Thermal chaos of quantum-corrected-AdS black hole in the extended phase space
We briefly analyzed the equation of state and critical points of the quantum-corrected-AdS black hole and used the Melnikov method to study its thermal chaotic behavior in the extended phase space of flat, closed, and open universes. The results show that the black hole’s thermodynamic behavior is s...
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Published in | The European physical journal. C, Particles and fields Vol. 84; no. 11; pp. 1133 - 14 |
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Main Authors | , , , , |
Format | Journal Article |
Language | English |
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01.11.2024
Springer Nature B.V SpringerOpen |
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ISSN | 1434-6052 1434-6044 1434-6052 |
DOI | 10.1140/epjc/s10052-024-13417-x |
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Abstract | We briefly analyzed the equation of state and critical points of the quantum-corrected-AdS black hole and used the Melnikov method to study its thermal chaotic behavior in the extended phase space of flat, closed, and open universes. The results show that the black hole’s thermodynamic behavior is similar to that of the Van der Waals system. Although the critical ratios at the critical points in the three types of universes differ, they are all independent of the quantum correction parameter. Only an open universe can attain the critical ratio of
3
8
corresponding to the Van der Waals system, while in the other two universes, the critical ratio is always greater than this value. For chaos, time perturbations will lead to chaotic behavior when their amplitude exceeds a critical value that depends on the quantum correction parameter and the radius of the dust sphere in the FRW model. Based on this, we found that the chaotic behavior of the black hole varies across different universes depending on the quantum correction parameter, but this parameter always makes chaos more likely. Using the value of the quantum correction parameter determined by Meissner, chaos is always more difficult to occur in an open universe compared to the other two types of universes. Which universe is most prone to chaos depends on the radius of the dust sphere. Finally, chaotic behavior is always present under spatial perturbations. |
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AbstractList | We briefly analyzed the equation of state and critical points of the quantum-corrected-AdS black hole and used the Melnikov method to study its thermal chaotic behavior in the extended phase space of flat, closed, and open universes. The results show that the black hole’s thermodynamic behavior is similar to that of the Van der Waals system. Although the critical ratios at the critical points in the three types of universes differ, they are all independent of the quantum correction parameter. Only an open universe can attain the critical ratio of
3
8
corresponding to the Van der Waals system, while in the other two universes, the critical ratio is always greater than this value. For chaos, time perturbations will lead to chaotic behavior when their amplitude exceeds a critical value that depends on the quantum correction parameter and the radius of the dust sphere in the FRW model. Based on this, we found that the chaotic behavior of the black hole varies across different universes depending on the quantum correction parameter, but this parameter always makes chaos more likely. Using the value of the quantum correction parameter determined by Meissner, chaos is always more difficult to occur in an open universe compared to the other two types of universes. Which universe is most prone to chaos depends on the radius of the dust sphere. Finally, chaotic behavior is always present under spatial perturbations. We briefly analyzed the equation of state and critical points of the quantum-corrected-AdS black hole and used the Melnikov method to study its thermal chaotic behavior in the extended phase space of flat, closed, and open universes. The results show that the black hole’s thermodynamic behavior is similar to that of the Van der Waals system. Although the critical ratios at the critical points in the three types of universes differ, they are all independent of the quantum correction parameter. Only an open universe can attain the critical ratio of 38 corresponding to the Van der Waals system, while in the other two universes, the critical ratio is always greater than this value. For chaos, time perturbations will lead to chaotic behavior when their amplitude exceeds a critical value that depends on the quantum correction parameter and the radius of the dust sphere in the FRW model. Based on this, we found that the chaotic behavior of the black hole varies across different universes depending on the quantum correction parameter, but this parameter always makes chaos more likely. Using the value of the quantum correction parameter determined by Meissner, chaos is always more difficult to occur in an open universe compared to the