<?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.2014.56058</article-id><article-id pub-id-type="publisher-id">JMP-45403</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>
 
 
  Mass Creation from Extra Dimensions
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>ao</surname><given-names>Vong Duc</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Nguyen</surname><given-names>Mong Giao</given-names></name><xref ref-type="aff" rid="aff2"><sup>2</sup></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib></contrib-group><aff id="aff1"><addr-line>Institute of Physics, Hanoi, Vietnam</addr-line></aff><aff id="aff2"><addr-line>Hung Vuong University, Ho Chi Minh City, Vietnam</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>nmgiao2011@yahoo.com.vn(NMG)</email>;</corresp></author-notes><pub-date pub-type="epub"><day>09</day><month>04</month><year>2014</year></pub-date><volume>05</volume><issue>06</issue><fpage>477</fpage><lpage>482</lpage><history><date date-type="received"><day>2</day>	<month>March</month>	<year>2014</year></date><date date-type="rev-recd"><day>29</day>	<month>March</month>	<year>2014</year>	</date><date date-type="accepted"><day>15</day>	<month>April</month>	<year>2014</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>
 
 
   In this work we consider a mechanism for mass creation based on the periodicity condition dictated from the compactification of extradimensions. It is shown that the existence and the compactification of extradimensions are the origin for creating particle mass in ordinary 4-dimensional space-time. Mass of Higgs particles themselves would be also originated from the geometric topology of extradimensions. 
 
</p></abstract><kwd-group><kwd>Origin of Mass</kwd><kwd> Mass of Higg Particles</kwd><kwd> Extra Dimensions</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>The existence of space-time extradimensions has been a subject of intensive research study during the last decades [<xref ref-type="bibr" rid="scirp.45403-ref1">1</xref>] -[<xref ref-type="bibr" rid="scirp.45403-ref3">3</xref>] .</p><p>The topology of extradimensions, especially their compactification, plays a crucial role in many physical aspects, mostly in the construction of various models of unified theory of interactions, such as superstring theory, extended general relativity, and so on [<xref ref-type="bibr" rid="scirp.45403-ref4">4</xref>] -[<xref ref-type="bibr" rid="scirp.45403-ref7">7</xref>] .</p><p>It is worth noting, on the other hand, that it is in such approaches the particle mass always remains a problem of actual characters.</p><p>In this work we propose a mechanism for mass creation through the compactification of spacetime extradimensions. The crucial argument is the proposed periodicity condition dictated from the compactification of extra dimensions.</p><p>The original field functions depend on all space-time coordinate components including those for extradimensions, the ordinary field functions, ordinary 4-dimensional space-time considered as effective field functions obtained by integration of the original ones over extra space-time.</p><p>In Section 2, we present some general principles related to the compactification of extradimensions.</p><p>In Section 3, a mechanism for mass creation is treated.</p></sec><sec id="s2"><title>2. Periodicity Compactification Condition</title><p>For simplicity let us begin with the case of one extra dimension. Denote the 5-dimensional coordinate vector by x<sup>M</sup> with M =<inline-formula><inline-graphic xlink:href="tmlimages\18-7501780x\ddf6ca19-db20-4754-8d6b-fa2aa1d7f5ae.png" xlink:type="simple"/></inline-formula>, 5. The Greek indices<inline-formula><inline-graphic xlink:href="tmlimages\18-7501780x\012f5ea4-342f-4d69-a482-4885236e8d63.