom. Because rES is isotropic, this cube-root(N) for protons-only was the initial method attempted. This accounts for the ‘extra 1 / r’ counter interaction that is critical to the EM wave process. In very simplified terms, the rES with strength at 1 / d2has a counter interaction at 1 / d3, with an extra 1 / r.

[0079] The spectral lines must be calculated as-if there are two items, protons at 1 X and neutrons at 2X, to arrive at the anisotropic xtrastatic force value. These interactions involve by both protons and neutrons, wherein the neutrons are acombination of protons / electrons held together within in the nuclear structure and are calculated based upon cube-root(Z+2N).

[0080] It is the use of particle-size units (re), that produce the necessary scaling for these calculations to produce useful results. The two basic scaling distances are the Bohr radius (aO), which is where the basic 1 :1 Hydrogen main isotope sets electron versus nucleus distance and Planck’s constant (h) based upon the position-in-field relative to the distance. The inventor has determined that the needed equations apply 1 / (d / ao)2, not the prior art 1 / d2, as in Coulomb’s electrostatic force equation as shown in standard textbooks. Accordingly, the position-in-field scaling must be scaled to a base unit and becomes dimensionless. In addition, determination of the necessary wave harmonics as expressed as the Rydberg constant (R~) is not infinity, but is limited to a lower value, the specific particle size of the electron (re).

[0081] The calculation shown in FIG. 6 is based on electron Pauli pairs (Z / 2). However, each pair is missing the necessary anisotropic, xtrastatic, and pre-magnetism interactions at 1 / d3. As such, the 2nd particle, locked-at-180 degrees becomes 1 / (2d)3= (-1 / 8). As a result, the total strength factor is (1 -1 / 8)=(7 / 8), so the net constant of (7 / 8) must be applied for each of the Pauli-pairs. This factor is inverted as a) the change in distance; the b) reduces the strength to offset, so (7 / 8) strength settles at (8 / 7d), such that the equation for Scaling (S) by Elements (N), SO SN becomes (8 / 7)((N / 2)1 / 3). That is further nuanced with the specific set of outer subshells as hybridization in prior art.

[0082] The physics spin isolated electromagnetic energy beam consists of multiple photons, each having isolation of physics-spin such that essentially all the photons arriving at the target have the same direction i.e., either up or down. The physics spin isolated electromagnetic energy beam is arranged such that only one of the two beams hits the target. In embodiments, the two physics spin isolated electromagnetic energy beams may be utilized to irradiate different portions of a substrate, or a plurality of substrates.

[0083] In embodiments, the irradiating of the radioactive substrate with a physics spin isolated electromagnetic energy beam comprises changing a distance between a source of the electromagnetic energy beam and the substrate over a range configured to irradiate the portion of the substrate at intervals of greater than or equal to about 3 / 8 Re.

[0084] FIG. 7 depicts a modified twin-single slit filter 700 suitable to produce the physics spin isolated electromagnetic energy beam according to embodiments disclosed herein. In embodiments, monochromatic electromagnetic beams 702A and 702B having a wavelength (A) is produced from a source 728 and directed through two coplanar slits 704 and 706 disposed through a first wave barrier 708. A third slit 710 is disposed through a second barrier 712. A physics spin isolated monochromatic electromagnetic beam 720A produced from the monochromatic electromagnetic beam 702A emanates from third slit 710. Likewise, a physics spin isolated monochromatic electromagnetic beam 720B produced from the monochromatic electromagnetic beam 702B also emanates from third slit 710 along a different path.

[0085] As the monochromatic electromagnetic beams 702A and 702B arrive at the first barrier 708 and pass through the corresponding slits 704 and 706, an interference patter is produced on the second barrier 712 separated from the first barrier 708 by a second distance 714, as is known in the art. However, it is believed that the alternating light band-dark band interference pattern produced on the second barrier 712 is the result of overlapping of the physics spins shown in FIG. 3 and not some wave property of the photons.

[0086] In embodiments, the position of third slit 710 is located within a dark band of the pattern of light and dark bands produced on the second barrier 712. Ostensibly, no photons are present in this region. However, the inventors have discovered that indeed photons are present in this region, they are simply not observable in this region due to interference between different beams, each having a particular spin isolation.

