<?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">IJAA</journal-id><journal-title-group><journal-title>International Journal of Astronomy and Astrophysics</journal-title></journal-title-group><issn pub-type="epub">2161-4717</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/ijaa.2012.24024</article-id><article-id pub-id-type="publisher-id">IJAA-26041</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>
 
 
  Two-Component Substance Basing the Direction Dependence of the Cosmological Deceleration Parameter
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>eonid</surname><given-names>M. Chechin</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>V. G. Fessenkov Astrophysical Institute, Almaty, Kazakhstan</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>chechin-lm@mail.ru</email></corresp></author-notes><pub-date pub-type="epub"><day>31</day><month>12</month><year>2012</year></pub-date><volume>02</volume><issue>04</issue><fpage>195</fpage><lpage>198</lpage><history><date date-type="received"><day>June</day>	<month>29,</month>	<year>2012</year></date><date date-type="rev-recd"><day>August</day>	<month>4,</month>	<year>2012</year>	</date><date date-type="accepted"><day>August</day>	<month>15,</month>	<year>2012</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>
 
  Purpose.Thetheoretical description of Hubble’s diagrams asymmetry of and calculating the anisotropy of the deceleration parameter phenomenon, that was recently found by R.-G.Cai and Z.-L.Tuo.Method. For doing this the concepts of Universe rotation and its two-component model were attracted.Result.Our result 
  <img style="width:41px;height:35px;" alt="" src="Edit_b9f884dc-2060-4487-ae74-6051c0e15b4e.bmp" width="58" height="35" />
  <img style="width:34px;height:16px;" alt="" src="Edit_19447c0a-92d7-48ca-9367-65737c2ee518.bmp" width="48" height="17" /> is in good correlation (case of the upper magnitude index) with the value 
  <img style="width:40px;height:35px;" alt="" src="Edit_2bc2b78d-d23f-4718-b1a6-81d8e9a33488.bmp" width="57" height="53" />
  <img style="width:47px;height:17px;" alt="" src="Edit_2bf54b17-f9af-48a4-ab88-c999c5f95095.bmp" width="50" height="21" /> that was got in [1].Significance. The result of article gives new basing of the Universe rotation axis existence.
 
</html></p></abstract><kwd-group><kwd>Anisotropy of the Deceleration Parameter; Universe Principal Axis</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>The discovering of the accelerating expansion of Universe though observations of distant supernovae [2,3] were stimulated large numbers of articles in which this effect was interprets not only in the framework of general relativity but from other theoretical viewpoints, also. In fact, in [<xref ref-type="bibr" rid="scirp.26041-ref4">4</xref>] it was considered the anisotropic case of the dark energy equation of state; in [<xref ref-type="bibr" rid="scirp.26041-ref5">5</xref>] the anisotropy of cosmic acceleration was searched in the framework of generalized teleparallel gravity; in [<xref ref-type="bibr" rid="scirp.26041-ref6">6</xref>] for the one variant of 5-dimensional inhomogeneous space-time it was found the anisotropic acceleration; in [<xref ref-type="bibr" rid="scirp.26041-ref7">7</xref>] the deceleration anisotropy was considered by usage of baryonic matter Born-Infeld type electrodynamics, and some others attempts [8-11].