Composite vacuum Brans-Dicke wormholes
We construct a new static spherically symmetric configuration composed of interior and exterior Brans-Dicke vacua matched at a thin matter shell. Both vacua correspond to the same Brans-Dicke coupling parameter \(\omega\), however they are described by the Brans class I solution with different sets...
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description | We construct a new static spherically symmetric configuration composed of interior and exterior Brans-Dicke vacua matched at a thin matter shell. Both vacua correspond to the same Brans-Dicke coupling parameter \(\omega\), however they are described by the Brans class I solution with different sets of parameters of integration. In particular, the exterior vacuum solution has \(C_{ext}(\omega)\equiv 0\). In this case the Brans class I solution for any \(\omega\) reduces to the Schwarzschild one being consistent with restrictions on the post-Newtonian parameters following from recent Cassini data. The interior region possesses a strong gravitational field, and so the interior vacuum solution has \(C_{int}(\omega)=-1/(\omega+2)\). In this case the Brans class I solution describes a wormhole spacetime provided \(\omega\) lies in the narrow interval \(-2-\frac{\sqrt{3}}{3} |
doi_str_mv | 10.48550/arxiv.1109.2273 |
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Both vacua correspond to the same Brans-Dicke coupling parameter \(\omega\), however they are described by the Brans class I solution with different sets of parameters of integration. In particular, the exterior vacuum solution has \(C_{ext}(\omega)\equiv 0\). In this case the Brans class I solution for any \(\omega\) reduces to the Schwarzschild one being consistent with restrictions on the post-Newtonian parameters following from recent Cassini data. The interior region possesses a strong gravitational field, and so the interior vacuum solution has \(C_{int}(\omega)=-1/(\omega+2)\). In this case the Brans class I solution describes a wormhole spacetime provided \(\omega\) lies in the narrow interval \(-2-\frac{\sqrt{3}}{3}<\omega<-2\). The interior and exterior regions are matched at a thin shell made from an ordinary perfect fluid with positive energy density and pressure obeying the barotropic equation of state \(p=k\sigma\) with \(0\le k\le1\). The resulting configuration represents a composite wormhole, i.e. the thin matter shell with the Schwarzschild-like exterior region and the interior region containing the wormhole throat.</description><identifier>EISSN: 2331-8422</identifier><identifier>DOI: 10.48550/arxiv.1109.2273</identifier><language>eng</language><publisher>Ithaca: Cornell University Library, arXiv.org</publisher><subject>Configurations ; Equations of state ; Flux density ; Gravitational fields ; Parameters ; Physics - General Relativity and Quantum Cosmology ; Thin walled shells ; Wormholes</subject><ispartof>arXiv.org, 2011-09</ispartof><rights>2011. This work is published under http://arxiv.org/licenses/nonexclusive-distrib/1.0/ (the “License”). 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Both vacua correspond to the same Brans-Dicke coupling parameter \(\omega\), however they are described by the Brans class I solution with different sets of parameters of integration. In particular, the exterior vacuum solution has \(C_{ext}(\omega)\equiv 0\). In this case the Brans class I solution for any \(\omega\) reduces to the Schwarzschild one being consistent with restrictions on the post-Newtonian parameters following from recent Cassini data. The interior region possesses a strong gravitational field, and so the interior vacuum solution has \(C_{int}(\omega)=-1/(\omega+2)\). In this case the Brans class I solution describes a wormhole spacetime provided \(\omega\) lies in the narrow interval \(-2-\frac{\sqrt{3}}{3}<\omega<-2\). The interior and exterior regions are matched at a thin shell made from an ordinary perfect fluid with positive energy density and pressure obeying the barotropic equation of state \(p=k\sigma\) with \(0\le k\le1\). The resulting configuration represents a composite wormhole, i.e. the thin matter shell with the Schwarzschild-like exterior region and the interior region containing the wormhole throat.