[0087] A first target substrate 718 is located at a target distance 716 from the second barrier 712. The physics spin isolated monochromatic electromagnetic beam 720A has a physics-spin arbitrarily labeled ‘down’ (arrow 722) in this example. The physics spin isolated monochromatic electromagnetic beam 720B has a physics-spin arbitrarily labeled ‘up’ (arrow 724) in this example.

[0088] In embodiments, a plurality of second target substrates 430 (only one of which is shown for simplicity) may be arranged to intersect another physics spin isolated monochromatic electromagnetic beam 720B at a second target distance 716’, which in embodiments may be located at the first target distance 716.

[0089] The physics spin isolated monochromatic electromagnetic beams 720A and 720B each independently consist essentially of a plurality of physics spin isolated photons. These physics spin isolated photons are only observable within a plurality of first discrete ranges along a path of the monochromatic electromagnetic beam, each of the first discrete ranges is centered at a corresponding distance from a source of the monochromatic electromagnetic beam. The physics spin isolated monochromatic electromagnetic beams are further characterized as having a plurality of second discrete ranges located in-between each of the first discrete ranges wherein essentially no photons are observable. Accordingly, only the portion of the target substrate 718 located at the target distance 716 is irradiated with the photons present in the physics spin isolated monochromatic electromagnetic beam at the corresponding first discrete range. Any portion of the first target substrate 718 which is not present within this first discrete range is not irradiated with the photons present in the physics spin isolated monochromatic electromagnetic beam. Accordingly, in embodiments, the target distance 716 may be controlled and / or modified to provide spatial resolution of irradiation or other types of activation on or of the target substrate by the physics spin isolated monochromatic electromagnetic beam.

[0090] In embodiments, the target distance 716 is selected, modified, controlled and / or configured such that photons of the physics spin isolated monochromatic electromagnetic beam 720A irradiate, activate, and / or interact with the portion of the first target substrate to be irradiated, allowing the intended result of that irradiation e.g., photocatalytic curing of a mask, only in the region irradiated.

[0091] It is noted that the prior art use of the terms ‘up’ and ‘down’ to describe spin is misleading. An ‘up’ spin of a physics spin isolated monochromatic electromagnetic beam is more completely described as having an inner-clockwise / outer-counterclockwise spin, and a ‘down’ spin of a physics spin isolated monochromatic electromagnetic beam is more completely described as inner-counterclockwise / outer-clockwise with the center as the same node. Accordingly, consistent with current understanding, photons and EM waves possess dual wave characteristics (See Vigen, A. (12-24-2023). The Nature and Causation of Light Amazon-ASIN B0CQXD14QN).

[0092] Each physics spin isolated monochromatic electromagnetic beam arriving at a barrier will show a pattern of alternating light bands where photons are observable and dark bands in which intermediate positions are interfering where photons are not observable and thus no activation of a substrate brought about by irradiation with photons will occur.

[0093] It is theorized that physics spin isolated monochromatic electromagnetic beams are produced via spin aggregation of the photons, in which both hemispheres of the subatomic particle, in this case the photon, move in the same direction and thus there is no change in the energy-level associated with the photons present in the physics spin isolated monochromatic electromagnetic beam.

[0094] In embodiments, the portion of the substrate to be activated or irradiated by the photons of the physics spin isolated monochromatic electromagnetic beam is located in an activation position, which is coincident with an entanglement node of the physics spin isolated monochromatic electromagnetic beam, where the spin of each photon present is inside one direction and outside the other, resulting in a change in the energylevel for a particular photon, or other subatomic particle i.e., protons and electrons. The rotation energy being the transposition rate of those poles defined by the subatomic particle’s axis, with the resulting change in the B-field for perpendicular magnetism linear acceleration according to relationships known in the art.