</p><p>Separately to previous variants it’s necessary to mention the fundamental article [<xref ref-type="bibr" rid="scirp.26041-ref12">12</xref>] especially where the asymmetry of Hubble’s diagrams for the North and the South sky hemispheres was searched. (Remind that the Hubble diagram describes in first approximation the linear proportionality between a galaxy’s distance and its redshift. Later on it was found that the velocity at which a distant galaxy is moving from us should be permanently increasing over time, i.e. the cosmic scale factor has a positive second derivative, while deceleration parameter is negative<img src="1-4500083\7a7c0683-6bba-47e5-8c00-8e51e9e469d9.jpg" />.) This asymmetry, according to authors, cannot be explains by peculiar motion of the observer, but most apparently due to the any bulk flow along the direction ((l, b) = (<img src="1-4500083\93c98458-6dc6-4bb2-9510-9f627842bce3.jpg" />,<img src="1-4500083\541bfdca-eae7-447d-b25e-a359d148b10f.jpg" />)) in the Universe existence that earlier was argued in article [13,14]. Recently R.-G. Cai and Z.-L. Tuo [<xref ref-type="bibr" rid="scirp.26041-ref1">1</xref>] determined more precisely this direction ((l, b) =<img src="1-4500083\2584eb82-8a8f-4186-a7e9-88b74c234107.jpg" />,<img src="1-4500083\c2fde1b2-0dac-4453-a32e-89b300ebee22.jpg" />)</p><p>and found the maximum anisotropy of the deceleration parameter<img src="1-4500083\ff15b940-99e9-4dc0-b701-489ddb94741a.jpg" />.</p><p>Evidently, these results are possible to summaries as follows—our Universe is anisotropic in realty and possesses by any principal space axis. That is why the cosmological deceleration parameter will be anisotropic, also and must be depend on the principal space direction in definite way. These statements require theoretical basing the direction dependence of the cosmological deceleration parameter phenomenon.</p></sec><sec id="s2"><title>2. Basic Cosmological Equations</title><p>Our searching we start from the well-known results. The uniform isotropic metric of the space-flat Universe (<img src="1-4500083\e5fa090c-926a-4831-8baa-8c977c399a73.jpg" />) have the standard form</p><disp-formula id="scirp.26041-formula6522"><label>(1)</label><graphic position="anchor" xlink:href="1-4500083\b57f97b2-b913-4e23-983e-5c2362a0642a.jpg"  xlink:type="simple"/></disp-formula><p>Einstein’s equations for the scale factor <img src="1-4500083\7a831331-741b-45ff-9f22-7056357ef0b6.jpg" /> are</p><disp-formula id="scirp.26041-formula6523"><label>(2)</label><graphic position="anchor" xlink:href="1-4500083\ce5816e3-a4ab-447b-809a-98c1e34f40aa.jpg"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.26041-formula6524"><label>(3)</label><graphic position="anchor" xlink:href="1-4500083\a50c0026-e035-4deb-adf1-74744d8ca50f.jpg"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.26041-formula6525"><label>(4)</label><graphic position="anchor" xlink:href="1-4500083\4572c505-51b5-4ada-bb4e-5bb95e7494b1.jpg"  xlink:type="simple"/></disp-formula><p>These equations is possible to deduce and from the Newtonian mechanics in the following way. Let’s consider the spherical volume of radius <img src="1-4500083\050faf3d-05e9-4289-a3fb-de0a19736cd7.jpg" /> where concentrates any substance with the density <img src="1-4500083\5a5ceb8d-531f-41a4-8798-7d029ca020b6.jpg" /> and with the Hubble velocity distribution</p><disp-formula id="scirp.26041-formula6526"><label>(5)</label><graphic position="anchor" xlink:href="1-4500083\6b6b30ea-ccc4-4fd0-99d9-08d972ebcdf7.jpg"  xlink:type="simple"/></disp-formula><p>In the motionless frame of reference the equation of motion of a probe