WO2014087950A1

WO2014087950A1 - Energy acquisition and nucleotide transformation method

Info

Publication number: WO2014087950A1
Application number: PCT/JP2013/082297
Authority: WO
Inventors: 新井和夫; 張田吉昭
Original assignee: 有限会社フローネット
Priority date: 2012-12-08
Filing date: 2013-11-29
Publication date: 2014-06-12
Also published as: JPWO2014087950A1

Abstract

[Problem] To acquire energy safely and with high efficiency, to decontaminate radioactive contaminants with high efficiency, or to generate rare metals at a low cost. [Solution] According to "trinucleon theory," in which the atomic nucleus of an element comprises protons, neutrons, and a third nucleon A⁰that has linking functionality between α-vesicles, by controlling the number of third nucleon A⁰sconstituting the atomic nucleus of a substance, energy is acquired from a substance comprising elements having an atomic number of at least 3, and nuclide transformation or nucleosynthesis of a single or plurality of substances is carried out.

Description

Energy acquisition and nuclide conversion methods

In the present invention, the energy contained in the substance (mother nucleus) from the substance, the substance having a smaller atomic number than the substance (new material nucleus), or the substance having a larger atomic number than the substance from a plurality of substances is highly efficient. It is related to the technology acquired.

We humans have been using large amounts of energy since the Industrial Revolution, and large amounts of fossil fuels such as coal and oil have been used to secure the energy. As a result, the problem of global warming due to CO ₂ emission, which is said to be caused by fossil fuels, has occurred in recent years.

On the other hand, energy consumption is increasing with economic development, and there is a fear that the fossil fuel, which is an energy source, is depleted.

Natural energy such as wind power, solar power, biotechnology, etc. is also used as clean energy, but none of the methods is capable of responding to rapidly increasing energy demand.

Therefore, nuclear power generation using nuclear reactors that do not emit CO ₂ has increased in importance, and responding to energy demands from this nuclear reactor has been pointed out as safety issues such as nuclear accidents and radioactive contamination. Regardless, it has been implemented as a means of acquiring large amounts of energy.

A nuclear reactor is a neutron absorbing material called a control rod that uses 95% to 97% of uranium 238, which is difficult to fission, as a nuclear fuel. It is a device that keeps the reaction controlled and obtains high energy. Nuclear fuel materials include plutonium and thorium in addition to uranium.
The fission reaction is represented by equation (1) and the like. As uranium 235 ( ²³⁵ ₉₂ U) absorbs neutrons (N ⁰ ), it splits into barium ( ¹³⁷ ₅₆ Ba) and krypton ( ⁹⁷ ₃₆ Kr), and neutrons (N ⁰ ) and 220 MeV energy (Q). It is said that it has gained.

²³⁵ ₉₂ U + N ⁰ → ¹³⁷ ₅₆ Ba + ⁹⁷ ₃₆ Kr + 2N ⁰ + Q (1)
In addition, each symbol of ^Mz _Z X of the element symbol X is as follows.
X: Element symbol, Z: Atomic number, Mz: Nuclear mass

Manganese, nickel, molybdenum used in steel, platinum and palladium used in catalysts, neodymium, dysprosium used in magnets, etc. are metals that significantly improve the properties of the material. Because it is said to be a rare metal and its market price rises, alternative metals with improved properties are being developed.

It is said that the fission chain reaction in a nuclear reactor controls the fission chain reaction by controlling the amount of neutron irradiation, while maintaining safety. A nuclear accident occurs. There is also a risk of radioactive contamination from the nuclear reactor accident.

In addition, some spent fuel in the reactor may be reused as fuel, such as plutonium, but eventually it must be treated safely as radioactive waste, which entails enormous disposal costs and disposal. Securing a material processing place is also a problem.

In March 2011, due to the tsunami of the Great East Japan Earthquake, an accident occurred at the Fukushima Daiichi nuclear power plant where the nuclear reactor's cooling capacity declined and the nuclear fuel rods became hot and melted down. Furthermore, since a large amount of radioactive materials such as cesium was released by the hydrogen explosion in the reactor building, the response to radioactive material contamination is also a big problem.

