tag:blogger.com,1999:blog-20831713162247825492024-02-08T11:35:10.107-08:00Nuclear sets Set n isolated and ordered on natural number n of nucleus structures D.p/n, each of which is submitted by identical cooperating individual elements n , defects D and form p refers to as by nuclear set.
Unknownnoreply@blogger.comBlogger1125tag:blogger.com,1999:blog-2083171316224782549.post-48611002462719730272016-11-09T09:27:00.001-08:002017-01-19T10:29:25.806-08:00<div dir="ltr" style="text-align: left;" trbidi="on">
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<b style="mso-bidi-font-weight: normal;"><span lang="EN-US" style="color: windowtext; mso-ansi-language: EN-USfont-size:10.0pt; mso-font-kerning: 0pt;"><span style="mso-spacerun: yes;"><span class="Apple-style-span" style="font-size: 14px; font-weight: normal;"><b style="mso-bidi-font-weight: normal;"><span lang="EN-US" style="color: windowtext; font-size: 10.0pt; mso-ansi-language: EN-US; mso-font-kerning: 0pt;"><span style="mso-spacerun: yes;"> </span><span class="GramE">THE CLOSED ENUMERABLE SETS<span style="font-weight: normal;">.</span></span></span></b><span lang="EN-US" style="color: windowtext; font-size: 10.0pt; mso-ansi-language: EN-US; mso-font-kerning: 0pt;"><span style="mso-spacerun: yes;"> </span><span class="GramE">Symmetry of atomic nucleus.</span><span style="mso-spacerun: yes;"> </span></span></span></span></span></b><br />
<b style="mso-bidi-font-weight: normal;"><span lang="EN-US" style="color: windowtext; mso-ansi-language: EN-USfont-size:10.0pt; mso-font-kerning: 0pt;"><span style="mso-spacerun: yes;"><span class="Apple-style-span" style="font-size: 14px; font-weight: normal;"><span lang="EN-US" style="color: windowtext; font-size: 10.0pt; mso-ansi-language: EN-US; mso-font-kerning: 0pt;"><span style="mso-spacerun: yes;"><br /></span></span></span></span></span></b>
<span lang="EN-US" style="color: windowtext; font-size: 8.0pt; mso-ansi-language: EN-US; mso-font-kerning: 0pt;">“Absence of absolute true makes </span><br />
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<a href="https://en.wikipedia.org/wiki/File:Nuclear_set_a.png">https://en.wikipedia.org/wiki/File:Nuclear_set_a.png</a><br />
<a href="https://en.wikipedia.org/wiki/File:Nuclear_set_b.png">https://en.wikipedia.org/wiki/File:Nuclear_set_b.png</a><br />
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<span lang="EN-US" style="color: windowtext; font-size: 10.0pt; mso-ansi-language: EN-US; mso-font-kerning: 0pt;"><span style="mso-spacerun: yes;"><span lang="EN" style="font-family: "times new roman" , "serif"; font-size: 12.0pt;">Contents</span></span></span><br />
<h2>
<span lang="EN-US" style="color: windowtext; font-size: 10.0pt; mso-ansi-language: EN-US; mso-font-kerning: 0pt;"><span style="mso-spacerun: yes;"><span lang="EN" style="font-family: "times new roman" , "serif"; font-size: 12.0pt;">
<span style="font-size: x-large;">The theory of nuclear sets</span></span></span></span></h2>
<h2>
<b><span style="font-weight: normal;"><span lang="EN-US" style="color: windowtext; font-size: 10.0pt; mso-ansi-language: EN-US; mso-font-kerning: 0pt;"><span style="mso-spacerun: yes;"><span lang="EN" style="font-family: "times new roman" , "serif"; font-size: 12.0pt;">