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="tmlimages\18-7501780x\c7233803-82df-48b0-8bbf-fa531799bc8d.png" xlink:type="simple"/></inline-formula>,&#183;&#183;&#183; will be used as conventional 4-dimensional Lorentz indices (0, 1, 2, and 3). We do not directly care from the extra dimensions is topologically compactified, but instead a specific periodicity condition is put on the field functions depending on extra dimensions, namely</p><disp-formula id="scirp.45403-formula46378"><label>(1)</label><graphic position="anchor" xlink:href="htmlimages\18-7501780x\86a5d837-754c-4b01-a071-1930f846f2dc.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="tmlimages\18-7501780x\a56f3f5a-5561-4923-80e3-b5a6ac5464d7.png" xlink:type="simple"/></inline-formula> is some parameter function depending on the compactification length L.</p><p>The condition (1) corresponds to the equation:</p><disp-formula id="scirp.45403-formula46379"><label>(2)</label><graphic position="anchor" xlink:href="htmlimages\18-7501780x\8a56e965-761b-4e5c-8a0e-26598906234f.png"  xlink:type="simple"/></disp-formula><p>With the relations:</p><disp-formula id="scirp.45403-formula46380"><label>(3)</label><graphic position="anchor" xlink:href="htmlimages\18-7501780x\75d327a6-217b-444e-90a3-c8414532661a.png"  xlink:type="simple"/></disp-formula><p>In general we can put</p><disp-formula id="scirp.45403-formula46381"><label>(4)</label><graphic position="anchor" xlink:href="htmlimages\18-7501780x\1d8392dc-0723-45f1-93aa-0818930a445a.png"  xlink:type="simple"/></disp-formula><p><img src="htmlimages\18-7501780x\b3a59b8f-515a-44ae-a3a7-8b75f068b99e.png" /></p><p>For neutral field, <inline-formula><inline-graphic xlink:href="tmlimages\18-7501780x\1014e0ff-a9fd-40a6-8ea1-cd8195b10f74.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="tmlimages\18-7501780x\629b5c8b-1292-4a37-b78d-121c1006ccd5.png" xlink:type="simple"/></inline-formula>is to be real and therefore <inline-formula><inline-graphic xlink:href="tmlimages\18-7501780x\465411eb-ddea-4d3b-b163-9b97ef34c8f3.png" xlink:type="simple"/></inline-formula></p><p>The periodicity condition (1) can be generalized for the case of arbitrary number of extra dimensions in the following manner.</p><p>For convenience we denote the extra dimension coordinates <inline-formula><inline-graphic xlink:href="tmlimages\18-7501780x\6743ad83-7bfb-43e8-97bb-5aa3e3136f36.png" xlink:type="simple"/></inline-formula> by <inline-formula><inline-graphic xlink:href="tmlimages\18-7501780x\2f515796-3e81-442d-ab74-58eaba9da1b9.png" xlink:type="simple"/></inline-formula> and write</p><disp-formula id="scirp.45403-formula46382"><label>(5)</label><graphic position="anchor" xlink:href="htmlimages\18-7501780x\15882d97-c8fe-4766-af3a-453bc2fa2440.png"  xlink:type="simple"/></disp-formula><p>The periodicity condition (1) is now generalized to be:</p><disp-formula id="scirp.45403-formula46383"><label>(6)</label><graphic position="anchor" xlink:href="htmlimages\18-7501780x\e81b77a3-8054-4e05-9c62-a82dedc4af53.png"  xlink:type="simple"/></disp-formula><p>and the corresponding Equation (2) becomes:</p><disp-formula id="scirp.45403-formula46384"><label>(7)</label><graphic position="anchor" xlink:href="htmlimages\18-7501780x\d108b019-8c16-497e-a874-cd8b29137d8b.png"  xlink:type="simple"/></disp-formula><p>with the relations:</p><disp-formula id="scirp.45403-formula46385"><label>(8)</label><graphic position="anchor" xlink:href="htmlimages\18-7501780x\22f0784e-7f2e-4221-b28c-a6848f6103b8.png"  xlink:type="simple"/></disp-formula></sec><sec id="s3"><title>3. Effective Field Equation and Mass</title><p>The general procedure of our treatment is as follows. We start from the (4 + d) dimensional Lorentz invariant Kinetic Lagrangian L(x, y) and the action for the field F(x, y) defined as</p><disp-formula id="scirp.45403-formula46386"><label>(9)</label><graphic position="anchor" xlink:href="htmlimages\18-7501780x\1c8afe7a-49df-4154-805c-af73abed3ef6.