particle that locates on the surface of this sphere, have the usual form</p><disp-formula id="scirp.26041-formula6527"><label>(6)</label><graphic position="anchor" xlink:href="1-4500083\783c2f24-64ab-41fc-9d9a-7f6fd0233937.jpg"  xlink:type="simple"/></disp-formula><p>Making the well-known Tolman transformation<img src="1-4500083\7ba1c04c-2872-451b-9b89-a8835c34e08b.jpg" />, that allows taking into account the pressure influence on equation of motion, and putting it into (6) we get Equation (2). Next, multiplying left and right sides of (6) by <img src="1-4500083\9a4b9b8f-6aa7-4380-a65f-4c87d91c2f4e.jpg" /> we get Equation (3), that is connected with (6) by the law of energy conservation (4) [<xref ref-type="bibr" rid="scirp.26041-ref15">15</xref>].</p></sec><sec id="s3"><title>3. Universe Rotation Axis</title><p>In article [<xref ref-type="bibr" rid="scirp.26041-ref16">16</xref>] it was shown that cosmic vacuum produces not only the Universe expansion but its rotation, also. Here the main results of this article are reproducing briefly.</p><p>Let’s start from searching the rotational movement of galaxies caused by the antigravitational vacuum force, only. As the model of examining type of galaxy the elliptical galaxy was chosen. For this shape of galaxy its equations of rotational motion are</p><disp-formula id="scirp.26041-formula6528"><label>(7)</label><graphic position="anchor" xlink:href="1-4500083\569b9eb5-11e5-4f13-927f-aca92e1aba2a.jpg"  xlink:type="simple"/></disp-formula><p>In (7) <img src="1-4500083\afba878d-6ef5-49ee-b40f-c4236b6c5fef.jpg" />is the first integral of the rotational motion, i.e.<img src="1-4500083\8cf06799-7871-43f5-a488-ae1598b2861a.jpg" />. It describes the component of angular velocity with respect to the specific momentum—C. Next, at deducing (7) it was put forward condition that galaxy angular velocity is very small. This allowed neglect the squared angular velocity components and the corresponding angular accelerations. And at last, it was assumed that arbitrary potential in (7) equals to the vacuum potential<img src="1-4500083\4907ca06-2c26-4db4-a101-ee3d03902106.jpg" />, where</p><disp-formula id="scirp.26041-formula6529"><label>(8)</label><graphic position="anchor" xlink:href="1-4500083\978dd6b4-ee83-48ba-b6c8-5beef14960f4.jpg"  xlink:type="simple"/></disp-formula><p>Analysis of Equation (7) shown that solution for the precession angle evolving is<img src="1-4500083\9c05ae59-fee5-4cd9-a1ff-376465e8b1ec.jpg" />. Basing on this result it is easy to calculate the angular velocity of the elliptical galaxy around <img src="1-4500083\08c57bb5-ca0e-4e7f-b5be-b92452b4c0c5.jpg" /> axis. As for this case the following condition <img src="1-4500083\2ecd1120-744a-48d1-992e-394c5c48be78.jpg" /> takes place, than its module equals</p><disp-formula id="scirp.26041-formula6530"><label>(9)</label><graphic position="anchor" xlink:href="1-4500083\95f17a74-5728-4bcb-a532-af027b877e88.jpg"  xlink:type="simple"/></disp-formula><p>This expression describes the angular velocity that galaxy acquires due to the vacuum antigravitational force.