</span></span></span></span></b><span style="font-weight: normal;"><span lang="EN-US" style="color: windowtext; font-size: 10.0pt; mso-ansi-language: EN-US; mso-font-kerning: 0pt;"><span style="mso-spacerun: yes;"><span lang="EN" style="font-family: "times new roman" , "serif"; font-size: 12.0pt;">§1.</span></span></span></span><b><span style="font-weight: normal;"><span lang="EN-US" style="color: windowtext; font-size: 10.0pt; mso-ansi-language: EN-US; mso-font-kerning: 0pt;"><span style="mso-spacerun: yes;"><span lang="EN" style="font-family: "times new roman" , "serif"; font-size: 12.0pt;"><b><span style="font-size: large;"> Nuclear set</span>.</b></span></span></span></span></b><span style="font-weight: normal;"><span lang="EN-US" style="color: windowtext; font-size: 10.0pt; mso-ansi-language: EN-US; mso-font-kerning: 0pt;"><span style="mso-spacerun: yes;"><span lang="EN" style="font-family: "times new roman" , "serif"; font-size: 12.0pt;"> 2</span></span></span></span></h2>
<h2>
<b><span style="font-weight: normal;"><span lang="EN-US" style="color: windowtext; font-size: 10.0pt; mso-ansi-language: EN-US; mso-font-kerning: 0pt;"><span style="mso-spacerun: yes;"><span lang="EN" style="font-family: "times new roman" , "serif"; font-size: 12.0pt;">
§2. <b><span style="font-family: "times new roman" , "serif";">Systematic</span> Definitions</b>. 4</span></span></span></span></b></h2>
<h2>
<b><span style="font-weight: normal;"><span lang="EN-US" style="color: windowtext; font-size: 10.0pt; mso-ansi-language: EN-US; mso-font-kerning: 0pt;"><span style="mso-spacerun: yes;"><span lang="EN" style="font-family: "times new roman" , "serif"; font-size: 12.0pt;">
§3.<span style="font-size: large;"> Common structural features</span>. 6</span></span></span></span></b></h2>
<h2>
<b><span style="font-weight: normal;"><span lang="EN-US" style="color: windowtext; font-size: 10.0pt; mso-ansi-language: EN-US; mso-font-kerning: 0pt;"><span style="mso-spacerun: yes;"><span lang="EN" style="font-family: "times new roman" , "serif"; font-size: 12.0pt;">
§4.<span style="font-size: large;"> R</span></span><span class="shorttext" style="font-size: large;"><span lang="EN" style="mso-ansi-language: EN;">egularity</span></span><span lang="EN" style="font-family: "times new roman" , "serif"; font-size: 12.0pt;"><span style="font-size: large;">. Tabular systematization</span>. 6</span></span></span></span></b></h2>
<h2>
<b><span style="font-weight: normal;"><span lang="EN-US" style="color: windowtext; font-size: 10.0pt; mso-ansi-language: EN-US; mso-font-kerning: 0pt;"><span style="mso-spacerun: yes;"><span lang="EN" style="font-family: "times new roman" , "serif"; font-size: 12.0pt;">
§5. Structuring. Linear </span><span class="shorttext"><span lang="EN" style="mso-ansi-language: EN;">decomposition</span></span><span lang="EN" style="font-family: "times new roman" , "serif"; font-size: 12.0pt;">. 7</span></span></span></span></b></h2>
<h2>
<b><span style="font-weight: normal;"><span lang="EN-US" style="color: windowtext; font-size: 10.0pt; mso-ansi-language: EN-US; mso-font-kerning: 0pt;"><span style="mso-spacerun: yes;"><span lang="EN" style="font-family: "times new roman" , "serif"; font-size: 12.0pt;">
§6. <span style="font-size: large;">Symmetry ratios. The symmetry of the </span></span><span class="shorttext" style="font-size: large;"><span lang="EN" style="mso-ansi-language: EN;">form</span></span><span lang="EN" style="font-family: "times new roman" , "serif"; font-size: 12.0pt;">. 8</span></span></span></span></b></h2>
<h2>
<b><span style="font-weight: normal;"><span lang="EN-US" style="color: windowtext; font-size: 10.0pt; mso-ansi-language: EN-US; mso-font-kerning: 0pt;"><span style="mso-spacerun: yes;"><span lang="EN" style="font-family: "times new roman" , "serif"; font-size: 12.0pt;">
§7. <span style="font-size: large;">The basis of the nuclear space</span>. 11</span></span></span></span></b></h2>
<h2>
<b><span style="font-weight: normal;"><span lang="EN-US" style="color: windowtext; font-size: 10.0pt; mso-ansi-language: EN-US; mso-font-kerning: 0pt;"><span style="mso-spacerun: yes;"><span lang="EN" style="font-family: "times new roman" , "serif"; font-size: 12.0pt;">
