<?xml version="1.0" encoding="UTF-8"?><!DOCTYPE article  PUBLIC "-//NLM//DTD Journal Publishing DTD v3.0 20080202//EN" "http://dtd.nlm.nih.gov/publishing/3.0/journalpublishing3.dtd"><article xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink" dtd-version="3.0" xml:lang="en" article-type="research article"><front><journal-meta><journal-id journal-id-type="publisher-id">JMP</journal-id><journal-title-group><journal-title>Journal of Modern Physics</journal-title></journal-title-group><issn pub-type="epub">2153-1196</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/jmp.2016.71013</article-id><article-id pub-id-type="publisher-id">JMP-62955</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>Physics&amp;Mathematics</subject></subj-group></article-categories><title-group><article-title>
 
 
  Confining Potential and Mass of Elementary Particles
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>ev</surname><given-names>I. Buravov</given-names></name><xref ref-type="aff" rid="aff1"><sub>1</sub></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib></contrib-group><aff id="aff1"><label>1</label><addr-line>Institute of Problems of Chemical Physics RAS, Chernogolovka, Russia</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>buravov@icp.ac.ru</email></corresp></author-notes><pub-date pub-type="epub"><day>06</day><month>01</month><year>2016</year></pub-date><volume>07</volume><issue>01</issue><fpage>129</fpage><lpage>133</lpage><history><date date-type="received"><day>14</day>	<month>July</month>	<year>2015</year></date><date date-type="rev-recd"><day>accepted</day>	<month>18</month>	<year>January</year>	</date><date date-type="accepted"><day>22</day>	<month>January</month>	<year>2016</year></date></history><permissions><copyright-statement>&#169; Copyright  2014 by authors and Scientific Research Publishing Inc. </copyright-statement><copyright-year>2014</copyright-year><license><license-p>This work is licensed under the Creative Commons Attribution International License (CC BY). http://creativecommons.org/licenses/by/4.0/</license-p></license></permissions><abstract><p><html>
 <head></head>
 
  In this paper we consider a model in which the masses of elementary particles are formed and stabilized thanks to confining potential, which is caused by recoil momentum at emission of specific virtual bosons by particle itself. The calculation of this confining potential 
  <em>Ф</em>(
  <em>R</em>) is carried out. It is shown that 
  <em>Ф</em>(
  <em>R</em>) may be in the form const 
  <img src="Edit_40853e7b-80ed-43e8-866b-82c5b9dec430.jpg" alt="" /> or const 
  <img src="Edit_2344b97a-f0ca-48dd-8413-fb8d357d3460.jpg" alt="" /> depending on continuous or discrete nature of the spectrum of emitted bosons.
 
</html></p></abstract><kwd-group><kwd>Confining Potential</kwd><kwd> Origin of Mass of Particle</kwd><kwd> Stabilizing of Particle Mass</kwd><kwd> Virtual Bosons</kwd><kwd> Spherical Bosonic Wave</kwd><kwd> Origin of Neutrino Masses</kwd><kwd> Neutrino Mass Formula</kwd><kwd> Calculation of Neutrino Masses</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>In the article the model of formation of mass of elementary particles is offered as a result of emitting of the special virtual bosons as spherical waves (conditionally we will name them as the bosons of Higgs). It is supposed here that confining potential which is necessary for stabilizing of particle mass appears because of effect of impulse recoil, especially for electron, muon, pion, kaon and neutrino.</p><p>In due time Poincare, proceeding from common sense, entered supposition about a presence in the structure of electron of some elastic elements due to which the charge of electron holds out in a small volume. This model was later used by many authors. We will consider it more detailed, following [<xref ref-type="bibr" rid="scirp.62955-ref1">1</xref>] [<xref ref-type="bibr" rid="scirp.62955-ref2">2</xref>] .</p><p>In accordance with [<xref ref-type="bibr" rid="scirp.62955-ref1">1</xref>] [<xref ref-type="bibr" rid="scirp.62955-ref2">2</xref>] virtual rest energy of electron Е consists of two parts: surface energy of elastic shell <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x6.png" xlink:type="simple"/></inline-formula> and electrostatic energy of the charged surface<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x7.png" xlink:type="simple"/></inline-formula>, where σ is the coefficient of surface tension of the shell, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x8.png" xlink:type="simple"/></inline-formula>is its radius, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x9.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x10.png" xlink:type="simple"/></inline-formula>is dielectric constant of vacuum, q is an electron charge (in units of SI). Virtual rest energy of such system is equal to:</p><disp-formula id="scirp.62955-formula106"><label>(1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/13-7502348x11.png"  xlink:type="simple"/></disp-formula><p>The radius of electron, corresponding to a minimum of energy (1) of the system, is determined from equation <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x12.png" xlink:type="simple"/></inline-formula> and is equal to:</p><disp-formula id="scirp.62955-formula107"><label>(2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/13-7502348x13.png"  xlink:type="simple"/></disp-formula><p>From Equations (1) and (2) the mass of electron is</p><p><img src="http://html.scirp.org/file/13-7502348x15.png" /><img src="http://html.scirp.org/file/13-7502348x14.png" /> (3)</p><p>It is possible also to write down that<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x16.png" xlink:type="simple"/></inline-formula>, where a σ value was determined in [<xref ref-type="bibr" rid="scirp.62955-ref3">3</xref>] with using the value of neutral pion mass<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x17.png" xlink:type="simple"/></inline-formula>:</p><disp-formula id="scirp.62955-formula108"><label>(4)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/13-7502348x18.png"  xlink:type="simple"/></disp-formula><p>and coefficient<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x19.png" xlink:type="simple"/></inline-formula>.