</p><p>Admitting <img src="1-4500083\21c6a9d9-f444-41dc-b58e-24ef372287ea.jpg" /> and putting that<img src="1-4500083\084f0550-f8c1-47b2-9fd3-62c10810159c.jpg" />we find<img src="1-4500083\7fe479f4-a82b-4c27-9492-0f7e7277fa93.jpg" />. So, its maximal magnitude will be under the condition<img src="1-4500083\a26a78a5-e329-4b4e-8c01-1f95e61ff8f7.jpg" />. Then expression for the vacuum angular velocity simplifies and takes on the form</p><disp-formula id="scirp.26041-formula6531"><label>(10)</label><graphic position="anchor" xlink:href="1-4500083\8afc59e2-c568-4c04-adf0-9dcdc6c3a14f.jpg"  xlink:type="simple"/></disp-formula><p>This expression interprets as the minimal angular velocity in the Universe that possesses an arbitrary object due to the vacuum presence. Its present numerical value is<img src="1-4500083\a5abb9da-2240-4871-94ce-b9286147f66f.jpg" />. Hence, the vacuum creates the identical initial angular velocity for all of cosmic objects, includeing the Universe itself.</p><p>At the earliest stages of the Universe evolution, for instance at the baryonic asymmetry epoch when vacuum density was <img src="1-4500083\aa10485b-1c50-42aa-aa59-fef4c981c35b.jpg" /> of order, the angular velocity occurs equal<img src="1-4500083\fd0127a0-a5d0-4acd-97e2-96e7e4dd925a.jpg" />. For the very early Universe when vacuum density was—<img src="1-4500083\5c0ac7f9-f0ea-4bf4-bd89-c670aac9b351.jpg" />, the Universe angular velocity is<img src="1-4500083\b6bc431b-d78f-4c53-9170-555bc11f5418.jpg" />. This magnitude practically equals to the result of article [<xref ref-type="bibr" rid="scirp.26041-ref17">17</xref>], which was done in the framework of general relativity theory (<img src="1-4500083\85d46aa1-2644-424d-bc12-22d4af3f4f32.jpg" />).</p><p>Henceforth, from these investigations we get the following conclusion—the Universe rotation leads to picking out the principal direction in the space, it may be named as the Universe rotation axis. (Mark, that measurement along this axis only gives the Hubble parameter for the uniform Universe, because in the perpendicular directions the Carioles and centrifugal forces act, also).</p></sec><sec id="s4"><title>4. Basing the Direction Dependence of the Cosmological Deceleration Parameter</title><p>For enriching our target, which was formulated in Section 1, put that distance</p><disp-formula id="scirp.26041-formula6532"><label>(11)</label><graphic position="anchor" xlink:href="1-4500083\f45d872b-ef69-493b-882a-c8564dcd7fea.jpg"  xlink:type="simple"/></disp-formula><p>where <img src="1-4500083\a84ffcdd-11d5-4a1a-b9e2-09b381cafba7.jpg" /> is the distance in uniform space, while<img src="1-4500083\a7446450-169f-4aae-af4b-c106bfd47761.jpg" />— small addition (perturb term) for describing the possible space anisotropy. Putting (11) into the Newtonian Equation (6) we get the equation</p><disp-formula id="scirp.26041-formula6533"><label>(12)</label><graphic position="anchor" xlink:href="1-4500083\f7fac661-b63e-4d5b-90fe-7df3e8b39d93.jpg"  xlink:type="simple"/></disp-formula><p>that may be decomposed on two parts, easily: main part</p><disp-formula id="scirp.26041-formula6534"><label>(13)</label><graphic position="anchor" xlink:href="1-4500083\f80aeeae-6693-4670-9649-f454c99292da.jpg"  xlink:type="simple"/></disp-formula><p>and perturb one</p><disp-formula id="scirp.26041-formula6535"><label>(14)</label><graphic position="anchor" xlink:href="1-4500083\42307cf1-1b2a-4714-96e6-a079a1a8baa0.jpg"  xlink:type="simple"/></disp-formula><p>Later on these equations will be considered as are independent each other.