§8. Properties of nested structures. 15</span></span></span></span></b></h2>
<h2>
<b><span style="font-weight: normal;"><span lang="EN-US" style="color: windowtext; font-size: 10.0pt; mso-ansi-language: EN-US; mso-font-kerning: 0pt;"><span style="mso-spacerun: yes;"><span lang="EN" style="font-family: "times new roman" , "serif"; font-size: 12.0pt;">
§9. </span><span class="shorttext"><span lang="EN" style="mso-ansi-language: EN;">Inter-element</span></span><span lang="EN" style="font-family: "times new roman" , "serif"; font-size: 12.0pt;"> connection and symmetry. 20</span></span></span></span></b></h2>
<h2>
<b><span style="font-weight: normal;"><span lang="EN-US" style="color: windowtext; font-size: 10.0pt; mso-ansi-language: EN-US; mso-font-kerning: 0pt;"><span style="mso-spacerun: yes;"><span lang="EN" style="font-family: "times new roman" , "serif"; font-size: 12.0pt;">
§10. <span style="font-size: large;">Quantum interactions. The energy of the nucleus</span>. 21</span></span></span></span></b></h2>
<h2>
<b><span style="font-weight: normal;"><span lang="EN-US" style="color: windowtext; font-size: 10.0pt; mso-ansi-language: EN-US; mso-font-kerning: 0pt;"><span style="mso-spacerun: yes;"><span lang="EN" style="font-family: "times new roman" , "serif"; font-size: 12.0pt;">
§11. Matrix of table and core. 22</span></span></span></span></b></h2>
<h2>
<b><span style="font-weight: normal;"><span lang="EN-US" style="color: windowtext; font-size: 10.0pt; mso-ansi-language: EN-US; mso-font-kerning: 0pt;"><span style="mso-spacerun: yes;"><span lang="EN" style="font-family: "times new roman" , "serif"; font-size: 12.0pt;">
§12.<span style="font-size: large;"> Rebuilding cores of set</span>. 24</span></span></span></span></b></h2>
<h2>
<b><span style="font-weight: normal;"><span lang="EN-US" style="color: windowtext; font-size: 10.0pt; mso-ansi-language: EN-US; mso-font-kerning: 0pt;"><span style="mso-spacerun: yes;"><span lang="EN" style="font-family: "times new roman" , "serif"; font-size: 12.0pt;">
§13. A</span><span class="shorttext"><span lang="EN" style="mso-ansi-language: EN;">ssociation</span></span><span lang="EN" style="font-family: "times new roman" , "serif"; font-size: 12.0pt;"> and decay of nuclei. 25</span></span></span></span></b></h2>
<h2>
<b><span style="font-weight: normal;"><span lang="EN-US" style="color: windowtext; font-size: 10.0pt; mso-ansi-language: EN-US; mso-font-kerning: 0pt;"><span style="mso-spacerun: yes;"><span lang="EN" style="font-family: "times new roman" , "serif"; font-size: 12.0pt;">
§14. The basic structure of the excited state. 27</span></span></span></span></b></h2>
<h2>
<b><span style="font-weight: normal;"><span lang="EN-US" style="color: windowtext; font-size: 10.0pt; mso-ansi-language: EN-US; mso-font-kerning: 0pt;"><span style="mso-spacerun: yes;"><span lang="EN" style="font-family: "times new roman" , "serif"; font-size: 12.0pt;">
§15. Table of basic dynamic states. 29</span></span></span></span></b></h2>
<h2>
<b><span style="font-weight: normal;"><span lang="EN-US" style="color: windowtext; font-size: 10.0pt; mso-ansi-language: EN-US; mso-font-kerning: 0pt;"><span style="mso-spacerun: yes;"><span lang="EN" style="font-family: "times new roman" , "serif"; font-size: 12.0pt;">
§16. <span style="font-size: large;">The symmetry of the atomic nuclei</span>. 32</span></span></span></span></b></h2>
<h2>
<b><span style="font-weight: normal;"><span lang="EN-US" style="color: windowtext; font-size: 10.0pt; mso-ansi-language: EN-US; mso-font-kerning: 0pt;"><span style="mso-spacerun: yes;"><span lang="EN" style="font-family: "times new roman" , "serif"; font-size: 12.0pt;">