[0001] FIG. 8 depicts a modified Stern Gerlach magnetic spin isolation filter 800 suitable to produce the physics spin isolated electromagnetic energy beam, comprising a non- uniform magnetic field 802 disposed between an inlet 826 and an outlet 828 of the magnetic spin isolation filter 800. In embodiments, magnetic spin isolation filter 800 includes a first magnet 804 and a second magnet 806, the first magnet 804 having a first cross section 808 oriented perpendicular to a path of the monochromatic electromagnetic beam 812; the second magnet 806 having a second cross 810 oriented perpendicular to the path of the monochromatic electromagnetic beam 812 produced by a source 834, which is different from the first cross section 808, such that the opening 814 between the two magnets 804 and 806 has a non-uniform magnetic field having a magnetic field strength 832 and length 816 in the direction of the path of the monochromatic electromagnetic beam 812 sufficient to separate the monochromatic electromagneticbeam 812 into a pair of physics spin isolated electromagnetic energy beams 818 and 820. As shown in FIG. 8, at least one of the physics spin isolated electromagnetic energy beams 818 and 820 emanating from the outlet 828 interact with a target substrate 822 and 824 to affect actuation or a change of a portion of the target substrate, as described above.

[0095] In embodiments, the first magnet 804, the second magnet 810, or both are, or include one or more electromagnetic elements 830 configurable to adjust the magnetic field strength 832 one or more points along the path of the monochromatic electromagnetic beam 812.

[0096] FIG. 9 depicts a modified Aharonov Bohm filter 900 suitable to produce the physics spin isolated electromagnetic energy beam, comprising two slits 902 and 04, through which two monochromatic electromagnetic beams 906 and 908 produced by a source 910, pass through striking a substrate 912, wherein the interference pattern produced by the two monochromatic electromagnetic beams 906 and 908 is a physics spin isolated electromagnetic energy beam, produced by interaction with a circular magnetic field 914. The direction of the magnetic field 914 is outward from the figure; the inward returning flux is not shown, but is outside the electron paths. The arrow 914 shows the direction of the field which interacts with the two monochromatic electromagnetic beams 906 and 908.

[0097] FIG. 10 depicts a physics spin isolated monochromatic electromagnetic beam 1000 according to embodiments disclosed herein, consisting essentially of a plurality of physics spin isolated photons depicted as dashes, wherein the physics spin isolated photons are only observable within a plurality of first discrete ranges 1002 along a path of the monochromatic electromagnetic beam 1000, each of the first discrete ranges 1002 is centered at a corresponding distance from a source 1004 of the monochromatic electromagnetic beam, wherein essentially no photons are observable within a plurality of second discrete ranges 1006 located in-between each of the first discrete ranges 1004.

[0098] In embodiments, the first discrete ranges 1002 wherein the physics spin isolated photons are observable, have a length 1008 of greater than or equal to about 0.1 nm. In embodiments, the first discrete ranges wherein the physics spin isolated photons are observable have a length of less than or equal to about 10 nm. In embodiments, anaverage length 1008 of the first discrete ranges is essentially equal to an average length of the second discrete ranges 1010 in which essentially no photons are observable.

[0099] In embodiments, the first discrete ranges 1002 wherein the spin-isolated photons are observable, have a length 1008 of greater than or equal to about 0.1 nm, or greater than or equal to about 1 nm, or greater than or equal to about 10 nm, or less than or equal to about 100 nm.

[0100] In embodiments, a magnetic field is oriented about at least a portion of the radioactive substrate, configured to produce a magnetic field sufficient to orient at least a portion of an xtrastatic axis of atoms present within the radioactive substrate with the magnetic field. In embodiments, the magnetic field may be produced by placing the substrate between the two poles of one or more permanent magnets, and / or electromagnets. In embodiments, the orientation of the magnetic field may be oriented at an angle from about 5° to about 90° relative to the orientation of the monochromatic physics spin isolated electromagnetic energy beam. In embodiments, the magnetic field is oriented essentially perpendicular to a direction of the monochromatic physics spin isolated electromagnetic energy beam.

[0101] In embodiments, two electrodes are oriented about at least a portion of the radioactive substrate, the two electrodes being in electrical communication with a power supply sufficient to produce a voltage therebetween having a difference in electric potential sufficient to produce an electrostatic field between the two electrodes which is sufficient to orient at least a portion of the xtrastatic axis of the atoms present within the radioactive substrate with the electrostatic field. In embodiments, the orientation of the electrostatic field may be oriented at an angle from about 5° to about 90° relative to the orientation of the monochromatic physics spin isolated electromagnetic energy beam. In embodiments, the electrostatic field is oriented essentially perpendicular to a direction of the monochromatic physics spin isolated electromagnetic energy beam.

