Asymptotically (anti)-de Sitter solutions in Gauss-Bonnet gravity without a cosmological constant
In this paper I show that one can have asymptotically de Sitter, anti-de Sitter (AdS), and flat solutions in Gauss-Bonnet gravity without a cosmological constant term in field equations. First, I introduce static solutions whose three surfaces at fixed r and t have constant positive (k=1), negative...
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description | In this paper I show that one can have asymptotically de Sitter, anti-de Sitter (AdS), and flat solutions in Gauss-Bonnet gravity without a cosmological constant term in field equations. First, I introduce static solutions whose three surfaces at fixed r and t have constant positive (k=1), negative (k=-1), or zero (k=0) curvature. I show that for k={+-}1 one can have asymptotically de Sitter, AdS, and flat spacetimes, while for the case of k=0, one has only asymptotically AdS solutions. Some of these solutions present naked singularities, while some others are black hole or topological black hole solutions. I also find that the geometrical mass of these five-dimensional spacetimes is m+2{alpha}|k|, which is different from the geometrical mass m of the solutions of Einstein gravity. This feature occurs only for the five-dimensional solutions, and is not repeated for the solutions of Gauss-Bonnet gravity in higher dimensions. Second, I add angular momentum to the static solutions with k=0, and introduce the asymptotically AdS charged rotating solutions of Gauss-Bonnet gravity. Finally, I introduce a class of solutions which yields an asymptotically AdS spacetime with a longitudinal magnetic field, which presents a naked singularity, and generalize it to the case of magnetic rotating solutions with two rotation parameters. |
doi_str_mv | 10.1103/PhysRevD.70.064019 |
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H.</creator><creatorcontrib>Dehghani, M. H.</creatorcontrib><description>In this paper I show that one can have asymptotically de Sitter, anti-de Sitter (AdS), and flat solutions in Gauss-Bonnet gravity without a cosmological constant term in field equations. First, I introduce static solutions whose three surfaces at fixed r and t have constant positive (k=1), negative (k=-1), or zero (k=0) curvature. I show that for k={+-}1 one can have asymptotically de Sitter, AdS, and flat spacetimes, while for the case of k=0, one has only asymptotically AdS solutions. Some of these solutions present naked singularities, while some others are black hole or topological black hole solutions. I also find that the geometrical mass of these five-dimensional spacetimes is m+2{alpha}|k|, which is different from the geometrical mass m of the solutions of Einstein gravity. This feature occurs only for the five-dimensional solutions, and is not repeated for the solutions of Gauss-Bonnet gravity in higher dimensions. Second, I add angular momentum to the static solutions with k=0, and introduce the asymptotically AdS charged rotating solutions of Gauss-Bonnet gravity. Finally, I introduce a class of solutions which yields an asymptotically AdS spacetime with a longitudinal magnetic field, which presents a naked singularity, and generalize it to the case of magnetic rotating solutions with two rotation parameters.</description><identifier>ISSN: 1550-7998</identifier><identifier>ISSN: 0556-2821</identifier><identifier>EISSN: 1550-2368</identifier><identifier>EISSN: 1089-4918</identifier><identifier>DOI: 10.1103/PhysRevD.70.064019</identifier><language>eng</language><publisher>United States</publisher><subject>ANGULAR MOMENTUM ; ASYMPTOTIC SOLUTIONS ; BLACK HOLES ; COSMOLOGICAL CONSTANT ; COSMOLOGY ; DE SITTER GROUP ; EINSTEIN FIELD EQUATIONS ; GRAVITATION ; MAGNETIC FIELDS ; MASS ; PHYSICS OF ELEMENTARY PARTICLES AND FIELDS ; ROTATION ; SINGULARITY ; SPACE-TIME ; TOPOLOGY</subject><ispartof>Physical review. 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D, Particles and fields</title><description>In this paper I show that one can have asymptotically de Sitter, anti-de Sitter (AdS), and flat solutions in Gauss-Bonnet gravity without a cosmological constant term in field equations. First, I introduce static solutions whose three surfaces at fixed r and t have constant positive (k=1), negative (k=-1), or zero (k=0) curvature. I show that for k={+-}1 one can have asymptotically de Sitter, AdS, and flat spacetimes, while for the case of k=0, one has only asymptotically AdS solutions. Some of these solutions present naked singularities, while some others are black hole or topological black hole solutions. I also find that the geometrical mass of these five-dimensional spacetimes is m+2{alpha}|k|, which is different from the geometrical mass m of the solutions of Einstein gravity. This feature occurs only for the five-dimensional solutions, and is not repeated for the solutions of Gauss-Bonnet gravity in higher dimensions. Second, I add angular momentum to the static solutions with k=0, and introduce the asymptotically AdS charged rotating solutions of Gauss-Bonnet gravity. Finally, I introduce a class of solutions which yields an asymptotically AdS spacetime with a longitudinal magnetic field, which presents a naked singularity, and generalize it to the case of magnetic rotating solutions with two rotation parameters.