§17. <span style="font-size: large;">Tunnel interaction</span> 35</span></span></span></span></b></h2>
<h2>
<b><span style="font-weight: normal;"><span lang="EN-US" style="color: windowtext; font-size: 10.0pt; mso-ansi-language: EN-US; mso-font-kerning: 0pt;"><span style="mso-spacerun: yes;"><span lang="EN" style="font-family: "times new roman" , "serif"; font-size: 12.0pt;">
§18.<span style="font-size: large;"> Exchange interactions</span>. 37</span></span></span></span></b></h2>
<h2>
<b><span style="font-weight: normal;"><span lang="EN-US" style="color: windowtext; font-size: 10.0pt; mso-ansi-language: EN-US; mso-font-kerning: 0pt;"><span style="mso-spacerun: yes;"><span lang="EN" style="font-family: "times new roman" , "serif"; font-size: 12.0pt;">
§19. Interactions in dynamic conditions 39</span></span></span></span></b></h2>
<h2>
<b><span style="font-weight: normal;"><span lang="EN-US" style="color: windowtext; font-size: 10.0pt; mso-ansi-language: EN-US; mso-font-kerning: 0pt;"><span style="mso-spacerun: yes;"><span lang="EN" style="font-family: "times new roman" , "serif"; font-size: 12.0pt;">
§20. Shards and chips. 39</span></span></span></span></b></h2>
<h2>
<b><span style="font-weight: normal;"><span lang="EN-US" style="color: windowtext; font-size: 10.0pt; mso-ansi-language: EN-US; mso-font-kerning: 0pt;"><span style="mso-spacerun: yes;"><span lang="EN" style="font-family: "times new roman" , "serif"; font-size: 12.0pt;">
§21. Mons. The structure of the shards. 40</span></span></span></span></b></h2>
<h2>
<b><span style="font-weight: normal;"><span lang="EN-US" style="color: windowtext; font-size: 10.0pt; mso-ansi-language: EN-US; mso-font-kerning: 0pt;"><span style="mso-spacerun: yes;"><span lang="EN" style="font-family: "times new roman" , "serif"; font-size: 12.0pt;">
§22. <span style="font-size: large;">Mons cosmology</span>. 41</span></span></span></span></b></h2>
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<span lang="EN-US" style="color: windowtext; font-size: 8.0pt; mso-ansi-language: EN-US; mso-font-kerning: 0pt;"><span style="mso-spacerun: yes;"> </span></span><span lang="EN-US" style="color: windowtext; font-size: 8.0pt; mso-ansi-language: EN-US; mso-font-kerning: 0pt;"><span style="mso-spacerun: yes;"><img alt="File:Nuclear set a.png" data-file-height="741" data-file-width="1024" height="579" src="https://upload.wikimedia.org/wikipedia/commons/thumb/a/a9/Nuclear_set_a.png/800px-Nuclear_set_a.png" width="800" /> </span></span><br />
<span lang="EN-US" style="color: windowtext; font-size: 8.0pt; mso-ansi-language: EN-US; mso-font-kerning: 0pt;"><span style="mso-spacerun: yes;"> </span></span><span lang="EN-US" style="color: windowtext; font-size: 8.0pt; mso-ansi-language: EN-US; mso-font-kerning: 0pt;"><span style="mso-spacerun: yes;"><img alt="File:Nuclear set b.png" data-file-height="741" data-file-width="1024" height="579" src="https://upload.wikimedia.org/wikipedia/commons/thumb/2/2a/Nuclear_set_b.png/800px-Nuclear_set_b.png" width="800" /> </span><span style="mso-spacerun: yes;"> </span></span></div>
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<span lang="EN-US" style="color: windowtext; font-size: 10.0pt; mso-ansi-language: EN-US; mso-font-kerning: 0pt;"><span style="mso-spacerun: yes;"> </span><i style="mso-bidi-font-style: normal;"><span style="mso-spacerun: yes;"> </span><span style="mso-spacerun: yes;"> </span><span class="GramE">Summary.</span></i></span><i style="mso-bidi-font-style: normal;"><span lang="EN-US" style="color: black; font-size: 8.0pt;"></span></i></div>
