Reissner–Nordström spacetimes in torsion modified gravity: isometries and perihelion precession
Abstract We analyze the orbits of a unit mass body in a background Reissner–Nordstr$$\ddot{\textrm{o}}$$m (RN) black hole in $$d$$$$=$$$$(3+1)$$ from the perspectives of Geometric Torsion (GT) modified gravity theory in $$(4+1)$$ dimensional bulk. A 4-form flux in bulk GT theory in $$d$$$$=$$$$(4+1)...
Ausführliche Beschreibung
Gespeichert in:
| Autor*in: |
Kumar, Jitesh [verfasserIn] Gupta, Rohit Kumar [verfasserIn] Kar, Supriya [verfasserIn] Rang, Nitish [verfasserIn] Singh, Sunita [verfasserIn] |
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| Format: |
E-Artikel |
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| Sprache: |
Englisch |
| Erschienen: |
2024 |
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| Schlagwörter: |
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| Anmerkung: |
© The Author(s), under exclusive licence to Springer Science+Business Media, LLC, part of Springer Nature 2024. Springer Nature or its licensor (e.g. a society or other partner) holds exclusive rights to this article under a publishing agreement with the author(s) or other rightsholder(s); author self-archiving of the accepted manuscript version of this article is solely governed by the terms of such publishing agreement and applicable law. |
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| Übergeordnetes Werk: |
Enthalten in: General relativity and gravitation - Springer US, 1970, 56(2024), 10 vom: Okt. |
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| Übergeordnetes Werk: |
volume:56 ; year:2024 ; number:10 ; month:10 |
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| DOI / URN: |
10.1007/s10714-024-03315-8 |
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SPR057771669 |
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| 520 | |a Abstract We analyze the orbits of a unit mass body in a background Reissner–Nordstr$$\ddot{\textrm{o}}$$m (RN) black hole in $$d$$$$=$$$$(3+1)$$ from the perspectives of Geometric Torsion (GT) modified gravity theory in $$(4+1)$$ dimensional bulk. A 4-form flux in bulk GT theory in $$d$$$$=$$$$(4+1)$$ has been shown to ensure a mass dipole correction to the $$(3+1)$$ dimensional gravity theory by Gupta, Kar and Rang recently. We argue that the dipole correction contributes topologically to the known exact geometries in General Theory of Relativity (GTR). Furthermore, the topological correction has been identified with non-Newtonian potential underlying a $$B_2 \wedge F_2$$ coupling term to Einstein–Hilbert action. The winding numbers ensured by the BF coupling to $$d=(3+1)$$ action in the framework presumably provide a clue towards a tunneling instanton in theory. | ||
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| 650 | 4 | |a Geometric torsion |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a Perihelion precession |7 (dpeaa)DE-He213 | |
| 700 | 1 | |a Gupta, Rohit Kumar |e verfasserin |4 aut | |
| 700 | 1 | |a Kar, Supriya |e verfasserin |4 aut | |
| 700 | 1 | |a Rang, Nitish |e verfasserin |4 aut | |
| 700 | 1 | |a Singh, Sunita |e verfasserin |4 aut | |
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10.1007/s10714-024-03315-8 doi (DE-627)SPR057771669 (SPR)s10714-024-03315-8-e DE-627 ger DE-627 rakwb eng 530 VZ 33.00 bkl Kumar, Jitesh verfasserin aut Reissner–Nordström spacetimes in torsion modified gravity: isometries and perihelion precession 2024 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © The Author(s), under exclusive licence to Springer Science+Business Media, LLC, part of Springer Nature 2024. Springer Nature or its licensor (e.g. a society or other partner) holds exclusive rights to this article under a publishing agreement with the author(s) or other rightsholder(s); author self-archiving of the accepted manuscript version of this article is solely governed by the terms of such publishing agreement and applicable law. Abstract We analyze the orbits of a unit mass body in a background Reissner–Nordstr$$\ddot{\textrm{o}}$$m (RN) black hole in $$d$$$$=$$$$(3+1)$$ from the perspectives of Geometric Torsion (GT) modified gravity theory in $$(4+1)$$ dimensional bulk. A 4-form flux in bulk GT theory in $$d$$$$=$$$$(4+1)$$ has been shown to ensure a mass dipole correction to the $$(3+1)$$ dimensional gravity theory by Gupta, Kar and Rang recently. We argue that the dipole correction contributes topologically to the known exact geometries in General Theory of Relativity (GTR). Furthermore, the topological correction has been identified with non-Newtonian potential underlying a $$B_2 \wedge F_2$$ coupling term to Einstein–Hilbert action. The winding numbers ensured by the BF coupling to $$d=(3+1)$$ action in the framework presumably provide a clue towards a tunneling instanton in theory. Killing symmetries (dpeaa)DE-He213 General relativity (dpeaa)DE-He213 Higher dimensional gauge theory (dpeaa)DE-He213 Geometric torsion (dpeaa)DE-He213 Perihelion precession (dpeaa)DE-He213 Gupta, Rohit Kumar verfasserin aut Kar, Supriya verfasserin aut Rang, Nitish verfasserin aut Singh, Sunita verfasserin aut Enthalten in General relativity and gravitation Springer US, 1970 56(2024), 10 vom: Okt. (DE-627)320528928 (DE-600)2015524-4 1572-9532 nnns volume:56 year:2024 number:10 month:10 https://dx.doi.org/10.1007/s10714-024-03315-8 X:SPRINGER Resolving-System lizenzpflichtig Volltext SYSFLAG_0 GBV_SPRINGER SSG-OPC-AST GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_69 GBV_ILN_70 GBV_ILN_72 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_2574 GBV_ILN_4029 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4116 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4155 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4315 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 33.00 VZ AR 56 2024 10 10 |
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10.1007/s10714-024-03315-8 doi (DE-627)SPR057771669 (SPR)s10714-024-03315-8-e DE-627 ger DE-627 rakwb eng 530 VZ 33.00 bkl Kumar, Jitesh verfasserin aut Reissner–Nordström spacetimes in torsion modified gravity: isometries and perihelion precession 2024 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © The Author(s), under exclusive licence to Springer Science+Business Media, LLC, part of Springer Nature 2024. Springer Nature or its licensor (e.g. a society or other partner) holds exclusive rights to this article under a publishing agreement with the author(s) or other rightsholder(s); author self-archiving of the accepted manuscript version of this article is solely governed by the terms of such publishing agreement and applicable law. Abstract We analyze the orbits of a unit mass body in a background Reissner–Nordstr$$\ddot{\textrm{o}}$$m (RN) black hole in $$d$$$$=$$$$(3+1)$$ from the perspectives of Geometric Torsion (GT) modified gravity theory in $$(4+1)$$ dimensional bulk. A 4-form flux in bulk GT theory in $$d$$$$=$$$$(4+1)$$ has been shown to ensure a mass dipole correction to the $$(3+1)$$ dimensional gravity theory by Gupta, Kar and Rang recently. We argue that the dipole correction contributes topologically to the known exact geometries in General Theory of Relativity (GTR). Furthermore, the topological correction has been identified with non-Newtonian potential underlying a $$B_2 \wedge F_2$$ coupling term to Einstein–Hilbert action. The winding numbers ensured by the BF coupling to $$d=(3+1)$$ action in the framework presumably provide a clue towards a tunneling instanton in theory. Killing symmetries (dpeaa)DE-He213 General relativity (dpeaa)DE-He213 Higher dimensional gauge theory (dpeaa)DE-He213 Geometric torsion (dpeaa)DE-He213 Perihelion precession (dpeaa)DE-He213 Gupta, Rohit Kumar verfasserin aut Kar, Supriya verfasserin aut Rang, Nitish verfasserin aut Singh, Sunita verfasserin aut Enthalten in General relativity and gravitation Springer US, 1970 56(2024), 10 vom: Okt. (DE-627)320528928 (DE-600)2015524-4 1572-9532 nnns volume:56 year:2024 number:10 month:10 https://dx.doi.org/10.1007/s10714-024-03315-8 X:SPRINGER Resolving-System lizenzpflichtig Volltext SYSFLAG_0 GBV_SPRINGER SSG-OPC-AST GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_69 GBV_ILN_70 GBV_ILN_72 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_2574 GBV_ILN_4029 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4116 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4155 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4315 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 33.00 VZ AR 56 2024 10 10 |