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="tmlimages\18-7501780x\951c8313-b26e-41c7-8ce7-93f940310b92.png" xlink:type="simple"/></inline-formula> and the integral is performed over the whole extra space time.</p><p>The principle of minimal action for S(y) then gives the Euler-Lagrange equation</p><disp-formula id="scirp.45403-formula46387"><label>(10)</label><graphic position="anchor" xlink:href="htmlimages\18-7501780x\653ea891-0bf6-4608-99a2-4b8cd7a9b165.png"  xlink:type="simple"/></disp-formula><p>which in turn leads to the equation of Klein-Gordon type:</p><p><img src="htmlimages\18-7501780x\8bb9d22f-a934-4a78-852f-b6157929c07d.png" /></p><p>For the effective field defined as</p><disp-formula id="scirp.45403-formula46388"><label>(11)</label><graphic position="anchor" xlink:href="htmlimages\18-7501780x\5a18691a-cf30-4a8d-aa2a-996c3dfa3969.png"  xlink:type="simple"/></disp-formula><p>For illustration let us consider in more details the cases of scalar, spinor and vector fields.</p><sec id="s3_1"><title>3.1. Scalar Field</title><p>The free neutral scalar field <inline-formula><inline-graphic xlink:href="tmlimages\18-7501780x\6ac3a008-00c4-4da3-8a20-4e3f602e8b2d.png" xlink:type="simple"/></inline-formula> is described by the Lagrangian</p><disp-formula id="scirp.45403-formula46389"><label>(12)</label><graphic position="anchor" xlink:href="htmlimages\18-7501780x\b9f38d49-c7f1-4366-ab8d-8ead00bca3f9.png"  xlink:type="simple"/></disp-formula><p>where<inline-formula><inline-graphic xlink:href="tmlimages\18-7501780x\e64cea72-38d9-4cb9-9f94-0e28456d7a9b.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="tmlimages\18-7501780x\a33b0b7e-d09b-41b9-b392-60a5c1b3e446.png" xlink:type="simple"/></inline-formula>is a Minkonski metric for extra dimensions:</p><p><img src="htmlimages\18-7501780x\8a6a88b7-d057-4458-ace7-381ae0c06e7f.png" /></p><p>By inverting (7) into (12), we obtain:</p><disp-formula id="scirp.45403-formula46390"><label>(13)</label><graphic position="anchor" xlink:href="htmlimages\18-7501780x\b166b657-4ce0-4a6f-bd19-24e69d155ad5.png"  xlink:type="simple"/></disp-formula><p>And from here the equation</p><disp-formula id="scirp.45403-formula46391"><label>(14)</label><graphic position="anchor" xlink:href="htmlimages\18-7501780x\24609930-b471-4608-b144-d90c78d0bc99.png"  xlink:type="simple"/></disp-formula><p>For the effective field</p><p><img src="htmlimages\18-7501780x\a41d2986-967c-4c13-8081-6a64ae6c1190.png" /></p><p>With</p><disp-formula id="scirp.45403-formula46392"><label>(15)</label><graphic position="anchor" xlink:href="htmlimages\18-7501780x\65e214e7-19af-4112-86e2-6b0a4d8dac29.png"  xlink:type="simple"/></disp-formula><p>It is worth nothing that the squared mass <inline-formula><inline-graphic xlink:href="tmlimages\18-7501780x\aa6f66de-8485-4069-abe4-aebb2544f2e6.png" xlink:type="simple"/></inline-formula> is positive if all the extra dimensions are space-live, and can be negative if there exist time-live extra dimensions.</p><p>For change scalar field instead of (12) we take</p><disp-formula id="scirp.45403-formula46393"><label>(16)</label><graphic position="anchor" xlink:href="htmlimages\18-7501780x\689d47c2-d678-4a76-8820-55515a18fb21.png"  xlink:type="simple"/></disp-formula><p>And instead of (13) we have:</p><disp-formula id="scirp.45403-formula46394"><label>(17)</label><graphic position="anchor" xlink:href="htmlimages\18-7501780x\251a1e08-e351-4140-b40b-2dd24389cdd6.png"  xlink:type="simple"/></disp-formula><p>And from here the equation the same Equation as (14) with:</p><disp-formula id="scirp.45403-formula46395"><label>(18)</label><graphic position="anchor" xlink:href="htmlimages\18-7501780x\3ab269f6-cb07-48b0-ad1c-7bff75ab9a83.png"  xlink:type="simple"/></disp-formula></sec><sec id="s3_2"><title>3.2. Spinor Field</title><p>In (4 + d) dimensional space-time, the spinor field is described by a <inline-formula><inline-graphic xlink:href="tmlimages\18-7501780x\f6b0a2a7-6d03-4c64-a68c-0ad8296e1f42.png" xlink:type="simple"/></inline-formula> component function <inline-formula><inline-graphic xlink:href="tmlimages\18-7501780x\996a2aaf-79c0-48bb-bfc6-9543d29e268c.png" xlink:type="simple"/></inline-formula> with the live Lagrangian</p><disp-formula id="scirp.45403-formula46396"><label>(19)</label><graphic position="anchor" xlink:href="htmlimages\18-7501780x\e51b5771-98ec-4d22-b64d-eb12d5204e55.