MG13 - Talk detail |
Participant |
Pradhan, Parthapratim | |||||||
Institution |
Department of Physics, V. S. Mahavidyalaya - Manikpara - Paschim Medinipur - West Bengal - India | |||||||
Session |
BH3 |
Accepted |
Yes |
Order |
4 |
Time |
10' | |
Talk |
Oral abstract |
Title |
Lyapunov Exponent and Extremal Black Hole | |||||
Co-authors | ||||||||
Abstract |
We explicitly derive the principal Lyapunov Exponent \emph{in terms of the radial equation of ISCO}(Innermost Stable Circular Orbit) and reciprocal of the Critical Exponent can also be expressed as in terms of the radial ISCO equation for Reisner Nordstr{\o}m) black-hole space-times. Using Lyapunov Exponent, we show that the stability and instability of equatorial circular geodesics, both massive and massless particles for such types of black-hole space-time. |
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Session |
BH1 |
Accepted |
No |
Order |
Time |
|||
Talk |
Poster abstract |
Title |
No ISCOs in Charged Myers Perry Black Hole Spacetime by measuring Lyapunov Exponent | |||||
Co-authors | ||||||||
Abstract |
We explicitly show that for more than four dimensions$(N \geq 3)$, there are no Innermost Stable Circular Orbit (ISCO) in charged Myers Perry blackhole spacetime. This result is verified by measuring Lyapunov Exponent. Using it, we show that the instability of equatorial circular geodesics, both massive and massless particles for such types of black-hole space-time. |
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Session |
GT3 |
Accepted |
Yes |
Order |
4 |
Time |
14:45 | |
Talk |
Poster abstract |
Title |
Stability of Equatorial Circular Geodesics for Kerr-Newman Spacetime via Lyapunov Exponent | |||||
Co-authors | ||||||||
Abstract |
We explicitly computed the principal Lyapunov Exponent \emph{in terms of the radial equation of ISCO}(Innermost Stable Circular Orbit) and reciprocal of the Critical Exponent can also be expressed as in terms of the radial ISCO equation. Using Lyapunov Exponent, we show that the stability and instability of equatorial circular geodesics, both massive and massless particles for Kerr-Newman black-hole space-time. The other aspect we have studied that among the all possible circular geodesics, which encircle the central black-hole, the ISCO has \emph{greatest} orbital period than the null circular orbit as measured by the asymptotic observers. Therefore, the ISCO provide the \emph{slowest way} to circle the black-hole. |
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Session |
AT1 |
Accepted |
Yes |
Order |
991 |
Time |
||
Talk |
Poster abstract |
Title |
No ISCOs in Charged Myers Perry spacettime by measuring Lyapunov Exponent | |||||
Co-authors | ||||||||
Abstract |
\begin{abstract} We explicitly show that for more than four dimensions$(N \geq 3)$, there are no Innermost Stable Circular Orbit (ISCO) in charged Myers Perry blackhole spacetime. This result is verified by measuring Lyapunov Exponent. Using it, we show that the instability of equatorial circular geodesics, both massive and massless particles for such types of black-hole space-time. \end{abstract} |
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Session |
GT3 |
Accepted |
Yes |
Order |
10 |
Time |
17:21 | |
Talk |
Oral abstract |
Title |
Extremal Versus Non-Extremal Blackhole | |||||
Co-authors | ||||||||
Abstract |
\begin{abstract} In this talk, I shall addresses a number of issues regarding the disparity between precisely extremely and nearly extremely geometries. \end{abstract} |
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