In addition, research and development of alternative metals for metals that significantly improve properties such as manganese, nickel, molybdenum, platinum, palladium, neodymium, and dysprosium, which are said to be rare metals, have been widely carried out, but a high-efficiency production method has yet to be realized It cannot be said that it has been done.

The present invention has been made in view of the above-mentioned problems, and is rare in addition to the acquisition of nuclear energy without fear of nuclear accidents or radioactive contamination due to waste treatment, and safe and economical radioactive waste treatment. The purpose is to acquire metals.

Conventionally, it has been said that "the basic quantity that must first be a problem when trying to know the nature of a nucleus is the nuclear mass".
The usual mass formula for nuclei is based on the “binucleon theory” that nuclei are composed of protons and neutrons. The existing expression is only a kind of empirical formula. For an atom whose atomic number Z is known, the mass of protons corresponding to the atomic number Z is subtracted from the measured mass value Mz of the nucleus obtained in the experiment, and the rest The mass (Mz-Z) is determined to be all due to neutrons, and the number of neutrons is determined and an inductive mass formula is created. Therefore, the number of neutrons is not determined pictorially or theoretically.
Note that the π particle predicted by Yukawa is a virtual particle, and as shown in Non-Patent Document 8, the π particle does not contribute (reflect) as the mass of the nucleus in the interpretation based on the existing physics theory.

Inventor Arai, the inventor, has long advocated “trinucleon theory” in which the nucleus is composed of protons (hereinafter referred to as P ⁺ ), neutrons (hereinafter referred to as N ⁰ ), and π ^* particles (non-patented). Literature 1 to Non-Patent Literature 6).
In recent years, as stated in Non-Patent Document 9, it is emphasized that the introduction of pi particles is indispensable in recent research and that pi particles play an important role in the nucleus. And justifies the existence of the π ^* particles claimed in the present invention.
In the present invention, the π ^* particle that is responsible for bonding nuclei proposed by Arai is real rather than virtual, so the third nucleon A ⁰ given by A ⁰ = a ⁰ + ε (binding potential energy) (hereinafter referred to as a ⁰⁾ as below imaged manner described "Sankakuko theory".
Note that a ⁰ is a substantial amount of particles after subtracting the binding potential energy ε when the third nucleon A ⁰ is bonded to other nucleons (protons and neutrons) in the nucleus.

In the “two-nucleon theory”, Arai's “trinucleon theory” is to understand that the nucleus is composed of P ⁺ and N ⁰ , and one of the atomic structure is P ⁺ and the other is a baryon. It is. The baryon constituents are N ⁰ and A ^0, and each element starts with a P ⁺ 1 hydrogen nucleus having an atomic number Z of 1, and as the atomic number Z increases, that is, P ⁺ increases one by one, Baryons are combined one by one in order from the lowest energy level (ie, N ⁰ alone).

The baryon is a composite particle composed of one N ⁰ , n _A A ⁰ and n _Q vibrational energy ε _b, and the mass expression of the baryon is as shown in (2).
m _Bi = m _N + n _A m _A + n _Q ε _b (2)
Here, m _Bi : baryon mass, m _N : N ⁰ mass, n _A : A ⁰ number, m _A : A ⁰ mass,
n _Q: ε _b number, ε _b: vibrational energy
FIG. 1 shows the space structure of a baryon (free state).

Note that the vibrational energy n _Q ε _b existing as an apparent mass in the baryon is latent as a binding energy between P ⁺ and N ^{0 in} the nucleus.
Here, the maximum number of Z is [Z] = 137 which is the total number of baryons, and the values of the total number of A ⁰ n _Z ^* and the total number of ε _b n _Q ^* are specified for all Z (Table 1 and Table 1). 2).
The characteristics of all 137 types of baryons are shown in Non-Patent Document 6.

Arai's “Trinucleon Theory” means that in the case of a substance with atomic number 3 or more, it is composed of the third nucleon A ⁰ in addition to P ⁺ and N ⁰ which are nucleons in the “binucleon theory”. is there.