[0102] In embodiments, the radioactive substrate is disposed within both a magnetic field and an electrostatic field, both of which are oriented essentially perpendicular to a direction or orientation of the monochromatic physics spin isolated electromagnetic energy beam directed to contact the radioactive substrate.

[0103] In embodiments, the radioactive substrate is a free flowing material, which in embodiments is a molten salt, e.g., in a thorium reactor to increase a degradation of protactinium formed in a molten salt reactor, to a flowing through a treatment cell through which the physics spin isolated electromagnetic energy beam source is directed into contact with the radioactive substrate. In embodiments, the treatment cell further includes a source of a magnetic field oriented about at least a portion of the radioactive substrate, configured to produce a magnetic field sufficient to orient at least a portion of an xtrastatic axis of atoms present within the radioactive substrate with the magnetic field, and / or two electrodes oriented about at least a portion of the radioactive substrate, the two electrodes being in electrical communication with a power supply sufficient to produce a voltage therebetween having a difference in electric potential sufficient to produce an electrostatic field between the two electrodes which is sufficient to orient at least a portion of the xtrastatic axis of the atoms present within the radioactive substrate with the electrostatic field.

[0104] While the foregoing is directed to embodiments of the present disclosure, other and further embodiments of the disclosure may be devised without departing from the basic scope thereof.

Claims

Claims1 . A method comprising: irradiating a radioactive substrate having a first atomic composition with a monochromatic physics spin isolated electromagnetic energy beam at a wavelength, an intensity, an integer energy level, a temperature, and for a period of time sufficient to change at least a portion of the first atomic composition into a second atomic composition over a period of time less than would occur at a natural rate of radioactive decay of the first atomic composition.

2. The method of claim 1 , wherein the wavelength (A) is determined from formula I:A = RE,Q# (1 / (Ni)2- 1 / (N2)2) (I); wherein:A is a wavelength of the physics spin isolated monochromatic electromagnetic beam;Q# is a second quantum number of the subshell of an electron of an atom of element E of a source of the electromagnetic beam,RE,©# is a Rydberg constant for the subshell of the electron of the atom of the element E of the source of the electromagnetic beam;Nx is an integer subset energy level starting at x=1 determined by formula (II)Nx+i = Nx +1 (II); wherein each N and x are determined independently, as integers greater than or equal to 1 ; and wherein RE,©# is determined by formula (III):RE,©# = 6re((DeN / (6 re))2-1 ) (III); wherein: reis the radius of an electron;DeN is a distance between a center of a nucleus and a center of an electron of the atom of the source of the electromagnetic beam.

3. The method of claim 2, wherein |Ni - N2| > 6.

4. The method of claim 1 , where the irradiation of the radioactive substrate with the physics spin isolated electromagnetic energy beam comprises delivering the physics spin isolated electromagnetic energy beam to a plurality of locations, each of the plurality of locations positioned an incremental distance apart, based on a starting position, wherein the incremental distance is less than one wavelength of the physics spin isolated electromagnetic energy beam.

5. The method of claim 1 , wherein the irradiation of the substrate with the physics spin isolated electromagnetic energy beam in pulsed on for a first period of time, followed by off for a recovery period of time sufficient to allow equilibration of a subatomic particle B-field.

6. The method of claim 5, wherein both the recovery period of time Trand an incremental distance Di are determined by:Tr = (DeN / C) / NxDi = (DeN ) / Nx wherein:DeN is the distance between an electron and a nucleus of a target atom; c is the speed of light; andNx is the integer energy level of photons of the physics spin isolated electromagnetic energy beam; wherein Nxis a larger of a value determined by (1 / Ni)2- (I / N2)2, and wherein N1 is a starting integer energy level and N2 is an ending integer energy level of the nucleus of the target atom.

7. The method of claim 6, wherein Di is greater than or equal to about 3 / 8*re, wherein reis a radius of an electron equal to 2.8179*10-15m.