</p><p>Performing the above mentioned Tolman transformation <img src="1-4500083\7583ca99-eff6-4e2c-9e29-eb7c8bb9658a.jpg" /> and substituting it into (13) we find equation</p><disp-formula id="scirp.26041-formula6536"><label>(15)</label><graphic position="anchor" xlink:href="1-4500083\f9e3bd97-6434-4adf-9a87-a3691c7054c9.jpg"  xlink:type="simple"/></disp-formula><p>For the case of vacuum (<img src="1-4500083\c624d559-d336-4941-8fea-d8601cb6cd19.jpg" />,<img src="1-4500083\7eac1de7-7d4b-4f33-bd88-417bd348f895.jpg" />) the inflationary regime of the Universe expanding follows from (15) immediately—</p><disp-formula id="scirp.26041-formula6537"><label>(16)</label><graphic position="anchor" xlink:href="1-4500083\831ae0cf-5d92-4006-9edf-5ad4b19b73ec.jpg"  xlink:type="simple"/></disp-formula><p>It leads to the Hubble expansion law</p><disp-formula id="scirp.26041-formula6538"><label>(17)</label><graphic position="anchor" xlink:href="1-4500083\bd19ebdd-fa7d-4932-b3db-edc015ee9299.jpg"  xlink:type="simple"/></disp-formula><p>and to the corresponding acceleration</p><disp-formula id="scirp.26041-formula6539"><label>(18)</label><graphic position="anchor" xlink:href="1-4500083\38ccda81-f628-44ba-b462-43a1bee7cc4d.jpg"  xlink:type="simple"/></disp-formula><p>Now consider the Equation (14). Suppose that in this equation<img src="1-4500083\a5e7fc6a-dea0-4422-89f3-98cb80ea26fa.jpg" />, where <img src="1-4500083\082c1360-98b8-42c3-885f-184291863e05.jpg" /> is the baryonic substance density. The baryonic substance pressure <img src="1-4500083\5d8a699c-a497-4931-8440-a098e1f8dc45.jpg" /> let equals zero, for simplicity. Last requirement means considering the presence of two-component substance—cosmic vacuum and baryonic dust—in the Universe, that are not interact each other in the main approximation.</p><p>By introducing the designation<img src="1-4500083\2b25c9e7-4c99-4d91-b3d0-6a0e8429d2a4.jpg" />, from (14) it follows</p><disp-formula id="scirp.26041-formula6540"><label>(19)</label><graphic position="anchor" xlink:href="1-4500083\767534cd-1fe3-46b6-8937-46a3139356a7.jpg"  xlink:type="simple"/></disp-formula><p>This oscillatory-type equation possesses by two roots</p><disp-formula id="scirp.26041-formula6541"><label>(20)</label><graphic position="anchor" xlink:href="1-4500083\fdd2a169-486a-47c1-9e39-a7e4769ef45e.jpg"  xlink:type="simple"/></disp-formula><p>They lead to the presence of two perturb (with respect to (17)) velocities</p><disp-formula id="scirp.26041-formula6542"><label>(21)</label><graphic position="anchor" xlink:href="1-4500083\14ef41bf-6c45-4e6e-910e-9edabc0bfa1a.jpg"  xlink:type="simple"/></disp-formula><p>and two corresponding accelerations</p><disp-formula id="scirp.26041-formula6543"><label>(22)</label><graphic position="anchor" xlink:href="1-4500083\f57076dd-0aeb-42f8-a844-2313dcfb07ce.jpg"  xlink:type="simple"/></disp-formula><p>From physical viewpoint expressions (20)-(22) mean that presence of baryonic dust matter creates two spaceopposite fluxes that are propagate on the background of expanding and accelerating “Hubble vacuum flux” along the Universe rotation axis (see division 3). That is why it possible writes down the expressions for total distance, velocity and acceleration of any probe particle (galaxy)</p><disp-formula id="scirp.26041-formula6544"><label>(23)</label><graphic position="anchor" xlink:href="1-4500083\b0cd6efc-1d4a-4741-ab77-82522c1a5277.jpg"  xlink:type="simple"/></disp-formula><p>Thus the cosmological deceleration parameter q with the accuracy no higher than <img src="1-4500083\ff91ab14-9cff-4488-bf33-71840274b9a8.jpg" /> is</p><disp-formula id="scirp.26041-formula6545"><label>(24)</label><graphic position="anchor" xlink:href="1-4500083\140c654a-f164-4e5d-9796-00a96327cafc.jpg"  xlink:type="simple"/></disp-formula><p>Basing on the definitions of <img src="1-4500083\7308f81e-8a29-406f-8a37-730671e59adc.jpg" /> and <img src="1-4500083\af4ab5df-3186-4736-83b4-bcaabb16055a.jpg" /> we introduce the new coefficient<img src="1-4500083\8e30b25c-28ac-4bc8-9f38-44a754dc00b6.jpg" />. As in unit of the critical density <img src="1-4500083\03560eb0-0df5-4fa8-827d-8e795f150927.jpg" /> and vacuum density<img src="1-4500083\11d0e2f8-2a05-4745-9893-b753c77e5621.jpg" />, coefficient<img src="1-4500083\9e0fd395-f698-4e91-88d6-1f61a5458af9.jpg" />, henceforth.