The nuclei of substances other than hydrogen and helium are, in principle, composed of α-spore conjugates (α clusters). An α vesicle is a unit structure mainly held by an α nucleus composed of two P ⁺ and two N ⁰ . Strictly speaking, this is the case where the atomic number (Z = the number of protons) is an even number (hereinafter referred to as α ⁺ cell), and in the case of an odd number, one proton / neutron combination (one P ⁺ and 1). Are composed of N ⁰ , hereinafter referred to as α ^- cells).

The α nucleus, more precisely the α ⁺ nucleus, is composed of two P ⁺ and two N ⁰ as in the general concept, but the space of the α ⁺ nucleus in the “trinucleon theory”. The structure is a mixture of self-revolving P ⁺ and N ⁰ , and P ⁺ is electrically repulsive, so their revolving orbits are not circumscribed, but the two N ⁰ are neutral. These revolving trajectories are circumscribed. Therefore, the image of the P ⁺ number 2 and the N ⁰ number 2 is shown in FIG. 2 as a basic form. This is a He (helium) nucleus.

And the nucleus of beryllium ⁹ ₄ Be, which is an element with atomic number Z = 4, is composed of P ⁺ 4 and baryons up to the fourth from the lowest energy level, and has two α vesicles. Two third nucleons A ⁰ are connected to the two α vesicles, and the A ⁰ revolution orbits of the two α vesicles are circumscribed to form an α cluster structure. It is. On one A ⁰ revolution track, there can be 1 to 4 A ^{0 due} to the dimensions of the A ⁰ revolution track radius and the A ⁰ radius. The spatial (geometric) structure is as shown in FIG.

As shown in FIG. 3, A ⁰ is configured to include (enclose) α nuclei in the circle of rotation, and form α vesicles. In addition, A ⁰ plays a role of binding a plurality of α vesicles, and the revolving P ⁺ or N ⁰ and A ⁰ are intermittently overlapped, whereby the binding potential energy between both ε _a ( (Latent) is consumed, and A ⁰ = a ⁰ + ε _a is considered, and as an optimum value by actual drawing, a ⁰ [0 · 2] (140 MeV) + ε _a [1/2 · (−1)] (40 MeV) Identified. [0 · 2] (140 MeV) can be replaced by existing π particles [0 · 2] (140 MeV), and hence A ⁰ [1/2 · 1] = π ⁰ [0 · 2] + ε _a [ ½ · (-1)]. Therefore, A ⁰ in FIG. 3 is drawn with the mass as m _π (π particle mass).

In FIG. 3, the revolution radius of each nucleon is given by a _r = (h / 2π) / mc, the nucleon radius is given as a _s = a _r / √2, and they are drawn in actual size ratios. h: Planck's constant, m: nucleon mass, c: speed of light. In this calculation, masses generally measured for P ⁺ , N ⁰ , and A ⁰ are applied.
That is, it can be said that the mass ratio of the nucleon P ⁺ or N ⁰ and A ⁰ creates such a spatial structure of the nucleus.

Thus, a structure in which a plurality of α vesicles are bound by A ⁰ corresponds to a generally referred to α cluster. An example of an α-cluster structure is shown in FIG. 4 for oxygen ¹⁷ ₈ O (having 6 A ⁰ ).

As described above, the “trinucleon theory” that Arai, the inventor of the inventor has proposed so far, is that the number of nuclei that do not decay instantaneously is the same number of Z N ⁰ as Z P ⁺ , and n _Z ^* it is composed of three kinds of nucleons of a ^0, the third nucleon a ⁰ is one in which the nuclei of the elements plays a role in binding the α cells, to.
In a recent study, for example, Itagaki et al. Published their research results as “the effect of“ glue ”played by neutrons and α-cluster binding form” (Non-Patent Document 7), but this also proved to Arai's proposal. Yes.

