Dark companion of Baryonic matter, III

Wherever one talks of dark matter, one does so where there is an observable matter and an associated unsolved dynamical issue to be settled. We promote this observation to the status of an axiom and conjecture that there is a dark companion to every baryonic matter, subject to certain rules as regar...

Ausführliche Beschreibung

Gespeichert in:
Bibliographische Detailangaben
1. Verfasser: Sobouti, Yousef
Format: Artikel
Sprache:eng
Schlagworte:
Online-Zugang:Volltext bestellen
Tags: Tag hinzufügen
Keine Tags, Fügen Sie den ersten Tag hinzu!
container_end_page
container_issue
container_start_page
container_title
container_volume
creator Sobouti, Yousef
description Wherever one talks of dark matter, one does so where there is an observable matter and an associated unsolved dynamical issue to be settled. We promote this observation to the status of an axiom and conjecture that there is a dark companion to every baryonic matter, subject to certain rules as regards its size, distribution. To pursue the proposition in a systematic way we resort to the rotation curves of spiral galaxies. They have non classical features. First, we design a spacetime metric around the galaxy to accommodate these features. Next we calculate the density and pressure of a hypothetical dark matter that could generate such a spacetime. In the weak field regime and for a spherical distribution of mass $M$, we are able to assign a dark perfect gas companion, whose density is almost proportional to $M^{1/2}$ and fades away almost as $r^{-2}$. However, in view of this orderly relation between the observable mass and its dark companion, one may choose to interpret the whole scenario as an alternative theory of gravitation.
doi_str_mv 10.48550/arxiv.0903.5007
format Article
fullrecord <record><control><sourceid>arxiv_GOX</sourceid><recordid>TN_cdi_arxiv_primary_0903_5007</recordid><sourceformat>XML</sourceformat><sourcesystem>PC</sourcesystem><sourcerecordid>0903_5007</sourcerecordid><originalsourceid>FETCH-LOGICAL-a657-d67dd2099384d78c28c16321988c82404cd26b0bab62d867a70c04ff61f44b483</originalsourceid><addsrcrecordid>eNotzjsLwjAUQOEsDqLuTpLJydbbJE1uR98WBBf3cpsYKNpWooj-e5_T2Q4fY8MEYoVpClMKj-oeQwYyTgFMl42XFE7ctvWFmqpteOv5nMKzbSrLa7rdjmHC8zzvs46n8_U4-LfHDuvVYbGNdvtNvpjtItKpiZw2zgnIMonKGbQCbaKlSDJEi0KBsk7oEkoqtXCoDRmwoLzXiVeqVCh7bPTbfp3FJVT1G1N8vMXHK18s-jgP</addsrcrecordid><sourcetype>Open Access Repository</sourcetype><iscdi>true</iscdi><recordtype>article</recordtype></control><display><type>article</type><title>Dark companion of Baryonic matter, III</title><source>arXiv.org</source><creator>Sobouti, Yousef</creator><creatorcontrib>Sobouti, Yousef</creatorcontrib><description>Wherever one talks of dark matter, one does so where there is an observable matter and an associated unsolved dynamical issue to be settled. We promote this observation to the status of an axiom and conjecture that there is a dark companion to every baryonic matter, subject to certain rules as regards its size, distribution. To pursue the proposition in a systematic way we resort to the rotation curves of spiral galaxies. They have non classical features. First, we design a spacetime metric around the galaxy to accommodate these features. Next we calculate the density and pressure of a hypothetical dark matter that could generate such a spacetime. In the weak field regime and for a spherical distribution of mass $M$, we are able to assign a dark perfect gas companion, whose density is almost proportional to $M^{1/2}$ and fades away almost as $r^{-2}$. However, in view of this orderly relation between the observable mass and its dark companion, one may choose to interpret the whole scenario as an alternative theory of gravitation.</description><identifier>DOI: 10.48550/arxiv.0903.5007</identifier><language>eng</language><subject>Physics - General Relativity and Quantum Cosmology</subject><creationdate>2009-03</creationdate><rights>http://arxiv.org/licenses/nonexclusive-distrib/1.0</rights><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>228,230,781,886</link.rule.ids><linktorsrc>$$Uhttps://arxiv.org/abs/0903.5007$$EView_record_in_Cornell_University$$FView_record_in_$$GCornell_University$$Hfree_for_read</linktorsrc><backlink>$$Uhttps://doi.org/10.48550/arXiv.0903.5007$$DView paper in arXiv$$Hfree_for_read</backlink></links><search><creatorcontrib>Sobouti, Yousef</creatorcontrib><title>Dark companion of