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<span lang="EN-US" style="color: windowtext; font-size: 10.0pt; mso-ansi-language: EN-US; mso-font-kerning: 0pt;"><span style="mso-spacerun: yes;"> </span></span><span lang="EN-US" style="color: black; font-size: 10.0pt;"></span></div>
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<span lang="EN-US" style="color: windowtext; font-size: 10.0pt; mso-ansi-language: EN-US; mso-font-kerning: 0pt;"><span style="mso-spacerun: yes;"> </span>In
this work the CLOSED ENUMERABLE SETS are submitted by the elementary
mechanical, evident, appreciable models. Such simplicity allows to
construct and check up adequate mathematical model, i.e. to systematize
and generalize characteristic properties of models and parts making her
and, having distributed these methods on natural objects, to offer a new
way of the description and research of the last.<span style="mso-spacerun: yes;"> </span>Symmetry of atomic nucleus there is one of consequences of the constructed theory.</span></div>
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<b><span lang="EN-US" style="color: windowtext; font-size: 10.0pt; mso-ansi-language: EN-US; mso-font-kerning: 0pt;">1. <span style="font-size: large;">The closed enumerable set</span></span></b><span lang="EN-US" style="color: windowtext; font-size: 10.0pt; mso-ansi-language: EN-US; mso-font-kerning: 0pt;"><span style="font-size: large;">: models, mathematics, physics</span>.</span></div>
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<span lang="EN-US" style="color: windowtext; font-size: 10.0pt; mso-ansi-language: EN-US; mso-font-kerning: 0pt;"><span style="font-size: large; mso-spacerun: yes;"> </span><span style="font-size: large;">The closed enumerable sets of two-dimensional models</span> (structures) M, having form P<sub>m</sub> and consisting of internal elements such as N<sub>m</sub> and D<sub>m</sub>= <span class="GramE">f(</span>P<sub>m</sub>, N<sub>m</sub>) is studied, i.e.: M(P<sub>m</sub>, D<sub>m</sub>, N<sub>m </sub>). </span><span lang="EN-US" style="color: black; font-size: 10.0pt;">For </span><span lang="EN-US" style="color: windowtext; font-size: 10.0pt; mso-ansi-language: EN-US; mso-font-kerning: 0pt;">N<sub>m</sub></span><span lang="EN-US" style="color: black; font-size: 10.0pt;"> from 0 to 111 set of models </span><span lang="EN-US" style="color: windowtext; font-size: 10.0pt; mso-ansi-language: EN-US; mso-font-kerning: 0pt;">M can be placed in cells of some periodic table. The set ordered on the table, allocates internal elements of model N<sub>m</sub>
which of concrete physical properties: A, B, C, E such, that
inter-element interactions in each of structures are completely
described by nine quantum of interaction: A^A, A^B, A^C, B^B, B^C, B^E,
C^C, C^E, E^E. These sizes form triangular 4х4 matrix T = [t<sub> <span class="SpellE">i</span>, j</sub>] which is a constant of the table.</span></div>
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<span lang="EN-US" style="color: windowtext; font-size: 10.0pt; mso-ansi-language: EN-US; mso-font-kerning: 0pt;"><span style="mso-spacerun: yes;"> </span>Each
model is characterized by 15 sizes, and only 4 of them: e, g, b, and k
are independent and determine structural symmetry. Through the allocated
factors all other properties of model are expressed: structural – N<sub>m</sub>, P<sub>m</sub>, etc.; mathematical – coordinate system, coordinates N<sub>m</sub>, etc.; physical – properties<sub> </sub>N<sub>m</sub>, number of quantum’s of interaction n<sub> AA</sub>, n<sub> AB</sub>,... The Last form a symmetric triangular matrix 4х4 [n <span class="SpellE"><sub>j<span class="GramE">,k</span></sub></span>] <sub>m</sub> which is a constant of concrete model.</span></div>