other two types of universes. Which universe is most prone to chaos depends on the radius of the dust sphere. Finally, chaotic behavior is always present under spatial perturbations. Abstract We briefly analyzed the equation of state and critical points of the quantum-corrected-AdS black hole and used the Melnikov method to study its thermal chaotic behavior in the extended phase space of flat, closed, and open universes. The results show that the black hole’s thermodynamic behavior is similar to that of the Van der Waals system. Although the critical ratios at the critical points in the three types of universes differ, they are all independent of the quantum correction parameter. Only an open universe can attain the critical ratio of $$\frac{3}{8}$$ 3 8 corresponding to the Van der Waals system, while in the other two universes, the critical ratio is always greater than this value. For chaos, time perturbations will lead to chaotic behavior when their amplitude exceeds a critical value that depends on the quantum correction parameter and the radius of the dust sphere in the FRW model. Based on this, we found that the chaotic behavior of the black hole varies across different universes depending on the quantum correction parameter, but this parameter always makes chaos more likely. Using the value of the quantum correction parameter determined by Meissner, chaos is always more difficult to occur in an open universe compared to the other two types of universes. Which universe is most prone to chaos depends on the radius of the dust sphere. Finally, chaotic behavior is always present under spatial perturbations. We briefly analyzed the equation of state and critical points of the quantum-corrected-AdS black hole and used the Melnikov method to study its thermal chaotic behavior in the extended phase space of flat, closed, and open universes. The results show that the black hole’s thermodynamic behavior is similar to that of the Van der Waals system. Although the critical ratios at the critical points in the three types of universes differ, they are all independent of the quantum correction parameter. Only an open universe can attain the critical ratio of $$\frac{3}{8}$$ 3 8 corresponding to the Van der Waals system, while in the other two universes, the critical ratio is always greater than this value. For chaos, time perturbations will lead to chaotic behavior when their amplitude exceeds a critical value that depends on the quantum correction parameter and the radius of the dust sphere in the FRW model. Based on this, we found that the chaotic behavior of the black hole varies across different universes depending on the quantum correction parameter, but this parameter always makes chaos more likely. Using the value of the quantum correction parameter determined by Meissner, chaos is always more difficult to occur in an open universe compared to the other two types of universes. Which universe is most prone to chaos depends on the radius of the dust sphere. Finally, chaotic behavior is always present under spatial perturbations. |
ArticleNumber | 1133 |
Author | Deng, Jian-Bo You, Lei Wang, Rui-Bo Tang, Yu-Cheng Hu, Xian-Ru |
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Cites_doi | 10.1103/PhysRevD.60.104026 10.1016/j.dark.2023.101168 10.1103/PhysRevLett.130.101501 10.1088/0264-9381/21/22/015 10.1103/PhysRevD.99.106012 10.1007/JHEP11(2012)110 10.1103/PhysRevD.108.104004 10.1088/0264-9381/21/22/014 10.3390/galaxies2010089 10.1017/CBO9780511803260 10.1103/PhysRevD.109.064012 10.1088/0264-9381/26/19/195011 10.1140/epjc/s10052-024-12914-3 10.1103/PhysRevD.7.2333 10.1103/PhysRevD.110.026002 10.1007/BF02345020 10.1088/0264-9381/20/9/304 10.3390/universe10100393 10.1140/epjc/s10052-020-7813-1 10.1140/epjc/s10052-024-13505-y 10.1007/JHEP07(2012)033 10.1140/epjc/s10052-023-11800-8 10.1103/PhysRevD.55.4848 10.1088/1361-6382/aa5c69 10.1016/0196-8858(85)90008-9 10.1093/oso/9780198508397.001.0001 10.1088/0264-9381/31/4/042001 10.1016/j.physletb.2018.04.014 10.1007/s10714-019-2612-4 10.1016/0370-1573(90)90012-Q |
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Snippet | We briefly analyzed the equation of state and critical points of the quantum-corrected-AdS black hole and used the Melnikov method to study its thermal chaotic... Abstract We briefly analyzed the equation of state and critical points of the quantum-corrected-AdS black hole and used the Melnikov method to study its... |
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StartPage | 1133 |
SubjectTerms | Astronomy Astrophysics and Cosmology Black holes Critical point Dust Elementary Particles Equations of state Hadrons Heavy Ions Measurement Science and Instrumentation Nuclear Energy Nuclear Physics Parameters Perturbation Physics Physics and Astronomy Quantum Field Theories Quantum Field Theory Regular Article - Theoretical Physics String Theory Thermodynamic properties Universe |
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Title | Thermal chaos of quantum-corrected-AdS black hole in the extended phase space |
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