</p><p>From (24) it is possible find the relative acceleration difference between two baryonic fluxes with respect to the “Hubble vacuum flux”—</p><disp-formula id="scirp.26041-formula6546"><label>(25)</label><graphic position="anchor" xlink:href="1-4500083\131a86a6-3af8-43ff-a908-abd5736330b5.jpg"  xlink:type="simple"/></disp-formula><p>Assuming that for modern epoch <img src="1-4500083\0c46b93e-f972-4a57-8479-4ceb43bdbf07.jpg" /> we approximately get<img src="1-4500083\e5b753e5-cd30-4385-9b40-7fc60f708d01.jpg" />. Hence, the first term in right side of (25) tends to 1.2, while the second term tends to zero. So,</p><disp-formula id="scirp.26041-formula6547"><label>(26)</label><graphic position="anchor" xlink:href="1-4500083\8556ff65-c937-4278-8333-1566bfbaaa14.jpg"  xlink:type="simple"/></disp-formula><p>Basing on our assumption<img src="1-4500083\b5670bba-601f-41b4-834e-1db0e7ff2d2d.jpg" />, that was argued earlier, we may put that it will satisfy if the ratio <img src="1-4500083\d68a699b-2304-4b1f-af3b-ce4ec8d5e779.jpg" />. This leads to the estimation <img src="1-4500083\5196d74c-0de3-4486-9227-2d7b0658fac1.jpg" /> that is in good correlation (case of the upper magnitude index) with the value <img src="1-4500083\8dcb9cb9-8bbb-4e29-bf52-20b444f6c7c5.jpg" /> in [<xref ref-type="bibr" rid="scirp.26041-ref1">1</xref>].</p></sec><sec id="s5"><title>5. Conclusion</title><p>From observational data it was established the asymmetry of Hubble’s diagrams for the North and the South sky hemispheres [13,14]. Moreover it was estimated the space anisotropy of the deceleration parameter phenomenon, that was done by R.-G. Cai and Z.-L. Tuo. These facts require the adequate theoretical basing, hence.</p><p>For doing this the concepts of Universe vacuum rotation and its two independent component model (cosmic vacuum and baryonic dust) were attracted. Our result on the phenomenon of anisotropy the deceleration parameter calculation—<img src="1-4500083\f56fb883-7d52-4bd5-9842-7f60d697951b.jpg" />—is in good correlation</p><p>(case of the upper magnitude index) with the value</p><p><img src="1-4500083\b69a9d32-6cac-472b-a3c4-e2467c7015d1.jpg" />, which was evaluated in [<xref ref-type="bibr" rid="scirp.26041-ref1">1</xref>].</p></sec><sec id="s6"><title>6. Acknowledgements</title><p>I would like to express the gratitude to Ministry of Education and Sciences, Republic of Kazakhstan for supports this searching in the framework of budget program 055, subprogram 101 “Grant financing of the scientific researchers”.</p><p>Also I thank a reviewer for his thought-out suggestions on the article’s content clarifying.</p></sec><sec id="s7"><title>REFERENCES</title></sec></body><back><ref-list><title>References</title><ref id="scirp.26041-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">R.-G. Cai and Z.-L. Tuo, “Direction Dependence of the Deceleration Parameter,” Vol. 1, 2011.</mixed-citation></ref><ref id="scirp.26041-ref2"><label>2</label><mixed-citation publication-type="other" xlink:type="simple">A. G. 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