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<span lang="EN-US" style="color: windowtext; font-size: 10.0pt; mso-ansi-language: EN-US; mso-font-kerning: 0pt;"><span style="mso-spacerun: yes;"> </span>The trace from multiplication of matrix constants of the table and model determines energy of model:</span><span lang="EN-US" style="color: black; font-size: 8.0pt;"></span></div>
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<span lang="EN-US" style="color: windowtext; font-size: 10.0pt; mso-ansi-language: EN-US; mso-font-kerning: 0pt;"><span style="mso-spacerun: yes;"> </span><span class="SpellE"><span class="GramE">Tr</span></span> ([t <span class="SpellE"><sub>i</sub></span><sub>, j</sub>] · [n <sub>j, k</sub>] <sub>m</sub>) = D<sub>m </sub>· </span><span class="apple-style-span"><span style="color: black; font-size: 10.0pt;">Δ</span></span><span style="mso-ansi-language: EN-US;"> </span><span lang="EN-US" style="color: black; font-size: 8.0pt;"></span></div>
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<span lang="EN-US" style="color: windowtext; font-size: 10.0pt; mso-ansi-language: EN-US; mso-font-kerning: 0pt;"><span style="mso-spacerun: yes;"> </span><span style="mso-spacerun: yes;"> </span></span><span lang="EN-US" style="color: black; font-size: 8.0pt;"></span></div>
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<span lang="EN-US" style="color: windowtext; font-size: 10.0pt; mso-ansi-language: EN-US; mso-font-kerning: 0pt;">Here </span><span class="apple-style-span"><span style="color: black; font-size: 10.0pt;">Δ</span></span><span style="mso-ansi-language: EN-US;"> </span><span lang="EN-US" style="color: windowtext; font-size: 10.0pt; mso-ansi-language: EN-US; mso-font-kerning: 0pt;">- the energy constant of the table and all quantum of interaction are proportional to her value.<span style="mso-spacerun: yes;"> </span>The
structure is dynamical object with the big number of the static and
excited conditions. Transition from one static condition in another
occurs through the excited condition. For concrete structure with set<sub> </sub>N<sub>m</sub>,<sub> </sub>static conditions differ in sizes<sub> </sub>P<sub>m</sub>, D<sub>m</sub>,<sub> </sub>factors
of symmetry and a set of quantum of interaction. The energy spectrum of
model is discrete and is caused by change of number D<sub>m</sub> at
transitions between conditions. Presence of opposite conditions of
models (static and excited) promotes their disorder and association. </span></div>
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<span lang="EN-US" style="color: windowtext; font-size: 10.0pt; mso-ansi-language: EN-US; mso-font-kerning: 0pt;"><span style="mso-spacerun: yes;"> </span>The
excited conditions of structures submit to the same tabulated laws and
are characterized by numbers of filling a - layers (orbits): n (1-6) and
m (1-a). The similar behaviors characterize also the subsequent of
excitation. The maximal number excited each structure is determined by
difference N-P.</span></div>
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<span lang="EN-US" style="color: windowtext; font-size: 10.0pt; mso-ansi-language: EN-US; mso-font-kerning: 0pt;"><span style="mso-spacerun: yes;"> </span>2. <b>Correlation</b>.<span style="font-size: small;"> Structural symmetry of atomic nucleus is physical example </span>of the UMTAE.</span></div>
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<span lang="EN-US" style="color: windowtext; font-size: 10.0pt; mso-ansi-language: EN-US; mso-font-kerning: 0pt;"><span style="mso-spacerun: yes;"> </span><b><span style="font-size: small;">The
studied CLOSED ENUMERABLE SETS of models is a real set of physical
objects and is similar on a structure to molecules and atoms nucleus.