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10.1007/s10714-024-03315-8 doi (DE-627)SPR057771669 (SPR)s10714-024-03315-8-e DE-627 ger DE-627 rakwb eng 530 VZ 33.00 bkl Kumar, Jitesh verfasserin aut Reissner–Nordström spacetimes in torsion modified gravity: isometries and perihelion precession 2024 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © The Author(s), under exclusive licence to Springer Science+Business Media, LLC, part of Springer Nature 2024. Springer Nature or its licensor (e.g. a society or other partner) holds exclusive rights to this article under a publishing agreement with the author(s) or other rightsholder(s); author self-archiving of the accepted manuscript version of this article is solely governed by the terms of such publishing agreement and applicable law. Abstract We analyze the orbits of a unit mass body in a background Reissner–Nordstr$$\ddot{\textrm{o}}$$m (RN) black hole in $$d$$$$=$$$$(3+1)$$ from the perspectives of Geometric Torsion (GT) modified gravity theory in $$(4+1)$$ dimensional bulk. A 4-form flux in bulk GT theory in $$d$$$$=$$$$(4+1)$$ has been shown to ensure a mass dipole correction to the $$(3+1)$$ dimensional gravity theory by Gupta, Kar and Rang recently. We argue that the dipole correction contributes topologically to the known exact geometries in General Theory of Relativity (GTR). Furthermore, the topological correction has been identified with non-Newtonian potential underlying a $$B_2 \wedge F_2$$ coupling term to Einstein–Hilbert action. The winding numbers ensured by the BF coupling to $$d=(3+1)$$ action in the framework presumably provide a clue towards a tunneling instanton in theory. Killing symmetries (dpeaa)DE-He213 General relativity (dpeaa)DE-He213 Higher dimensional gauge theory (dpeaa)DE-He213 Geometric torsion (dpeaa)DE-He213 Perihelion precession (dpeaa)DE-He213 Gupta, Rohit Kumar verfasserin aut Kar, Supriya verfasserin aut Rang, Nitish verfasserin aut Singh, Sunita verfasserin aut Enthalten in General relativity and gravitation Springer US, 1970 56(2024), 10 vom: Okt. (DE-627)320528928 (DE-600)2015524-4 1572-9532 nnns volume:56 year:2024 number:10 month:10 https://dx.doi.org/10.1007/s10714-024-03315-8 X:SPRINGER Resolving-System lizenzpflichtig Volltext SYSFLAG_0 GBV_SPRINGER SSG-OPC-AST GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_69 GBV_ILN_70 GBV_ILN_72 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_2574 GBV_ILN_4029 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4116 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4155 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4315 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 33.00 VZ AR 56 2024 10 10 |
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10.1007/s10714-024-03315-8 doi (DE-627)SPR057771669 (SPR)s10714-024-03315-8-e DE-627 ger DE-627 rakwb eng 530 VZ 33.00 bkl Kumar, Jitesh verfasserin aut Reissner–Nordström spacetimes in torsion modified gravity: isometries and perihelion precession 2024 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © The Author(s), under exclusive licence to Springer Science+Business Media, LLC, part of Springer Nature 2024. Springer Nature or its licensor (e.g. a society or other partner) holds exclusive rights to this article under a publishing agreement with the author(s) or other rightsholder(s); author self-archiving of the accepted manuscript version of this article is solely governed by the terms of such publishing agreement and applicable law. Abstract We analyze the orbits of a unit mass body in a background Reissner–Nordstr$$\ddot{\textrm{o}}$$m (RN) black hole in $$d$$$$=$$$$(3+1)$$ from the perspectives of Geometric Torsion (GT) modified gravity