</p><p>In Equation (1) the value <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x20.png" xlink:type="simple"/></inline-formula> obviously fulfills the role of confining potential due to which the mass of electron is stabilized.</p><p>Preliminary we will represent information about the calculation of the masses for several elementary particles and then pass to more detailed consideration of confining potential.</p><p>In [<xref ref-type="bibr" rid="scirp.62955-ref3">3</xref>] the calculation of the ratio for the masses of the particles e, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x21.png" xlink:type="simple"/></inline-formula>was made on the basis of starting model assumption that the stopped muon, pion and kaon can be represented as spherical resonators for quanta of virtual neutrinos excited into an elastic lepton shell with surface energy<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x21.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x22.png" xlink:type="simple"/></inline-formula>, where R is a</p><p>radius of elastic shell, σ is the coefficient of surface tension, the same that is in Equations (1)-(4). In [<xref ref-type="bibr" rid="scirp.62955-ref3">3</xref>] it was shown that virtual rest energy of these particles can be written down in general case in some more complex forms, than those for an electron:</p><disp-formula id="scirp.62955-formula109"><label>(5)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/13-7502348x23.png"  xlink:type="simple"/></disp-formula><p>where ρ is a radius of the compressed electric cloud, and N is the number of neutrino quanta that is determined from the decay scheme: N = 2 for muon, 3―for pion, and 21―for kaon. The masses of particles and characteristic sizes <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x24.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x24.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x25.png" xlink:type="simple"/></inline-formula> are determined in general case at minimization of virtual rest-energy (5) on R and ρ. Calculated in [<xref ref-type="bibr" rid="scirp.62955-ref3">3</xref>] values of the masses of e, μ, π<sup>0 </sup>and K<sup>0</sup> are in relation 0.547: 105.707: 134.963: 493.87 (MeV) (by attachment to mass of neutral pion), that is in accord with experience data. It is shown that the masses of all considered particles, as well as for an electron, are proportional to the square of their equilibrium size<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x24.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x25.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x26.png" xlink:type="simple"/></inline-formula>:</p><disp-formula id="scirp.62955-formula110"><label>(6)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/13-7502348x27.png"  xlink:type="simple"/></disp-formula><p>It is assumed in the Standard Model that the masses of row of elementary particles can be represented in the form:</p><p><img data-original="http://html.scirp.org/file/13-7502348x29.png" /><img data-original="http://html.scirp.org/file/13-7502348x28.png" /> (7)</p><p>where H = 246 GeV is the characteristic energy in the model of Higgs [<xref ref-type="bibr" rid="scirp.62955-ref4">4</xref>] [<xref ref-type="bibr" rid="scirp.62955-ref5">5</xref>] , <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x30.png" xlink:type="simple"/></inline-formula>is a dimensionless factor, characteristic for a certain particle with mass of M. We can make compatible formulas (6) and (7) for the masses, if preliminary we equate right parts of Equations (6) and (7); that results to:</p><disp-formula id="scirp.62955-formula111"><label>(8)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/13-7502348x31.png"  xlink:type="simple"/></disp-formula><p>where unknown size<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x32.png" xlink:type="simple"/></inline-formula>, that is comparable to 1/2 the Compton wave- length of electron<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x32.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x33.png" xlink:type="simple"/></inline-formula>.</p><p>The result of the Formula (6) was used in [<xref ref-type="bibr" rid="scirp.62955-ref6">6</xref>] for the calculation of neutrino masses <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x34.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x34.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x35.png" xlink:type="simple"/></inline-formula>, for which the square of their electromagnetic radius was found in works [<xref ref-type="bibr" rid="scirp.62955-ref7">7</xref>] - [<xref ref-type="bibr" rid="scirp.62955-ref9">9</xref>] . It is shown in them that neutrinos of all types have a complex internal structure as a consequence of the virtual transitions <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x34.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x36.png" xlink:type="simple"/></inline-formula>, where the lepton index <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x34.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x36.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x37.png" xlink:type="simple"/></inline-formula> means e, μ or τ; W are intermediate vector bosons, which are carriers of the weak interaction with mass М<sub>w</sub> = 80.4 GeV [<xref ref-type="bibr" rid="scirp.62955-ref10">10</xref>] . Taking into account such virtual transitions in [<xref ref-type="bibr" rid="scirp.62955-ref7">7</xref>] - [<xref ref-type="bibr" rid="scirp.62955-ref9">9</xref>] , it is found that the square of the electromagnetic radius of neutrino is equal to:</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x38.png" xlink:type="simple"/></inline-formula> (9),</p><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x39.png" xlink:type="simple"/></inline-formula> is the weak interaction constant, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x39.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x40.png" xlink:type="simple"/></inline-formula>, and numerical constant η is 1 - 2. For a mean value <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x39.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x40.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x41.png" xlink:type="simple"/></inline-formula> taking into account <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x39.