</description><subject>ANGULAR MOMENTUM</subject><subject>ASYMPTOTIC SOLUTIONS</subject><subject>BLACK HOLES</subject><subject>COSMOLOGICAL CONSTANT</subject><subject>COSMOLOGY</subject><subject>DE SITTER GROUP</subject><subject>EINSTEIN FIELD EQUATIONS</subject><subject>GRAVITATION</subject><subject>MAGNETIC FIELDS</subject><subject>MASS</subject><subject>PHYSICS OF ELEMENTARY PARTICLES AND FIELDS</subject><subject>ROTATION</subject><subject>SINGULARITY</subject><subject>SPACE-TIME</subject><subject>TOPOLOGY</subject><issn>1550-7998</issn><issn>0556-2821</issn><issn>1550-2368</issn><issn>1089-4918</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2004</creationdate><recordtype>article</recordtype><recordid>eNo1kE1LAzEURYMoWKt_wFXAjS6mvkwyycyyVq1CQfFjHV4zSRuZTsokrcy_t6V19e6Dy-FyCLlmMGIM-P37so8fdvs4UjACKYBVJ2TAigKynMvy9JhVVZXn5CLGHwCeS6UGBMexX61TSN5g0_T0Ftvk77La0k-fku1oDM0m-dBG6ls6xU2M2UNoW5voosOtTz399WkZNokiNSGuQhMWe9buaWPa0S7JmcMm2qvjHZLv56evyUs2e5u-TsazzHBVpqx2jkkxBwdc5ghlwWou5dw6VTOBNhccLVaoOMwFAtZOmIpJh7lQknMs-JDcHLghJq-j8cmapdlPNUnnoKDIBdu18kPLdCHGzjq97vwKu14z0HuV-l-lVqAPKvkfIbFqtg</recordid><startdate>20040915</startdate><enddate>20040915</enddate><creator>Dehghani, M. 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H.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c378t-dff164b0f0362a0851d366bef7d14ae243aea9a730b4a0adf4c916fa247633a53</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2004</creationdate><topic>ANGULAR MOMENTUM</topic><topic>ASYMPTOTIC SOLUTIONS</topic><topic>BLACK HOLES</topic><topic>COSMOLOGICAL CONSTANT</topic><topic>COSMOLOGY</topic><topic>DE SITTER GROUP</topic><topic>EINSTEIN FIELD EQUATIONS</topic><topic>GRAVITATION</topic><topic>MAGNETIC FIELDS</topic><topic>MASS</topic><topic>PHYSICS OF ELEMENTARY PARTICLES AND FIELDS</topic><topic>ROTATION</topic><topic>SINGULARITY</topic><topic>SPACE-TIME</topic><topic>TOPOLOGY</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Dehghani, M. H.</creatorcontrib><collection>CrossRef</collection><collection>OSTI.GOV</collection><jtitle>Physical review. D, Particles and fields</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Dehghani, M. H.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Asymptotically (anti)-de Sitter solutions in Gauss-Bonnet gravity without a cosmological constant</atitle><jtitle>Physical review. D, Particles and fields</jtitle><date>2004-09-15</date><risdate>2004</risdate><volume>70</volume><issue>6</issue><artnum>064019</artnum><issn>1550-7998</issn><issn>0556-2821</issn><eissn>1550-2368</eissn><eissn>1089-4918</eissn><abstract>In this paper I show that one can have asymptotically de Sitter, anti-de Sitter (AdS), and flat solutions in Gauss-Bonnet gravity without a cosmological constant term in field equations. First, I introduce static solutions whose three surfaces at fixed r and t have constant positive (k=1), negative (k=-1), or zero (k=0) curvature. I show that for k={+-}1 one can have asymptotically de Sitter, AdS, and flat spacetimes, while for the case of k=0, one has only asymptotically AdS solutions. Some of these solutions present naked singularities, while some others are black hole or topological black hole solutions. I also find that the geometrical mass of these five-dimensional spacetimes is m+2{alpha}|k|, which is different from the geometrical mass m of the solutions of Einstein gravity. This feature occurs only for the five-dimensional solutions, and is not repeated for the solutions of Gauss-Bonnet gravity in higher dimensions. Second, I add angular momentum to the static solutions with k=0, and introduce the asymptotically AdS charged rotating solutions of Gauss-Bonnet gravity. Finally, I introduce a class of solutions which yields an asymptotically AdS spacetime with a longitudinal magnetic field, which presents a naked singularity, and generalize it to the case of magnetic rotating solutions with two rotation parameters.</abstract><cop>United States</cop><doi>10.1103/PhysRevD.70.064019</doi></addata></record> |
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subjects | ANGULAR MOMENTUM ASYMPTOTIC SOLUTIONS BLACK HOLES COSMOLOGICAL CONSTANT COSMOLOGY DE SITTER GROUP EINSTEIN FIELD EQUATIONS GRAVITATION MAGNETIC FIELDS MASS PHYSICS OF ELEMENTARY PARTICLES AND FIELDS ROTATION SINGULARITY SPACE-TIME TOPOLOGY |
title | Asymptotically (anti)-de Sitter solutions in Gauss-Bonnet gravity without a cosmological constant |
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