Black Hole Entropy from Indistinguishable Quantum Geometric Excitations

In loop quantum gravity the quantum geometry of a black hole horizon consists of discrete nonperturbative quantum geometric excitations (or punctures) labeled by spins, which are responsible for the quantum area of the horizon. If these punctures are compared to a gas of particles, then the spins as...

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Main Author: Abhishek Majhi
Format: Article
Language:English
Published: Wiley 2016-01-01
Series:Advances in High Energy Physics
Online Access:http://dx.doi.org/10.1155/2016/2903867
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author Abhishek Majhi
author_facet Abhishek Majhi
author_sort Abhishek Majhi
collection DOAJ
description In loop quantum gravity the quantum geometry of a black hole horizon consists of discrete nonperturbative quantum geometric excitations (or punctures) labeled by spins, which are responsible for the quantum area of the horizon. If these punctures are compared to a gas of particles, then the spins associated with the punctures can be viewed as single puncture area levels analogous to single particle energy levels. Consequently, if we assume these punctures to be indistinguishable, the microstate count for the horizon resembles that of Bose-Einstein counting formula for gas of particles. For the Bekenstein-Hawking area law to follow from the entropy calculation in the large area limit, the Barbero-Immirzi parameter (γ) approximately takes a constant value. As a by-product, we are able to speculate the state counting formula for the SU(2) quantum Chern-Simons theory coupled to indistinguishable sources in the weak coupling limit.
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spelling doaj-art-5173d69c928f4c25bdfc499391dfe3b52025-02-03T07:25:39ZengWileyAdvances in High Energy Physics1687-73571687-73652016-01-01201610.1155/2016/29038672903867Black Hole Entropy from Indistinguishable Quantum Geometric ExcitationsAbhishek Majhi0The Institute of Mathematical Sciences, CIT Campus, 4th Cross St., Taramani, Chennai, Tamil Nadu, IndiaIn loop quantum gravity the quantum geometry of a black hole horizon consists of discrete nonperturbative quantum geometric excitations (or punctures) labeled by spins, which are responsible for the quantum area of the horizon. If these punctures are compared to a gas of particles, then the spins associated with the punctures can be viewed as single puncture area levels analogous to single particle energy levels. Consequently, if we assume these punctures to be indistinguishable, the microstate count for the horizon resembles that of Bose-Einstein counting formula for gas of particles. For the Bekenstein-Hawking area law to follow from the entropy calculation in the large area limit, the Barbero-Immirzi parameter (γ) approximately takes a constant value. As a by-product, we are able to speculate the state counting formula for the SU(2) quantum Chern-Simons theory coupled to indistinguishable sources in the weak coupling limit.http://dx.doi.org/10.1155/2016/2903867
spellingShingle Abhishek Majhi
Black Hole Entropy from Indistinguishable Quantum Geometric Excitations
Advances in High Energy Physics
title Black Hole Entropy from Indistinguishable Quantum Geometric Excitations
title_full Black Hole Entropy from Indistinguishable Quantum Geometric Excitations
title_fullStr Black Hole Entropy from Indistinguishable Quantum Geometric Excitations
title_full_unstemmed Black Hole Entropy from Indistinguishable Quantum Geometric Excitations
title_short Black Hole Entropy from Indistinguishable Quantum Geometric Excitations
title_sort black hole entropy from indistinguishable quantum geometric excitations
url http://dx.doi.org/10.1155/2016/2903867
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