Baryonic matter, III</title><description>Wherever one talks of dark matter, one does so where there is an observable matter and an associated unsolved dynamical issue to be settled. We promote this observation to the status of an axiom and conjecture that there is a dark companion to every baryonic matter, subject to certain rules as regards its size, distribution. To pursue the proposition in a systematic way we resort to the rotation curves of spiral galaxies. They have non classical features. First, we design a spacetime metric around the galaxy to accommodate these features. Next we calculate the density and pressure of a hypothetical dark matter that could generate such a spacetime. In the weak field regime and for a spherical distribution of mass $M$, we are able to assign a dark perfect gas companion, whose density is almost proportional to $M^{1/2}$ and fades away almost as $r^{-2}$. However, in view of this orderly relation between the observable mass and its dark companion, one may choose to interpret the whole scenario as an alternative theory of gravitation.</description><subject>Physics - General Relativity and Quantum Cosmology</subject><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2009</creationdate><recordtype>article</recordtype><sourceid>GOX</sourceid><recordid>eNotzjsLwjAUQOEsDqLuTpLJydbbJE1uR98WBBf3cpsYKNpWooj-e5_T2Q4fY8MEYoVpClMKj-oeQwYyTgFMl42XFE7ctvWFmqpteOv5nMKzbSrLa7rdjmHC8zzvs46n8_U4-LfHDuvVYbGNdvtNvpjtItKpiZw2zgnIMonKGbQCbaKlSDJEi0KBsk7oEkoqtXCoDRmwoLzXiVeqVCh7bPTbfp3FJVT1G1N8vMXHK18s-jgP</recordid><startdate>20090328</startdate><enddate>20090328</enddate><creator>Sobouti, Yousef</creator><scope>GOX</scope></search><sort><creationdate>20090328</creationdate><title>Dark companion of Baryonic matter, III</title><author>Sobouti, Yousef</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-a657-d67dd2099384d78c28c16321988c82404cd26b0bab62d867a70c04ff61f44b483</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2009</creationdate><topic>Physics - General Relativity and Quantum Cosmology</topic><toplevel>online_resources</toplevel><creatorcontrib>Sobouti, Yousef</creatorcontrib><collection>arXiv.org</collection></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext_linktorsrc</fulltext></delivery><addata><au>Sobouti, Yousef</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Dark companion of Baryonic matter, III</atitle><date>2009-03-28</date><risdate>2009</risdate><abstract>Wherever one talks of dark matter, one does so where there is an observable matter and an associated unsolved dynamical issue to be settled. We promote this observation to the status of an axiom and conjecture that there is a dark companion to every baryonic matter, subject to certain rules as regards its size, distribution. To pursue the proposition in a systematic way we resort to the rotation curves of spiral galaxies. They have non classical features. First, we design a spacetime metric around the galaxy to accommodate these features. Next we calculate the density and pressure of a hypothetical dark matter that could generate such a spacetime. In the weak field regime and for a spherical distribution of mass $M$, we are able to assign a dark perfect gas companion, whose density is almost proportional to $M^{1/2}$ and fades away almost as $r^{-2}$. However, in view of this orderly relation between the observable mass and its dark companion, one may choose to interpret the whole scenario as an alternative theory of gravitation.</abstract><doi>10.48550/arxiv.0903.5007</doi><oa>free_for_read</oa></addata></record>
fulltext fulltext_linktorsrc
identifier DOI: 10.48550/arxiv.0903.5007
ispartof
issn
language eng
recordid cdi_arxiv_primary_0903_5007
source arXiv.org
subjects Physics - General Relativity and Quantum Cosmology
title Dark companion of Baryonic matter, III
url https://sfx.bib-bvb.de/sfx_tum?ctx_ver=Z39.88-2004&ctx_enc=info:ofi/enc:UTF-8&ctx_tim=2024-12-16T19%3A16%3A12IST&url_ver=Z39.88-2004&url_ctx_fmt=infofi/fmt:kev:mtx:ctx&rfr_id=info:sid/primo.exlibrisgroup.com:primo3-Article-arxiv_GOX&rft_val_fmt=info:ofi/fmt:kev:mtx:journal&rft.genre=article&rft.atitle=Dark%20companion%20of%20Baryonic%20matter,%20III&rft.au=Sobouti,%20Yousef&rft.date=2009-03-28&rft_id=info:doi/10.48550/arxiv.0903.5007&rft_dat=%3Carxiv_GOX%3E0903_5007%3C/arxiv_GOX%3E%3Curl%3E%3C/url%3E&disable_directlink=true&sfx.directlink=off&sfx.report_link=0&rft_id=info:oai/&rft_id=info:pmid/&rfr_iscdi=true