Therefore it is possible to admit, that the laws revealed for one
objects, are the general. For an example it is possible to take some
elements from Periodic system of elements of D.I. Mendeleyev and using
modeling formulas to reveal structures conterminous to them from the
modeling table. Really, let N coincides with a serial number of an
element or number of protons, then D or number of neutrons will be
determined by a difference between integer atoms mass A and N, i.e.
D=A-N. In such representation of 27 elements of Periodic system coincide
with structures from the modeling table under characteristics N, P, D,
but differ in factors of symmetry e, g, b, and k. If to take into
account isotopes, then the much more elements coincide. Nucleuses of
atoms have lower symmetry, i.e. insufficient number of neutrons.<span style="mso-spacerun: yes;"> </span>Assuming,
that the space outside of a nucleus has the neutron nature, does a
concept about expansion of the universe is more clearly.<span style="mso-spacerun: yes;"> </span>This
expansion occurs due to deformation of nucleus and disappearance of
heavy chemical elements. It is possible to tell, that the nucleus has a
planetary structure. Further, <i style="mso-bidi-font-style: normal;">the Periodic system of elements of D.I. Mendeleyev should be characterized: matrix - </i>T<i style="mso-bidi-font-style: normal;"> and energy - </i></span></b></span><b><span class="apple-style-span" style="font-size: small;"><span style="color: black; font-size: 10.0pt;">Δ</span></span><span style="font-size: small;"><i style="mso-bidi-font-style: normal;"><span lang="EN-US" style="color: windowtext; font-size: 10.0pt; mso-ansi-language: EN-US; mso-font-kerning: 0pt;"> constants, and each chemical element</span></i><span lang="EN-US" style="color: windowtext; font-size: 10.0pt; mso-ansi-language: EN-US; mso-font-kerning: 0pt;"> <i>- coefficients of symmetry of atomic nucleus</i>. The electronic environment of atom is determined by structure of a nucleus, also his symmetry. </span></span></b></div>
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<span lang="EN-US" style="color: windowtext; font-size: 10.0pt; mso-ansi-language: EN-US; mso-font-kerning: 0pt;">3. <b>The purposes</b>.<span style="mso-spacerun: yes;"> </span>Algebra of the closed enumerable set is a rebus for intellectuals.</span><span lang="EN-US" style="color: black; font-size: 8.0pt;"></span></div>
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<br /></div>
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<span lang="EN-US" style="color: windowtext; font-size: 10.0pt; mso-ansi-language: EN-US; mso-font-kerning: 0pt;">The
special place in becoming and development of the theory is occupied
with mathematical methods. Internal space of model this closed
enumerable set N<sub>m</sub> with the actions w, i.e. algebra<i> </i><i style="mso-bidi-font-style: normal;">N<sub>m<span style="mso-spacerun: yes;"> </span></sub></i>= [N<sub>m</sub>, w] - Sector; and not structural space this open integer set N with the actions W, i.e. algebra<i> N</i>
= {N, W} - Natural algebra. Presences of two algebras are the objective
need, caused by existence of vacuum, which shares and unites models.
Then the theory of radiation and interaction of structures is reduced to
the decision of boundary tasks in system of two algebras. Energy of the
model is written down in a ring above system of real numbers, in other
algebra this record will look in another way. New algebraic systems
through a set of new actions display new types of interactions and their
properties. On this way it is possible to open new material forms:
fields, essences, appearances.</span></div>
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<br />
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<br />
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<span lang="EN-US" style="mso-ansi-language: EN-US;">Оглавление</span></div>
<div class="MsoNormal">
Теория ядерных множеств</div>
<div class="MsoNormal">
§1.<span style="mso-spacerun: yes;"> </span>Ядерное
множество.<span style="mso-tab-count: 1;"> </span>2</div>
<div class="MsoNormal">
§2.<span style="mso-spacerun: yes;"> </span>Систематизация.