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x40.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x41.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x42.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x39.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x40.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x41.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x42.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x43.png" xlink:type="simple"/></inline-formula> from (9) it follows that the characteristic values of the squared neutrino radii are equal to:</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x44.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x44.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x45.png" xlink:type="simple"/></inline-formula>,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x44.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x45.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x46.png" xlink:type="simple"/></inline-formula> (10)</p><p>To define the masses of neutrino in [<xref ref-type="bibr" rid="scirp.62955-ref6">6</xref>] simple suppositions are made:</p><p>1. Although neutrinos do not have an electric charge, they seems to have small electrostatic energy due to that spacial distributions of diverse charges produced by virtual pairs <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x47.png" xlink:type="simple"/></inline-formula> are slightly different. In this case the electrostatic energy of neutrino has a value<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x47.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x48.png" xlink:type="simple"/></inline-formula>, where r is a virtual electromagnetic radius of neutrino, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x47.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x48.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x49.png" xlink:type="simple"/></inline-formula>is an unknown small parameter related to the distribution of charges in a structure of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x47.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x48.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x49.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x50.png" xlink:type="simple"/></inline-formula>.<sub> </sub></p><p>2. Virtual rest-energy of neutrino consists of the confining potential <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x51.png" xlink:type="simple"/></inline-formula> and electrostatic energy:</p><disp-formula id="scirp.62955-formula112"><label>(11)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/13-7502348x52.png"  xlink:type="simple"/></disp-formula><p>3. The value of s is identical for all neutrinos.</p><p>Similarly, as for an electron, mass of neutrino would be found at being of a minimum of virtual energy (11):</p><disp-formula id="scirp.62955-formula113"><label>(12)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/13-7502348x53.png"  xlink:type="simple"/></disp-formula><p>but as a value <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x54.png" xlink:type="simple"/></inline-formula><sup> </sup>is unknown, for determination of the neutrino masses we will take advantage of theoretical results [<xref ref-type="bibr" rid="scirp.62955-ref7">7</xref>] - [<xref ref-type="bibr" rid="scirp.62955-ref9">9</xref>] for the square of electromagnetic radius of neutrino <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x54.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x55.png" xlink:type="simple"/></inline-formula> and of Formula (6). Thus, putting the found values (10) for <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x54.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x55.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x56.png" xlink:type="simple"/></inline-formula> in Formula (6) instead of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x54.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x55.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x56.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x57.png" xlink:type="simple"/></inline-formula>, we find that the masses of neutrino are equal to:</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x58.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x58.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x59.png" xlink:type="simple"/></inline-formula>,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x58.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x59.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x60.png" xlink:type="simple"/></inline-formula> (13)</p><p>Similar values for three neutrino mass eigenstates (ν<sub>1</sub>, ν<sub>2</sub>, ν<sub>3</sub>) were received in [<xref ref-type="bibr" rid="scirp.62955-ref11">11</xref>] on the basis of Super-Ka- miokande experimental results [<xref ref-type="bibr" rid="scirp.62955-ref12">12</xref>] , inventively solving system of two equations with 3 unknown quantities, if supposing the case of inverted mass spectrum.</p><p>Values <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x61.png" xlink:type="simple"/></inline-formula> for a neutrino also can be found from Formula (8) at the substitution of values <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x61.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x62.png" xlink:type="simple"/></inline-formula> instead of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x61.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x62.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x63.png" xlink:type="simple"/></inline-formula>:</p><disp-formula id="scirp.62955-formula114"><label>(14)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/13-7502348x64.png"  xlink:type="simple"/></disp-formula><p>We will notice that as <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x65.png" xlink:type="simple"/></inline-formula> [<xref ref-type="bibr" rid="scirp.62955-ref5">5</xref>] [<xref ref-type="bibr" rid="scirp.62955-ref13">13</xref>] , taking into account Equations (4), (6) and (9) we get a general formula for the masses of neutrino in the form:</p><disp-formula id="scirp.62955-formula115"><label>(15)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/13-7502348x66.png"  xlink:type="simple"/></disp-formula><p>where a dimensionless factor <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x67.png" xlink:type="simple"/></inline-formula> is equal to:</p><disp-formula id="scirp.62955-formula116"><label>(16)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/13-7502348x68.png"  xlink:type="simple"/></disp-formula><p>θ<sub>w</sub>―is the angle of Weinberg, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x69.png" xlink:type="simple"/></inline-formula>and all 3 dimensionless coefficients: <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x69.