theory in $$(4+1)$$ dimensional bulk. A 4-form flux in bulk GT theory in $$d$$$$=$$$$(4+1)$$ has been shown to ensure a mass dipole correction to the $$(3+1)$$ dimensional gravity theory by Gupta, Kar and Rang recently. We argue that the dipole correction contributes topologically to the known exact geometries in General Theory of Relativity (GTR). Furthermore, the topological correction has been identified with non-Newtonian potential underlying a $$B_2 \wedge F_2$$ coupling term to Einstein–Hilbert action. The winding numbers ensured by the BF coupling to $$d=(3+1)$$ action in the framework presumably provide a clue towards a tunneling instanton in theory. Killing symmetries (dpeaa)DE-He213 General relativity (dpeaa)DE-He213 Higher dimensional gauge theory (dpeaa)DE-He213 Geometric torsion (dpeaa)DE-He213 Perihelion precession (dpeaa)DE-He213 Gupta, Rohit Kumar verfasserin aut Kar, Supriya verfasserin aut Rang, Nitish verfasserin aut Singh, Sunita verfasserin aut Enthalten in General relativity and gravitation Springer US, 1970 56(2024), 10 vom: Okt. (DE-627)320528928 (DE-600)2015524-4 1572-9532 nnns volume:56 year:2024 number:10 month:10 https://dx.doi.org/10.1007/s10714-024-03315-8 X:SPRINGER Resolving-System lizenzpflichtig Volltext SYSFLAG_0 GBV_SPRINGER SSG-OPC-AST GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_69 GBV_ILN_70 GBV_ILN_72 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_2574 GBV_ILN_4029 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4116 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4155 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4315 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 33.00 VZ AR 56 2024 10 10 |
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10.1007/s10714-024-03315-8 doi (DE-627)SPR057771669 (SPR)s10714-024-03315-8-e DE-627 ger DE-627 rakwb eng 530 VZ 33.00 bkl Kumar, Jitesh verfasserin aut Reissner–Nordström spacetimes in torsion modified gravity: isometries and perihelion precession 2024 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © The Author(s), under exclusive licence to Springer Science+Business Media, LLC, part of Springer Nature 2024. Springer Nature or its licensor (e.g. a society or other partner) holds exclusive rights to this article under a publishing agreement with the author(s) or other rightsholder(s); author self-archiving of the accepted manuscript version of this article is solely governed by the terms of such publishing agreement and applicable law. Abstract We analyze the orbits of a unit mass body in a background Reissner–Nordstr$$\ddot{\textrm{o}}$$m (RN) black hole in $$d$$$$=$$$$(3+1)$$ from the perspectives of Geometric Torsion (GT) modified gravity theory in $$(4+1)$$ dimensional bulk. A 4-form flux in bulk GT theory in $$d$$$$=$$$$(4+1)$$ has been shown to ensure a mass dipole correction to the $$(3+1)$$ dimensional gravity theory by Gupta, Kar and Rang recently. We argue that the dipole correction contributes topologically to the known exact geometries in General Theory of Relativity (GTR). Furthermore, the topological correction has been identified with non-Newtonian potential underlying a $$B_2 \wedge F_2$$ coupling term to Einstein–Hilbert action. The winding numbers ensured by the BF coupling to $$d=(3+1)$$ action in the framework presumably provide a clue towards a tunneling instanton in theory. Killing symmetries (dpeaa)DE-He213 General relativity (dpeaa)DE-He213 Higher dimensional gauge theory (dpeaa)DE-He213 Geometric torsion (dpeaa)DE-He213 Perihelion precession (dpeaa)DE-He213 Gupta, Rohit Kumar verfasserin aut Kar, Supriya verfasserin aut Rang, Nitish verfasserin aut Singh, Sunita verfasserin aut Enthalten in General relativity and gravitation Springer US, 1970 56(2024), 10 vom: Okt. (DE-627)320528928 (DE-600)2015524-4 1572-9532 nnns volume:56 year:2024 number:10 month:10 https://dx.doi.org/10.1007/s10714-024-03315-8 X:SPRINGER Resolving-System lizenzpflichtig Volltext SYSFLAG_0 GBV_SPRINGER SSG-OPC-AST GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_69 GBV_ILN_70 GBV_ILN_72 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2118 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_2574 GBV_ILN_4029 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4116 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4155 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4315 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 33.00 VZ AR 56 2024 10 10 |