Определения.<span style="mso-tab-count: 1;"> </span>4</div>
<div class="MsoNormal">
§3.<span style="mso-spacerun: yes;"> </span>Общие структурные
характеристики.<span style="mso-tab-count: 1;"> </span><span lang="EN-US" style="mso-ansi-language: EN-US;">6</span></div>
<div class="MsoNormal">
<span lang="EN-US" style="mso-ansi-language: EN-US;">§4.<span style="mso-spacerun: yes;"> </span>Закономерности. Табличная систематизация.<span style="mso-tab-count: 1;"> </span>6</span></div>
<div class="MsoNormal">
§5.<span style="mso-spacerun: yes;"> </span>Структуризация.
Линейные разложения .<span style="mso-tab-count: 1;"> </span>7</div>
<div class="MsoNormal">
§6.<span style="mso-spacerun: yes;"> </span>Коэффициенты
симметрии. Симметрия формы.<span style="mso-tab-count: 1;"> </span>8</div>
<div class="MsoNormal">
§7.<span style="mso-spacerun: yes;"> </span>Базис ядерного
пространства.<span style="mso-tab-count: 1;"> </span>11</div>
<div class="MsoNormal">
§8.<span style="mso-spacerun: yes;"> </span>Свойства
вложенных структур.<span style="mso-tab-count: 1;"> </span>15</div>
<div class="MsoNormal">
§9.<span style="mso-spacerun: yes;"> </span>Межэлементные
связи и симметрия.<span style="mso-tab-count: 1;"> </span>20</div>
<div class="MsoNormal">
§10.<span style="mso-spacerun: yes;"> </span>Квант
взаимодействия. Энергия ядра.<span style="mso-tab-count: 1;"> </span>21</div>
<div class="MsoNormal">
§11.<span style="mso-spacerun: yes;"> </span>Матрицы таблицы
и ядра.<span style="mso-tab-count: 1;"> </span>22</div>
<div class="MsoNormal">
§12.<span style="mso-spacerun: yes;"> </span>Перестройка
ядер множества.<span style="mso-tab-count: 1;"> </span>24</div>
<div class="MsoNormal">
§13.<span style="mso-spacerun: yes;"> </span>Объединение и
распад ядер.<span style="mso-tab-count: 1;"> </span>25</div>
<div class="MsoNormal">
§14.<span style="mso-spacerun: yes;"> </span>Основное
возбужденное состояние структуры.<span style="mso-tab-count: 1;"> </span>27</div>
<div class="MsoNormal">
§15.<span style="mso-spacerun: yes;"> </span>Таблица основных
динамических состояний.<span style="mso-tab-count: 1;"> </span>29</div>
<div class="MsoNormal">
§16.<span style="mso-spacerun: yes;"> </span>Симметрия
атомных ядер.<span style="mso-tab-count: 1;"> </span>32</div>
<div class="MsoNormal">
§17.<span style="mso-spacerun: yes;"> </span>Туннельные
взаимодействия<span style="mso-tab-count: 1;"> </span>35</div>
<div class="MsoNormal">
§18.<span style="mso-spacerun: yes;"> </span>Обменные
взаимодействия.<span style="mso-tab-count: 1;"> </span>37</div>
<div class="MsoNormal">
§19.<span style="mso-spacerun: yes;"> </span>Взаимодействия в
динамических состояниях<span style="mso-tab-count: 1;"> </span>39</div>
<div class="MsoNormal">
§20.<span style="mso-spacerun: yes;"> </span>Осколки и чипы.<span style="mso-tab-count: 1;"> </span>39</div>
<div class="MsoNormal">
§21.<span style="mso-spacerun: yes;"> </span>Моны. Структура
осколка.<span style="mso-tab-count: 1;"> </span><span lang="EN-US" style="mso-ansi-language: EN-US;">40</span></div>
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<span lang="EN-US" style="mso-ansi-language: EN-US;">§22.<span style="mso-spacerun: yes;"> </span>Моновская космология.<span style="mso-tab-count: 1;"> </span>41</span></div>
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