In addition, Arai has also proposed that the nuclear mass according to "Trinucleon theory" is as follows. That is, an element that does not instantaneously transmutate (hereinafter referred to as a stable element) has an n _Z ^* (total number of A ⁰ ) corresponding to the Z number (atomic number), and the nuclear mass M _{Z of} this stable element. ^* Is determined by equation (3).

_{^{_{_{M Z * = Z (m P}}}} + m N) + n Z * m A ··· (3)
Where m _x = (Aπ + B) [Z] m _e
However, X [A · B], [Z] = 137
P ⁺ [3.4], N ⁰ [3.4], A ⁰ [1/2 · 1]
m _P : P ⁺ mass, m _N : N ⁰ mass, m _A : A ⁰ mass, _me : electron mass

As shown in Table 1, Table 2, and FIG. 5, the nuclear mass M _Z ^* calculated by the equation (3) is in good agreement with the nuclear mass (M _Z ) of a stable element generally measured so far. This fact can be said that the formula (3) is qualified as a nuclear mass formula with a theoretical basis.
That is, Table 1, Table 2, and FIG. 5 can be said to be valuable verification results that theoretically explain quantitative data regarding few nuclei. In Tables 1 and 2, the total number of ε _b n _Q ^* obtained from the mass expression (2) of baryons is also shown.

The present invention based on the “trinucleon theory” described so far will be described below.
An important point of the present invention is to control the number of A ⁰ having the function of binding α vesicles in the nucleus of a substance based on the nuclear mass formula (3) presented by Arai, the inventor of the inventor.

Here, ^A0 will be described.
When α particles are irradiated onto beryllium by the method used in the reactor initiator, the generated particles are determined to be N ⁰ (neutrons) as shown in equation (4). Since this reaction is understood by the existing “binucleon theory”, the generated particles are N ⁰ .

⁹ ₄ Be + ⁴ ₂ α → ¹² ₆ C + N ⁰ (4)

However, the inventor has come to the recognition that the generated particles are not N ⁰ but 4A ⁰ + A ^{0 *} by “trinucleon theory”. That is, even when irradiated with α particles in beryllium is α particles + charge is α cells also positive charge in beryllium, to separate the irradiation, the N ⁰ rather, as in equation (5) 4A ⁰ + A ^{0 *} .

⁹ ₄ Be + ⁴ ₂ α → ¹² ₆ C + 4A ⁰ + A ^{0 *} (5)

That is, in the “trinucleon theory”, N ⁰ can be expressed by the equations (6) and (7). From these equations, the release of general concept one N ⁰ (the "Nikakuko theory") is comprised of four A ^⁰ {4A ^0} (quadrupole bodies) and one and the sum of A ^{0 *} It can be considered. In addition, () shows energy.

N ⁰ [3 • 4] = 4A ⁰ [1/2 • 1] + A ^{0 *} [1 • 0] (6)
(940MeV) (180MeV) (220MeV)
A ^{0 *} [1 · 0] = A ⁰ [1/2 · 1] + ε _b [1/2 · (−1)] ·· (7)
(40MeV)

A ⁰ is a particle of π ⁰ on the revolution orbit in the α vesicle, and is moving along its own orbital motion while constraining P ⁺ and N ⁰ in the α nucleus under the binding force of ε _a .
This A ⁰ to disengage from the orbit (peeling) should not be particles as the same time the incident bullet when thrust away the A ⁰ from orbit trapped in orbit. Therefore, the irradiation particles are not at the same energy level as A ^0, it is A ^{0 *} of higher energy level than A ^0.

The characteristics of the irradiated particle A ^{0 *} are determined as follows.
The estimated energy value of the particles irradiated for the removal of one A ⁰ is expressed by Equation (8).

π [0 · 2] + ε _a [1/2 · (−1)] + ε _b [1/2 · (−1)] = A ^{0 *} [1 · 0] (8)
140MeV 40MeV 40MeV 220MeV
(Π particle mass) (binding energy) (vibration energy)

A ⁰ is obtained by adding energy ε _a = 40 MeV to π ⁰ particles.

The present invention as has been described so far, by controlling the number of A ⁰ based on a nucleus Mass formula, for different materials, separation of the mother nucleus, and performs nuclide and synthesis of nuclei.