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Springer Nature or its licensor (e.g. a society or other partner) holds exclusive rights to this article under a publishing agreement with the author(s) or other rightsholder(s); author self-archiving of the accepted manuscript version of this article is solely governed by the terms of such publishing agreement and applicable law.</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">Abstract We analyze the orbits of a unit mass body in a background Reissner–Nordstr$$\ddot{\textrm{o}}$$m (RN) black hole in $$d$$$$=$$$$(3+1)$$ from the perspectives of Geometric Torsion (GT) modified gravity theory in $$(4+1)$$ dimensional bulk. A 4-form flux in bulk GT theory in $$d$$$$=$$$$(4+1)$$ has been shown to ensure a mass dipole correction to the $$(3+1)$$ dimensional gravity theory by Gupta, Kar and Rang recently. We argue that the dipole correction contributes topologically to the known exact geometries in General Theory of Relativity (GTR). Furthermore, the topological correction has been identified with non-Newtonian potential underlying a $$B_2 \wedge F_2$$ coupling term to Einstein–Hilbert action. The winding numbers ensured by the BF coupling to $$d=(3+1)$$ action in the framework presumably provide a clue towards a tunneling instanton in theory.</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Killing symmetries</subfield><subfield code="7">(dpeaa)DE-He213</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">General relativity</subfield><subfield code="7">(dpeaa)DE-He213</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Higher dimensional gauge theory</subfield><subfield code="7">(dpeaa)DE-He213</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Geometric torsion</subfield><subfield code="7">(dpeaa)DE-He213</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Perihelion precession</subfield><subfield code="7">(dpeaa)DE-He213</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Gupta, Rohit 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Kumar, Jitesh |
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Kumar, Jitesh ddc 530 bkl 33.00 misc Killing symmetries misc General relativity misc Higher dimensional gauge theory misc Geometric torsion misc Perihelion precession Reissner–Nordström spacetimes in torsion modified gravity: isometries and perihelion precession |
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530 VZ 33.00 bkl Reissner–Nordström spacetimes in torsion modified gravity: isometries and perihelion precession Killing symmetries (dpeaa)DE-He213 General relativity (dpeaa)DE-He213 Higher dimensional gauge theory (dpeaa)DE-He213 Geometric torsion (dpeaa)DE-He213 Perihelion precession (dpeaa)DE-He213 |
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Reissner–Nordström spacetimes in torsion modified gravity: isometries and perihelion precession |
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reissner–nordström spacetimes in torsion modified gravity: isometries and perihelion precession |
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Reissner–Nordström spacetimes in torsion modified gravity: isometries and perihelion precession |
| abstract |