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x70.png" xlink:type="simple"/></inline-formula>and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x69.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x70.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x71.png" xlink:type="simple"/></inline-formula> are much smaller than 1. The values <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x69.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x70.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x71.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x72.png" xlink:type="simple"/></inline-formula> are determined from Equation (12):</p><disp-formula id="scirp.62955-formula117"><label>(17)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/13-7502348x73.png"  xlink:type="simple"/></disp-formula><p>and are equal to:</p><disp-formula id="scirp.62955-formula118"><label>(18)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/13-7502348x74.png"  xlink:type="simple"/></disp-formula><p>In Equation (5), also as in (1), the value <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x75.png" xlink:type="simple"/></inline-formula> plays a role of confining potential thanks to which the mass of the elementary particle is stabilized. This conception of the mass origin is simple and clear: complete internal energy is equal to Mc<sup>2</sup>; however, physical reason for the origin of confining potential is not clear. A model is offered in this article, explaining the origin of this potential and holding pressure due to the effect of impulse recoil of the special emitted virtual bosons.</p><p>So then for the ground of this model we will enter next suppositions:</p><p>1. By analogy with the model of Poincare we will suppose that every elementary particle has confining potential<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x76.png" xlink:type="simple"/></inline-formula>, except for photons and gravitons. It is assumed that rest-energy of particle consists of confining potential, kinetic energy of internal motion, energy of the internal fields and electrostatic energy of the internal charges.</p><p>2. Every elementary particle radiates the special virtual bosons as spherical waves<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x77.png" xlink:type="simple"/></inline-formula>. Here <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x77.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x78.png" xlink:type="simple"/></inline-formula> is a wave-number of virtual boson, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x77.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x78.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x79.png" xlink:type="simple"/></inline-formula>is its angular frequency, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x77.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x78.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x79.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x80.png" xlink:type="simple"/></inline-formula>is distance from the center of a particle<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x77.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x78.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x79.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x80.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x81.png" xlink:type="simple"/></inline-formula>, A is a normalizing constant not substantial for further consideration.</p><p>3. We will suppose that mass of such bosons <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x82.png" xlink:type="simple"/></inline-formula> is much more than masses of intermediate vector bosons W and Z<sup>0</sup>, where Z<sup>0</sup> is a neutral carrier of the weak interaction with mass 91.2 GeV [<xref ref-type="bibr" rid="scirp.62955-ref10">10</xref>] . Then a time of exis-</p><p>tence of such virtual bosons τ is much smaller than <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x83.png" xlink:type="simple"/></inline-formula> and distance of their run <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x83.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x84.png" xlink:type="simple"/></inline-formula> from the surface of elementary particle is much smaller than<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x83.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x84.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x85.png" xlink:type="simple"/></inline-formula>.</p><p>4. Every elementary particle is the inexhaustible source of such virtual spherical waves, but the mass of the particle-source does not decrease, because virtual bosons through an instant τ return back into a source, due to interacting with the fields of vacuum.</p><p>5. We suppose that complete amount of the bosons emitted by a particle in a unit of time N<sub>H</sub> is proportional to area of particle surface with a coefficient<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x86.png" xlink:type="simple"/></inline-formula>, characterizing intensity of radiation for the certain group of particles:<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x86.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x87.png" xlink:type="simple"/></inline-formula>.</p><p>As every moving wave carries an impulse, it ensues from these suppositions, that on the surface of elementary particle because of the effect of impulse recoil, spherical waves are creating holding force of pressure F(R) and confining potential</p><disp-formula id="scirp.62955-formula119"><graphic  xlink:href="http://html.scirp.org/file/13-7502348x88.png"  xlink:type="simple"/></disp-formula><p>We will consider 2 cases for forms of boson spectrum:</p><p>a) the emitted bosons have a continuous spectrum of radiation in the interval of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x89.png" xlink:type="simple"/></inline-formula> from 0 to <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x89.