Neutron and proton generating processes

Abstract

Neutron and proton generating processes consist in a thermal neutrons generation process arising in particular circumstances after destabilization of a coherent electrons beam wherein electrons have a minimum carrying-energy of 1.022 MeV; a thermal protons generation process arising in particular circumstances after destabilization of a coherent positrons beam wherein positrons have a minimum carrying-energy of 1.022 MeV; and a stochastically equal numbers of thermal protons and neutrons generation process arising in particular circumstances after destabilization of a coherent electromagnetic photons beam wherein photons have a minimum energy of 1.022 MeV. Large amounts of residual energy and metastable partons would be produced during each process.

Claims

1. Processes for generating neutrons and protons.

2. A process for generating neutrons and protons as in claim 1 wherein protons and neutrons are generated by destabilization of elementary particles.

3. A process for generating neutrons and protons as in claim 2 wherein the elementary particles are photons.

4. A process for generating neutrons and protons as in claim 2 wherein the protons are produced by way of destabilization of positron carrying energy, and neutrons are produced by destabilization of electron carrying energy.

5. A process for generating neutrons and protons as in claim 1 wherein a coherent photon beam made of photons, each minimally possessing 1.022 MeV of energy, is destabilized by way of a beam of elementary particles, comprised of, but not limited to, photons, electrons, positron, protons, and neutrons that intersect the path of said incoming beam according to proximity, amount and velocity parameters configured to provide optimal output.

6. The process for generating neutrons and protons of claim 5 wherein said incoming photon beam is generated by a FEL laser able to generate coherent photon beams in the 1.022 MeV range.

Description

BRIEF DESCRIPTION OF THE DRAWINGS

[0038] FIG. 1 Schematic illustration of a beam generating equipment for generating protons and neutrons from destabilizing photons each having 1.022 MeV energy, as per claims 5 and 6.

[0039] FIG. 2 Schematic illustration of a beam generating equipment for generating neutrons from destabilizing electrons each having 1.022 MeV carrying energy, as per claim 4.

[0040] FIG. 3 Schematic illustration of a beam generating equipment for generating protons from destabilizing positrons each having 1.022 MeV carrying energy, as per claim 4

DETAILED DESCRIPTION

[0041] The scattering energies that caused some protons and neutrons to be produced during the 1970's SPEAR facility experiments ran into the 6 to 7 GeV range as documented in the paper titled Evidence for Jet Structure in Hadron Production by e+ eAnnihilation previously mentioned. But considering that for the 2 possible threesome electron-positron configurations considered to mutually capture and initiate the hypothesized irreversible adiabatic acceleration sequence, these particles need to have little or even no translational energy while being in very close proximity to each other for the process to be triggered, it appears that to maximize nucleon production during such processes, the scattering energy level must be kept as close as possible to the 1.022 MeV threshold carrying-energy for each electron, positron, or photon of the incoming beams being used, while taking care that the total scattering energy doesn't go under the 1.022 MeV energy threshold, which prevents pair production.

PROTON AND NEUTRON GENERATION BY PHOTON DESTABILIZATION

[0042] To produce protons an neutrons in stochastically approximate equal numbers, there is need to destabilize a coherent photon beam made of photons each minimally possessing 1.022 MeV of energy. The incoming photon beam may be generated by a FEL laser or other device able to generate coherent photon beams in the 1.022 MeV range (FIG. 1).

[0043] The required destabilizing factor that cause the 1.022 MeV photons of the incoming photon beam to destabilize is provided by a beam of elementary particles made of photons, electrons, positron, protons or neutrons or other particles that intersect the path of the incoming beam according to proximity, amount and velocity parameters configured to provide optimal output (see FIG. 1).

[0044] In the case of use of a 1.022 MeV incoming beam, both incoming beam and destabilizing beam have to be as tightly colimated as possible for the pairs to appear in sufficient numbers and proximity for the threesomes to form (see FIG. 1).

[0045] The incoming photon beam can be made of photons of less than 1.022 MeV energy photons, provided that the destabilizing beam contributes the required missing energy upon scattering.

[0046] The primary output of the intersection of both beams is a beam stochastically containing approximate equal numbers of protons and neutrons, and as secondary output, radiation energy and stray metastable partons amounting to approximately 465 MeV of new energy for each proton or neutron produced (see FIG. 1).

Neutron Generation by Destabilization of Electron Carrying Energy

[0047] To produce neutrons from the destabilization of an incoming electron beam, each electron being induced with 1.022 MeV of energy, the destabilizing factor is provided by a beam of elementary particles made of photons, electrons, positron, protons or neutrons or other particles that intersect the path of the incoming electron beam according to proximity, amount and velocity parameters configured to provide for optimal output (see FIG. 2).

[0048] The decoupled electron-positron pair that appears as the 1.022 MeV electron carrier-photon decouples, is generated by structure in the immediate proximity of the carried electron, initiating the production of a thermal neutron initially devoid of translational energy, all of the incoming electron carrying-energy having been converted to mass.

[0049] The primary output of the intersection of both beams is a neutron beam, plus as secondary output, radiation energy and stray metastable partons amounting to approximately 465 MeV of new energy for each neutron produced (see FIG. 2).

Proton Generation by Destabilization of Positron Carrying Energy

[0050] To produce protons from the destabilization of an incoming positron beam, each positron being induced with 1.022 MeV of energy, the destabilizing factor is provided by a beam of elementary particles made of photons, electrons, positron, protons or neutrons or other particles that intersect the path of the incoming positron beam according to proximity, amount and velocity parameters configured to provide for optimal output (see FIG. 3).

[0051] The decoupled electron-positron pair that appears as the 1.022 MeV positron carrier-photon decouples, is generated by structure in the immediate proximity of the carried positron, initiating the production of a thermal proton initially devoid of translational energy, all of the incoming positron carrying-energy having been converted to mass.

[0052] The primary output of the intersection of both beams is a proton beam, plus as secondary output, radiation energy and stray metastable partons amounting to approximately 465 MeV of new energy for each proton produced (see FIG. 3).

[0053] The foregoing is considered as illustrative only of the principles of the invention. Further, since numerous modifications and changes will readily occur to those skilled in the art, it is not desired to limit the invention to the exact construction and operation shown and described, and accordingly, all suitable modifications and equivalents may be resorted to, falling within the scope of the invention.