Abstract We analyze the orbits of a unit mass body in a background Reissner–Nordstr$$\ddot{\textrm{o}}$$m (RN) black hole in $$d$$$$=$$$$(3+1)$$ from the perspectives of Geometric Torsion (GT) modified gravity theory in $$(4+1)$$ dimensional bulk. A 4-form flux in bulk GT theory in $$d$$$$=$$$$(4+1)$$ has been shown to ensure a mass dipole correction to the $$(3+1)$$ dimensional gravity theory by Gupta, Kar and Rang recently. We argue that the dipole correction contributes topologically to the known exact geometries in General Theory of Relativity (GTR). Furthermore, the topological correction has been identified with non-Newtonian potential underlying a $$B_2 \wedge F_2$$ coupling term to Einstein–Hilbert action. The winding numbers ensured by the BF coupling to $$d=(3+1)$$ action in the framework presumably provide a clue towards a tunneling instanton in theory. © The Author(s), under exclusive licence to Springer Science+Business Media, LLC, part of Springer Nature 2024. Springer Nature or its licensor (e.g. a society or other partner) holds exclusive rights to this article under a publishing agreement with the author(s) or other rightsholder(s); author self-archiving of the accepted manuscript version of this article is solely governed by the terms of such publishing agreement and applicable law. |
| abstractGer |
Abstract We analyze the orbits of a unit mass body in a background Reissner–Nordstr$$\ddot{\textrm{o}}$$m (RN) black hole in $$d$$$$=$$$$(3+1)$$ from the perspectives of Geometric Torsion (GT) modified gravity theory in $$(4+1)$$ dimensional bulk. A 4-form flux in bulk GT theory in $$d$$$$=$$$$(4+1)$$ has been shown to ensure a mass dipole correction to the $$(3+1)$$ dimensional gravity theory by Gupta, Kar and Rang recently. We argue that the dipole correction contributes topologically to the known exact geometries in General Theory of Relativity (GTR). Furthermore, the topological correction has been identified with non-Newtonian potential underlying a $$B_2 \wedge F_2$$ coupling term to Einstein–Hilbert action. The winding numbers ensured by the BF coupling to $$d=(3+1)$$ action in the framework presumably provide a clue towards a tunneling instanton in theory. © The Author(s), under exclusive licence to Springer Science+Business Media, LLC, part of Springer Nature 2024. Springer Nature or its licensor (e.g. a society or other partner) holds exclusive rights to this article under a publishing agreement with the author(s) or other rightsholder(s); author self-archiving of the accepted manuscript version of this article is solely governed by the terms of such publishing agreement and applicable law. |
| abstract_unstemmed |
Abstract We analyze the orbits of a unit mass body in a background Reissner–Nordstr$$\ddot{\textrm{o}}$$m (RN) black hole in $$d$$$$=$$$$(3+1)$$ from the perspectives of Geometric Torsion (GT) modified gravity theory in $$(4+1)$$ dimensional bulk. A 4-form flux in bulk GT theory in $$d$$$$=$$$$(4+1)$$ has been shown to ensure a mass dipole correction to the $$(3+1)$$ dimensional gravity theory by Gupta, Kar and Rang recently. We argue that the dipole correction contributes topologically to the known exact geometries in General Theory of Relativity (GTR). Furthermore, the topological correction has been identified with non-Newtonian potential underlying a $$B_2 \wedge F_2$$ coupling term to Einstein–Hilbert action. The winding numbers ensured by the BF coupling to $$d=(3+1)$$ action in the framework presumably provide a clue towards a tunneling instanton in theory. © The Author(s), under exclusive licence to Springer Science+Business Media, LLC, part of Springer Nature 2024. Springer Nature or its licensor (e.g. a society or other partner) holds exclusive rights to this article under a publishing agreement with the author(s) or other rightsholder(s); author self-archiving of the accepted manuscript version of this article is solely governed by the terms of such publishing agreement and applicable law. |
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| title_short |
Reissner–Nordström spacetimes in torsion modified gravity: isometries and perihelion precession |
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https://dx.doi.org/10.1007/s10714-024-03315-8 |
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Gupta, Rohit Kumar Kar, Supriya Rang, Nitish Singh, Sunita |
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Gupta, Rohit Kumar Kar, Supriya Rang, Nitish Singh, Sunita |
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2024-10-18T04:52:24.481Z |
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|
| score |
7.4000835 |