According to the present invention based on the “trinucleon theory”, there is no single release of P ⁺ or N ^{0 in} the change of the Z number of the nucleus, and the release is the α nucleus ( ⁴ ₂ He nucleus, its mass), e− other is the only ^{a 0.} As the number of Z increases as n _Z0 ^* > n _Z1 ^* + n _Z2 ^* (where Z ₀ = Z ₁ + Z ₂ ), the parent nucleus of Z ₀ is two child nuclei of Z ₁ and Z ₂ (stable) When the mother nucleus (Z ₀ ) is separated into two child nuclei (Z ₁ and Z ₂ ), {n _Z0 ^* − (n _Z1 ^* + n _Z2 ^*) } A ⁰ As it is released, energy is released.

In the separation of the mother nucleus according to the present invention, high-speed A ^{0 *} is irradiated with the mother nucleus as a target nucleus, and the n _a ⁰ obtained from the nuclear mass formula are separated, and both the first and second stable nucleuses are separated from each other. While separating into two nuclei, energy of n _b α particles, n _a A ⁰ and n _c ε can be obtained. These A ⁰ and ε can be used as irradiation A ^{0 *} .
The reaction is as shown in formula (9).

^{_{^{_{_{M0 z0 X n0 Q0 -n a A}}}}} 0 → M1 z1 X n1 Q1 + M2 z2 X n2 Q2 + N _b α + n _c ε (9)
Here, Z0 = Z1 + Z2 + 2n b, n a = n0- (n1 + n2), n b = {Z0- (Z1 + Z2)} / 2, n c = Q0- (Q1 + Q2)

Here, the ^{_{^{_{^{MZ * Z X nZ * n Q}}}}} * each symbol of element symbol X, are as follows.
X: element symbol, Z: atomic number, Mz ^*: nuclear mass, n _z *: ^{A 0} _{Total, n} ^{Q *:} _ε _b the total number

Nuclide according to the invention, the nucleus by irradiating a high-speed A ^{0 *} as a target, separating the n _a number of A ⁰ obtained from nuclei mass expression, stability of the smaller atomic number than the atomic number of the nucleus You can get a nucleus. This reaction is a phenomenon called β ⁺ decay, which is the so-called decay number k times in equation (10).

_{^{_{^{z0 X n0 -n a A 0 →}}}} z1 X n1 ··· (10)
Where n _a = n0−n1, Z1 = Z0−k

Further, by irradiating the number of A ⁰ obtained from nuclei mass expression at low speed, by adding A ⁰ in the mother nucleus, it is possible to obtain a stable Kokaku of atomic number greater than atomic number of nucleus. This reaction is a phenomenon called β ^- decay with a so-called decay number k times in equation (11).

_{^{_{^{z0 X n0 + n a A 0}}}} → z1 X n1 ··· (11)
Where n _a = n1-n0, Z1 = Z0 + k

Synthesis of nuclei by the present invention, one of the nuclear as the target nucleus, the number of A ⁰ obtained from the other nuclear and nuclear mass formula by irradiating at a low speed, it is possible to synthesize stable nuclei. In addition, as for the nucleus to irradiate, it is desirable to select a nucleus with small mass among both nuclei.
The reaction is as shown in Formula (12).

_{^{_{^{z1 X n1 + z2 X n2 +}}}} n a A 0 → z3 X n3 ··· (12)
Where n _a = n3− (n1 + n2), Z3 = Z1 + Z2

Since the energy inherent in the nucleus of a substance having an atomic number of 3 or more is utilized, the energy can be obtained at low cost with a small device.

Energy acquisition without global environmental pollution such as CO ₂ emissions and dust emissions becomes possible.

Because the mother nucleus is separated into non-radioactive nuclei, energy can be obtained without fear of radioactive contamination.

With respect to spent fuel, which is a waste in a nuclear reactor, a long-lived radioactive material waste can be converted into a non-radioactive material by the nuclear separation of the present invention.

