Weak deflection angle of a dirty black hole
In this paper, we present the weak deflection angle in a Schwarzschild black hole of mass m surrounded by the dark matter of mass M and thickness Δrs. The Gauss-Bonnet theorem, formulated for asymptotic spacetimes, is found to be ill-behaved in the third-order of 1/Δrs for very large Δrs. Using the...
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oai:animorepository.dlsu.edu.ph:faculty_research-17442024-03-25T07:58:34Z Weak deflection angle of a dirty black hole Pantig, Reggie C. Rodulfo, Emmanuel T. In this paper, we present the weak deflection angle in a Schwarzschild black hole of mass m surrounded by the dark matter of mass M and thickness Δrs. The Gauss-Bonnet theorem, formulated for asymptotic spacetimes, is found to be ill-behaved in the third-order of 1/Δrs for very large Δrs. Using the finite-distance for the radial locations of the source and the receiver, we derived the expression for the weak deflection angle up to the third-order of 1/Δrs using Ishihara (et al.) method. The result showed that the required dark matter thickness is ∼23mM for the deviations in the weak deflection angle to occur. Such thickness requirement is better by a factor of 2 as compared to the deviations in the shadow radius (∼3mM). It implies that the use of the weak deflection angle in detecting dark matter effects in one's galaxy is better than using any deviations in the shadow radius. 2020-08-01T07:00:00Z text text/html https://animorepository.dlsu.edu.ph/faculty_research/745 info:doi/10.1016/j.cjph.2020.06.015 Faculty Research Work Animo Repository Schwarzschild black holes Dark matter (Astronomy) Gauss-Bonnet theorem |
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Schwarzschild black holes Dark matter (Astronomy) Gauss-Bonnet theorem Pantig, Reggie C. Rodulfo, Emmanuel T. Weak deflection angle of a dirty black hole |
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In this paper, we present the weak deflection angle in a Schwarzschild black hole of mass m surrounded by the dark matter of mass M and thickness Δrs. The Gauss-Bonnet theorem, formulated for asymptotic spacetimes, is found to be ill-behaved in the third-order of 1/Δrs for very large Δrs. Using the finite-distance for the radial locations of the source and the receiver, we derived the expression for the weak deflection angle up to the third-order of 1/Δrs using Ishihara (et al.) method. The result showed that the required dark matter thickness is ∼23mM for the deviations in the weak deflection angle to occur. Such thickness requirement is better by a factor of 2 as compared to the deviations in the shadow radius (∼3mM). It implies that the use of the weak deflection angle in detecting dark matter effects in one's galaxy is better than using any deviations in the shadow radius. |
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Pantig, Reggie C. Rodulfo, Emmanuel T. |
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Pantig, Reggie C. Rodulfo, Emmanuel T. |
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Pantig, Reggie C. |
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Weak deflection angle of a dirty black hole |
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Weak deflection angle of a dirty black hole |
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Weak deflection angle of a dirty black hole |
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Weak deflection angle of a dirty black hole |
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Weak deflection angle of a dirty black hole |
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weak deflection angle of a dirty black hole |
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