Talk detail

MG13 - Talk detail

Back to previous page

 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.

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.

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.

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}

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}

Back to previous page