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="tmlimages\18-7501780x\5d3eaec6-0263-4b09-a2c3-2b6de27ea0dc.png" xlink:type="simple"/></inline-formula> denote (4 + d) Dirac <inline-formula><inline-graphic xlink:href="tmlimages\18-7501780x\f05a2c73-a3bd-4d41-8f81-8b6f01075bab.png" xlink:type="simple"/></inline-formula> matrices obeying the ant commutation relations:</p><disp-formula id="scirp.45403-formula46397"><label>(20)</label><graphic position="anchor" xlink:href="htmlimages\18-7501780x\8842497b-f6c5-4ae1-9230-9ee1e841ea69.png"  xlink:type="simple"/></disp-formula><p>By inverting</p><disp-formula id="scirp.45403-formula46398"><label>(21)</label><graphic position="anchor" xlink:href="htmlimages\18-7501780x\9ee7fe67-ddc0-4194-b693-bc6c4f48f267.png"  xlink:type="simple"/></disp-formula><p>Into (19) we obtain:</p><disp-formula id="scirp.45403-formula46399"><label>(22)</label><graphic position="anchor" xlink:href="htmlimages\18-7501780x\acb4e0ec-6361-4a81-8f3c-2560eb2272f3.png"  xlink:type="simple"/></disp-formula><p>And from here the equation</p><disp-formula id="scirp.45403-formula46400"><label>(23)</label><graphic position="anchor" xlink:href="htmlimages\18-7501780x\791747c8-e211-44ae-8a70-7ebfdd58c5f3.png"  xlink:type="simple"/></disp-formula><p>By acting from the left both sides of this equation by</p><p><img src="htmlimages\18-7501780x\9271b9c6-1aca-4a57-bc0f-7ba9a88647ca.png" /></p><p>And taking into account the relations (20) we have:</p><disp-formula id="scirp.45403-formula46401"><label>(24)</label><graphic position="anchor" xlink:href="htmlimages\18-7501780x\da87d8f9-0cb3-419c-b8af-d7bed16be59f.png"  xlink:type="simple"/></disp-formula><p>And hence</p><disp-formula id="scirp.45403-formula46402"><label>(25)</label><graphic position="anchor" xlink:href="htmlimages\18-7501780x\ec175fb8-0462-4da1-9f38-76315efa4903.png"  xlink:type="simple"/></disp-formula><p>We note that <inline-formula><inline-graphic xlink:href="tmlimages\18-7501780x\743629f2-97e7-4198-a7d9-918250adf060.png" xlink:type="simple"/></inline-formula> if all the extra dimensions are space-like, <inline-formula><inline-graphic xlink:href="tmlimages\18-7501780x\43ef9f76-a3e2-4db0-a1ba-3ed758b09f9f.png" xlink:type="simple"/></inline-formula>if all <inline-formula><inline-graphic xlink:href="tmlimages\18-7501780x\ea0030ca-3451-4b61-a745-1d2babd559a2.png" xlink:type="simple"/></inline-formula> are real, and <inline-formula><inline-graphic xlink:href="tmlimages\18-7501780x\1f3e9562-edc6-4315-a989-5e0597886466.png" xlink:type="simple"/></inline-formula> can be negative if there exists time-like extra dimension</p></sec><sec id="s3_3"><title>3.3. Vector Field</title><p>We restrict ourselves to the case d = l and consider the neutral vector field <inline-formula><inline-graphic xlink:href="tmlimages\18-7501780x\2c29af76-7b07-4a50-8e58-1cf12ea868a4.png" xlink:type="simple"/></inline-formula> satisfying the periodicity condition</p><disp-formula id="scirp.45403-formula46403"><label>(26)</label><graphic position="anchor" xlink:href="htmlimages\18-7501780x\d52347b4-a5db-4d8e-88bf-9912f1a56fc9.png"  xlink:type="simple"/></disp-formula><p>And in correspondence</p><disp-formula id="scirp.45403-formula46404"><label>(27)</label><graphic position="anchor" xlink:href="htmlimages\18-7501780x\a7d4811b-68fc-4336-acf0-36092bec6f3b.png"  xlink:type="simple"/></disp-formula><p>The free vector field <inline-formula><inline-graphic xlink:href="tmlimages\18-7501780x\b350a416-083b-4be5-8648-b2ea4ab99d05.png" xlink:type="simple"/></inline-formula> is