By the nuclide conversion and nucleosynthesis of the present invention, rare metals such as gold, platinum, dysprosium and vanadium can be produced at low cost.

The free baryon spatial structure is shown. Shows the spatial structure of α ⁺ nuclei. The spatial structure of beryllium ⁹ ₄ Be is shown. The spatial structure of oxygen ¹⁷ ₈ O is shown. The atomic number and atomic nucleus mass and A ⁰ Total relationship shown in the graph.

As examples of the present invention, methods such as energy acquisition, decontamination of radioactive elements, and generation of rare metals will be described below.

First, a specific method for obtaining energy by a nuclear separation reaction is described. The key to acquiring the energy inherent in the nucleus is to avoid releasing radioactive nuclei during the energy acquisition.
Considering that ₁₄ Si and ₂₆ Fe (excluding ₈ O), which are present in large quantities inside the earth, are fission nuclei of heavy elements, there is a probability that they will be generated in the nucleus as stable elements during natural fission. It can be considered as a high element.
Therefore, as the mother nucleus candidates, those that produce a stable element Si or Fe or a combination of Si and Fe as child nuclei are selectively considered. The following process is suitable as a reference example of the present invention.

By irradiating the mother nucleus such as Ni, Zr, or Te with high-speed A ^{0 *} and stripping off the number of A ⁰ obtained from the nuclear mass equation that binds the α nuclei of the mother nucleus, the equations (13) to as shown in equation _{(16), 25ε b, 38ε} b, 58ε b, it is possible to energy acquisition 13ε _b. In addition, it can be regarded as a part of the stripped A ⁰ also won energy. In the formula (16), ⁴ ₂ He ⁰ ₀ is an α nucleus.

⁶⁵ ₂₈ Ni ⁴⁶ ₆₉ -16A ⁰ → 2 ³¹ ₁₄ Si ¹⁵ ₂₂ + 25ε _b (13)

⁹⁵ ₄₀ Zr ⁷⁹ ₁₁₆ -22A ⁰ → ³¹ ₁₄ Si ¹⁵ ₂₂ + ⁶⁰ ₂₆ Fe ⁴² ₅₆ + 38ε _b (14)

¹²⁷ ₅₂ Te ¹¹⁹ ₁₇₀ -35A ⁰ → 2 ⁶⁰ ₂₆ Fe ⁴² ₅₆ + 58ε _b (15)

⁶⁵ ₂₈ Ni ⁴⁶ ₆₉ -4A ⁰ → ⁶⁰ ₂₆ Fe ⁴² ₅₆ + ⁴ ₂ He ⁰ ₀ + 13ε _b (16)

Here, the ^{_{^{_{^{MZ * Z X nZ * n Q}}}}} * each symbol of element symbol X, are as follows.
X: element symbol, Z: atomic number, Mz ^*: nuclear mass, n _z *: ^{A 0} _{Total, n} ^{Q *:} _ε _b the total number

In addition, as a reference example of the present invention in the decontamination of radioactive elements, the decontamination process of the most typical long-lived radioactive substance cesium ¹³⁷ ₅₅ Cs will be described.

In the category of α cluster structure theory, the nuclear separation method of the present invention based on the “trinucleon theory” is based on the optimal A ⁰ group coordination state and mass level (ie, on the stable line of the mass spectrum). Doing things in a mess is nothing but voluntary and encouraging static nuclear separation. Static nuclear separation means that only non-radioactive nuclei (stable nuclei) are produced, which is safe.

Therefore, by irradiating ¹³⁷ ₅₅ Cs with high-speed A ^{0 *} and stripping 45 A ^0s that bind α vesicles of the parent nucleus of ¹³⁷ ₅₅ Cs, as shown in equation (17), long Decontamination can be achieved by transmuting lifetime radioactive nuclei into ⁶⁰ ₂₆ Fe ⁴² ₅₆ and ⁶⁷ ₂₉ Cu ⁴⁸ ₇₅ which are non-radioactive stable nuclei. Further, this decontamination process, energy winning 45 of A ⁰ and 75Ipushiron _b also becomes possible, resulting Fe and Cu can also be used separately industries.