8. The method of claim 1 , wherein the physics spin isolated electromagnetic energy beam is polarized.

9. The method of claim 1 , where the physics spin isolated electromagnetic energy beam is produced using a modified double slit / single slit filter comprising a single slit from which the physics spin isolated electromagnetic energy beam is produced, positioned within an interference pattern produced by a double slit.

10. The method of claim 1 , where the physics spin isolated electromagnetic energy beam is produced using a modified Stern Gerlach filter; or a modified Aharonov Bohm filter.1 1 . The method of claim 1 , wherein the radioactive substrate having the first atomic composition comprises a radioactive waste material and / or a radioactive fuel material.

12. The method of claim 10, wherein the second atomic composition is essentially nonradioactive.

13. The method of claim 1 , wherein the irradiating of the radioactive substrate with a physics spin isolated electromagnetic energy beam comprises changing a distance between a source of the electromagnetic energy beam and the substrate over a range configured to irradiate the portion of the substrate at intervals of greater than or equal to about 3 / 8 re, wherein reis a radius of an electron equal to about 2.8179*10-15m.

14. The method of claim 1 , wherein the radioactive substrate is disposed within a magnetic field sufficient to orient at least a portion of an xtrastatic axis of the atoms with the magnetic field, wherein the magnetic field is oriented essentially perpendicular to a direction of the monochromatic physics spin isolated electromagnetic energy beam.

15. The method of claim 1 , wherein the radioactive substrate is disposed between two electrodes having a difference in electric potential sufficient to produce an electrostatic field sufficient to orient at least a portion of the xtrastatic axis of the atoms with the electrostatic field, wherein the electrostatic field is oriented essentially perpendicular to a direction of the monochromatic physics spin isolated electromagnetic energy beam.

16. The method of claim 1 , wherein the radioactive substrate is disposed between two electrodes having a difference in electric potential sufficient to produce an electrostatic field sufficient to orient at least a portion of the xtrastatic axis of the atoms with the electrostatic field, wherein the electrostatic field is oriented essentially perpendicular to a direction of the monochromatic physics spin isolated electromagnetic energy beam; and a magnetic field sufficient to orient at least a portion of the xtrastatic axis of the atoms with the magnetic field, wherein the magnetic field is oriented essentially perpendicular to a direction of the monochromatic physics spin isolated electromagnetic energy beam.

17. A system comprising: a monochromatic physics spin isolated electromagnetic energy beam source configured to irradiate a radioactive substrate having a first atomic composition at a wavelength, an intensity, a temperature, and for a period of time sufficient to change at least a portion of the first atomic composition into a second atomic composition over a period of time less than would occur at a natural rate of radioactive decay of the first atomic composition.

18. The system of claim 17, configured to irradiate the radioactive substrate with a physics spin isolated electromagnetic energy beam at a plurality of distances between a source of the electromagnetic energy beam and the substrate over a range configured to irradiate the portion of the substrate at intervals of at a minimum spacing of about 3 / 8 re, wherein reis a radius of an electron equal to 2.8179*1 O’15m and a maximum sequence spacing and a maximum interval of intervals less than the chosen wavelength which has ranges from 10-14to 1 O05m.

19. The system of claim 17, further comprising a source of a magnetic field oriented about at least a portion of the radioactive substrate, configured to produce a magnetic field sufficient to orient at least a portion of an xtrastatic axis of atoms present within the radioactive substrate with the magnetic field, wherein the magnetic field is orientedessentially perpendicular to a direction of the monochromatic physics spin isolated electromagnetic energy beam; further comprising two electrodes oriented about at least a portion of the radioactive substrate, having a difference in electric potential sufficient to produce an electrostatic field sufficient to orient at least a portion of the xtrastatic axis of the atoms with the electrostatic field, wherein the electrostatic field is oriented essentially perpendicular to a direction of the monochromatic physics spin isolated electromagnetic energy beam; or a combination thereof.

20. The system of claim 17, wherein the radioactive substrate is a free flowing material flowing through a treatment cell in which the physics spin isolated electromagnetic energy beam source is directed into contact with the radioactive substrate.

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