described by the Lagrangian</p><disp-formula id="scirp.45403-formula46405"><label>(28)</label><graphic position="anchor" xlink:href="htmlimages\18-7501780x\f8678c4d-2ac3-4b34-9982-297919a6c5fa.png"  xlink:type="simple"/></disp-formula><p>where</p><p><img src="htmlimages\18-7501780x\48514cec-a575-4ce9-b620-502d68a9ed08.png" /></p><p>By inverting (27) into (28) we have:</p><disp-formula id="scirp.45403-formula46406"><label>(29)</label><graphic position="anchor" xlink:href="htmlimages\18-7501780x\4999d4c6-6aa2-4c6b-b811-9e0373da7ca5.png"  xlink:type="simple"/></disp-formula><p>Now we define a new physical vector field <inline-formula><inline-graphic xlink:href="tmlimages\18-7501780x\81b646cf-fec6-4089-8631-6c713122f1ad.png" xlink:type="simple"/></inline-formula> by putting</p><disp-formula id="scirp.45403-formula46407"><label>(30)</label><graphic position="anchor" xlink:href="htmlimages\18-7501780x\8e76cb07-7c2f-419b-8829-243e5ae8be7c.png"  xlink:type="simple"/></disp-formula><p>Expressed in terms of<inline-formula><inline-graphic xlink:href="tmlimages\18-7501780x\3edf1a1d-20ad-4d36-80f4-8ce277051b88.png" xlink:type="simple"/></inline-formula>, the Lagrangian (29) has the form:</p><disp-formula id="scirp.45403-formula46408"><label>(31)</label><graphic position="anchor" xlink:href="htmlimages\18-7501780x\624b239f-3691-4ab5-b89c-3ccd82d235c8.png"  xlink:type="simple"/></disp-formula><p>The Lagrangian (31) leads to the equation:</p><disp-formula id="scirp.45403-formula46409"><label>(32)</label><graphic position="anchor" xlink:href="htmlimages\18-7501780x\20f3126c-d08d-419e-815c-e546b28d557b.png"  xlink:type="simple"/></disp-formula><p>which means that the effective vector field</p><p><img src="htmlimages\18-7501780x\f8ee3609-625c-4591-80e0-b3a7daf615fd.png" /></p><p>Has squared mass</p><disp-formula id="scirp.45403-formula46410"><label>(33)</label><graphic position="anchor" xlink:href="htmlimages\18-7501780x\2932657a-7308-422a-8a25-d3a368515d42.png"  xlink:type="simple"/></disp-formula><p>It’s positive or negative depending upon whether the extra dimension is space-like or time-like.</p></sec></sec><sec id="s4"><title>4. Conclusion and Discussion</title><p>In this work we have proposed a mechanism for the creation of particle mass. The key idea is that the mass is originated from the compactification of extra dimensions followed by the periodicity condition for the particle fields.</p><p>It is worth noting that according to the mechanism the existence of tachyon having negative squared mass is closely related to the existence of time-like extra dimensions.</p><p>In this work we have considered originality for mass creation, which is originated from the compactification of extradimensions. It is shown that the mass spectrum is completely determined by some functions of compactification length and closely related to the metric of extradimensions.</p><p>The key idea is that the existence and the compactification of extradimensions are the origin for creating particle mass in ordinary 4-dimensional space-time. In this connection one might think that the mass of Higgs particles themselves would be also originated from the geometric topology of extradimensions. The problem of whether there exists some mechanism allowing the extradimensions to create Higgs particles would be a problem of significant meaning. It might be also that the particles could acquire mass through different mechanisms, including those related to extradimensions. This could lead to thinking that the probability for experimentally finding Higgs particles is much smaller than the value theoretically obtained when Higgs mechanism is considered as the only one for mass creation.</p></sec></body><back><ref-list><title>References</title><ref id="scirp.45403-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Cs’aki, C. 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