</description><subject>Configurations</subject><subject>Equations of state</subject><subject>Flux density</subject><subject>Gravitational fields</subject><subject>Parameters</subject><subject>Physics - General Relativity and Quantum Cosmology</subject><subject>Thin walled shells</subject><subject>Wormholes</subject><issn>2331-8422</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2011</creationdate><recordtype>article</recordtype><sourceid>BENPR</sourceid><sourceid>GOX</sourceid><recordid>eNotj0tLw0AURgdBsNTuu5KA4C5x7tzMa6nxCYVuug_X6QRTm06caar-e1Pr6tscPs5hbA68KI2U_Jbid3soALgthNB4xiYCEXJTCnHBZiltOOdCaSElTthNFbo-pHbvswO5Yeiy-0i7lD-07sNnXyF272Hr0yU7b2ib_Ox_p2z19LiqXvLF8vm1ulvkJMHmmkjqN9KOtFEclW-MleCV8RpGBYDGCYtri6V33q2haZzRyllCa6UgiVN2dbr9a6j72HYUf-pjS31sGYHrE9DH8Dn4tK83YYi7UakW3EgFgMriL8IBSsM</recordid><startdate>20110911</startdate><enddate>20110911</enddate><creator>Sushkov, Sergey V</creator><creator>Kozyrev, Sergey M</creator><general>Cornell University Library, arXiv.org</general><scope>8FE</scope><scope>8FG</scope><scope>ABJCF</scope><scope>ABUWG</scope><scope>AFKRA</scope><scope>AZQEC</scope><scope>BENPR</scope><scope>BGLVJ</scope><scope>CCPQU</scope><scope>DWQXO</scope><scope>HCIFZ</scope><scope>L6V</scope><scope>M7S</scope><scope>PIMPY</scope><scope>PQEST</scope><scope>PQQKQ</scope><scope>PQUKI</scope><scope>PRINS</scope><scope>PTHSS</scope><scope>GOX</scope></search><sort><creationdate>20110911</creationdate><title>Composite vacuum Brans-Dicke wormholes</title><author>Sushkov, Sergey V ; Kozyrev, Sergey M</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-a519-7aa57ba7ca786036ef8951e68e7133111fc293d934ececd1ffc876c9a39952a53</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2011</creationdate><topic>Configurations</topic><topic>Equations of state</topic><topic>Flux density</topic><topic>Gravitational fields</topic><topic>Parameters</topic><topic>Physics - General Relativity and Quantum Cosmology</topic><topic>Thin walled shells</topic><topic>Wormholes</topic><toplevel>online_resources</toplevel><creatorcontrib>Sushkov, Sergey V</creatorcontrib><creatorcontrib>Kozyrev, Sergey M</creatorcontrib><collection>ProQuest SciTech Collection</collection><collection>ProQuest Technology Collection</collection><collection>Materials Science & Engineering Collection</collection><collection>ProQuest Central (Alumni Edition)</collection><collection>ProQuest Central UK/Ireland</collection><collection>ProQuest Central Essentials</collection><collection>ProQuest Central</collection><collection>Technology Collection</collection><collection>ProQuest One Community College</collection><collection>ProQuest Central Korea</collection><collection>SciTech Premium Collection</collection><collection>ProQuest Engineering Collection</collection><collection>Engineering Database</collection><collection>Publicly Available Content Database</collection><collection>ProQuest One Academic Eastern Edition (DO NOT USE)</collection><collection>ProQuest One Academic</collection><collection>ProQuest One Academic UKI Edition</collection><collection>ProQuest Central China</collection><collection>Engineering Collection</collection><collection>arXiv.org</collection><jtitle>arXiv.org</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Sushkov, Sergey V</au><au>Kozyrev, Sergey M</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Composite vacuum Brans-Dicke wormholes</atitle><jtitle>arXiv.org</jtitle><date>2011-09-11</date><risdate>2011</risdate><eissn>2331-8422</eissn><abstract>We construct a new static spherically symmetric configuration composed of interior and exterior Brans-Dicke vacua matched at a thin matter shell. Both vacua correspond to the same Brans-Dicke coupling parameter \(\omega\), however they are described by the Brans class I solution with different sets of parameters of integration. In particular, the exterior vacuum solution has \(C_{ext}(\omega)\equiv 0\). In this case the Brans class I solution for any \(\omega\) reduces to the Schwarzschild one being consistent with restrictions on the post-Newtonian parameters following from recent Cassini data. The interior region possesses a strong gravitational field, and so the interior vacuum solution has \(C_{int}(\omega)=-1/(\omega+2)\). In this case the Brans class I solution describes a wormhole spacetime provided \(\omega\) lies in the narrow interval \(-2-\frac{\sqrt{3}}{3}<\omega<-2\). The interior and exterior regions are matched at a thin shell made from an ordinary perfect fluid with positive energy density and pressure obeying the barotropic equation of state \(p=k\sigma\) with \(0\le k\le1\). The resulting configuration represents a composite wormhole, i.e. the thin matter shell with the Schwarzschild-like exterior region and the interior region containing the wormhole throat.</abstract><cop>Ithaca</cop><pub>Cornell University Library, arXiv.org</pub><doi>10.48550/arxiv.1109.2273</doi><oa>free_for_read</oa></addata></record> |
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subjects | Configurations Equations of state Flux density Gravitational fields Parameters Physics - General Relativity and Quantum Cosmology Thin walled shells Wormholes |
title | Composite vacuum Brans-Dicke wormholes |
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