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x90.png" xlink:type="simple"/></inline-formula> with the function of probability distribution<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x89.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x90.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x91.png" xlink:type="simple"/></inline-formula>, where<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x89.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x90.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x91.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x92.png" xlink:type="simple"/></inline-formula>. As be shown, in this case confining potential is proportional to<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x89.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x90.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x91.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x92.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x93.png" xlink:type="simple"/></inline-formula>.</p><p>b) the emitted bosons have a discrete spectrum of radiation : <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x94.png" xlink:type="simple"/></inline-formula>with the function of probability distribution<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x94.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x95.png" xlink:type="simple"/></inline-formula>. In this case the confining potential appears to be proportional to R<sup>2</sup>.</p><p>Let’s consider the case of a). We will enter the condition of normalizing for <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x96.png" xlink:type="simple"/></inline-formula> so that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x96.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x97.png" xlink:type="simple"/></inline-formula>. Then the number of impulses in an interval from <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x96.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x97.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x98.png" xlink:type="simple"/></inline-formula> to <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x96.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x97.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x98.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x99.png" xlink:type="simple"/></inline-formula> is equal to<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x96.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x97.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x98.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x99.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x100.png" xlink:type="simple"/></inline-formula>, and complete force of pressure, operating on a surface 4πR<sup>2</sup> is equal to:</p><disp-formula id="scirp.62955-formula120"><label>(19)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/13-7502348x101.png"  xlink:type="simple"/></disp-formula><p>Consequently confining potential for the case of a) is:</p><disp-formula id="scirp.62955-formula121"><label>(20)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/13-7502348x102.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x103.png" xlink:type="simple"/></inline-formula> is a quantum-mechanical mean value of k.</p><p>For the case of b) we will enter the condition of normalizing for<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x104.png" xlink:type="simple"/></inline-formula>:<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x104.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x105.png" xlink:type="simple"/></inline-formula>. In this case total force of pressure on a surface 4πR<sup>2</sup> is equal to:</p><disp-formula id="scirp.62955-formula122"><label>(21)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/13-7502348x106.png"  xlink:type="simple"/></disp-formula><p>The sum <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x107.png" xlink:type="simple"/></inline-formula> in Formula (21) by definition is equal to <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x107.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x108.png" xlink:type="simple"/></inline-formula> where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x107.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x108.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x109.png" xlink:type="simple"/></inline-formula> is a quantum-mechanical mean value of n. As a result the confining potential <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x107.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x108.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x109.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/13-7502348x110.png" xlink:type="simple"/></inline-formula> is:</p><disp-formula id="scirp.62955-formula123"><label>(22)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/13-7502348x111.png"  xlink:type="simple"/></disp-formula><p>Thus, in the article it’s assumed that every elementary particle produces the special bosonic field that is present only in a thin layer at the surface of a particle. It is shown that this field can create the confining potential, stabilizing the mass of particle during the time of its life.</p></sec><sec id="s2"><title>Cite this paper</title><p>Lev I.Buravov, (2016) Confining Potential and Mass of Elementary Particles. Journal of Modern Physics,07,129-133. doi: 10.4236/jmp.2016.71013</p></sec></body><back><ref-list><title>References</title><ref id="scirp.62955-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Dirac, P.A.M. (1962) Proceedings of the Royal Society of London, Series A, Mathematical and Physical Sciences, 268, 57-67. http://dx.doi.org/10.1098/rspa.1962.0124</mixed-citation></ref><ref id="scirp.62955-ref2"><label>2</label><mixed-citation publication-type="other" xlink:type="simple">Feynman, R., Leighton, R. and Sands, M. (1964) The Feynman Lectures on Physics, Vol. 2. Addison Wesley Pub. 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