¹³⁷ ₅₅ Cs ¹³⁵ ₂₀₆ -45A ⁰ → ⁶⁰ ₂₆ Fe ⁴² ₅₆ + ⁶⁷ ₂₉ Cu ⁴⁸ ₇₅ + 75ε _b (17)

Next, a method for producing rare metals at low cost by nuclide conversion will be described.
As a reference example of the present invention for nuclide conversion, mercury is used as a target nucleus, irradiation with high-speed A ^{0 *} and stripping of four A ⁰ in the mercury nucleus, as shown in formula (18), Stable gold can be produced.

²⁰² ₈₀ Hg ²²⁰ -4A ⁰ → ²⁰¹ ₇₉ Au ²¹⁶ + e ⁺ (18)

As another example, the lead as a target nucleus is irradiated with high-speed A ^{0 *,} by stripping the twelve A ⁰ in Namarikaku, as shown in equation (19), a stable gold Can be generated.

²⁰⁸ ₈₂ Pb ²²⁸ -12A ⁰ → ²⁰¹ ₇₉ Au ²¹⁶ + ⁴ ₂ He ⁰ + e ⁺ (19)

Next, a method for producing rare metals at low cost by nuclear synthesis will be described.
As a reference example of the present invention of the nuclear synthesis target nucleic iodine, as well as iron and the incident nuclear radiation, by adding irradiated with 52 pieces of A ⁰ at a low speed, as shown in equation (20) stable Gold can be generated.

¹²⁹ ₅₃ I ¹²² + ⁶⁰ ₂₆ Fe ⁴² + 52A ⁰ → ¹⁹⁹ ₇₉ Au ²¹⁶ (20)

As examples of other nuclear synthesis, krypton target nuclei, with and irradiates zinc incident nuclei, by adding irradiated with 48 A ⁰ at a low speed, as shown in equation (21), stable Rare metal dysprosium can be produced.

⁸⁴ ₃₆ Kr ⁶⁵ + ⁷⁰ ₃₀ Zn ⁵⁰ + 48A ⁰ → ¹⁶³ ₆₆ Dy ¹⁶³ (21)

The preferred embodiments of the present invention have been described in detail above. However, the present invention is not limited to the above-described embodiments, and various modifications and substitutions can be made to the above-described embodiments without departing from the scope of the present invention. Can be added.

1 Proton (P ⁺ )
2 Neutrons (N ⁰ )
3 Nucleon A ⁰
4 P ⁺ revolution orbit 5 N ⁰ revolution orbit 6 A ⁰ revolution orbit 7 α cell

Claims

Nucleus of the element is, protons, by "Sankakuko theory" that is composed of nucleons A 0 having a neutron and α cells binding function, the material atomic number is from 3 or more elements, the nucleons A 0 of the substance A method for obtaining energy inherent in the nucleus (mother nucleus) of the substance by separating a part and controlling the number thereof.
Controlling the number of nucleons A 0 constituting the atomic nuclei of a substance by “trinucleon theory” in which the atomic nucleus is composed of protons, neutrons, and nucleons A 0 having an α-cell coupling function A method for converting the nuclide of the substance.
By controlling the number of nucleons A 0 to be added to a plurality of substances by the “trinucleon theory” that the atomic nuclei are composed of protons, neutrons, and nucleons A 0 having an α-cell coupling function. A method for producing (nucleating synthesis) a nuclide different from the above substance.
According to the “trinucleon theory” in which the atomic nucleus of the element is composed of protons, neutrons, and nucleons A 0 having an α-cell coupling function, a part of the nucleus nucleons A 0 of the mother nucleus A method of separating by separation into a plurality of stable nuclear materials (child nuclei) having a small atomic number and releasing other separated products (α nuclei, nucleon A 0 , kinetic energy, vibration energy, etc.).
Wherein the control of the number of nucleons A 0, performs control based on the total number of nucleons A 0 of the calculation result by nuclear Mass expression of the elements, method according to claims 1 to 4.