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Thermodynamics of Quantum Isolated Horizons with model Hamiltonians
General Relativity and Quantum Cosmology · Submitted 20 Mar 2013
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim Arguing that the known classical results must follow in the correspondence limit (viz. the equilibrium temperature as observed by a local observer) the model is fixed, yielding the energy spectrum of the QIH.
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The abstract, sentence by sentence
Following a recent proposal, we consider the most general structure possible for the Hamiltonian operator associated with the Quantum Isolated Horizon(QIH) with explanations of the underlying physical motivations. An extensive thermodynamic analysis with this model Hamiltonian is presented. Considering {\it fixed} number of punctures, the canonical partition function can now be written in the usual energy ensemble. Arguing that the known classical results must follow in the correspondence limit (viz. the equilibrium temperature as observed by a local observer) the model is fixed, yielding the energy spectrum of the QIH.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | Following a recent proposal, we consider the most general structure possible for the Hamiltonian operator associated with the Quantum Isolated Horizon(QIH) with explanations of the underlying physical motivations. | contribution 0.87 | 0.84 | 0.06 | asserted 0.92 |
| s1 | An extensive thermodynamic analysis with this model Hamiltonian is presented. | contribution 0.86 | 0.91 | 0.08 | asserted 0.99 |
| s2 | Considering {\it fixed} number of punctures, the canonical partition function can now be written in the usual energy ensemble. | method 0.91 | 0.76 | 0.07 | asserted 0.85 |
| s3 | Arguing that the known classical results must follow in the correspondence limit (viz. the equilibrium temperature as observed by a local observer) the model is fixed, yielding the energy spectrum of the QIH. | method 0.45 | 0.84 | 0.46 | asserted 0.94 |
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The paper
Original abstract
Following a recent proposal, we consider the most general structure possible for the Hamiltonian operator associated with the Quantum Isolated Horizon(QIH) with explanations of the underlying physical motivations. An extensive thermodynamic analysis with this model Hamiltonian is presented. Considering {\it fixed} number of punctures, the canonical partition function can now be written in the usual energy ensemble. Arguing that the known classical results must follow in the correspondence limit (viz. the equilibrium temperature as observed by a local observer) the model is fixed, yielding the energy spectrum of the QIH.
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How the literature uses it
2 arXiv papers cite this in 7 sentences
Papers citing it · 6 sentences without a confident label
Cites it as support 1 paper
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Furthermore, one can show [ref] that the expectation values of the proposed Hamiltonian and area operators for the QIH are proportional for a given $Ł$.
Energy spectrum of black holes : a new view · Introduction · 0.99
What it cites · 102 sentences without a confident label
Contests 1 paper
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But, the proposal was based on some ad hoc arguments and semiclassical approximations and above all, QIHs with such energy spectrum has been shown to be thermodynamically unstable [ref] .
Stability of Quantum Isolated Horizon : A Local Observer's View · Model Hamiltonian and Energy spectrum of QIH · contest 0.82
Uses the method or tool of 2 papers
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Now, to get more insight about the thermodynamical properties of QIH we shall switch over to the canonical ensemble and follow the arguments made in [ref] .
Charged Quantum Black Holes : Thermal Stability Criterion · Canonical Ensemble · 0.89
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Now, to get more insight about the thermodynamical properties of QIH we shall switch over to the canonical ensemble and follow the arguments made in [ref] .
Generalized Hawking-Page Phase Transition · Canonical Ensemble · 0.89
Compares with 3 papers
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Since, we have $=2π$, the above expression for specific heat reduces to $C=N^2d^2/d^2$, which is the expression for specific heat obtained in [ref] (correct expression to be found in the erratum).
Black hole entropy and isolated horizons thermodynamics · A Specific Case : $E_j ∝A_j$ · 0.89
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Now, as far as the thermodynamic aspect of this paper is concerned, it is worth mentioning that unlike [ref] we deal with usual canonical energy ensemble as we have an explicit structure of the Hamiltonian.
The thermodynamic limit and black hole entropy in the area ensemble · Discussion · 0.92
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Now, as far as the thermodynamic aspect of this paper is concerned, it is worth mentioning that unlike [ref] we deal with usual canonical energy ensemble as we have an explicit structure of the Hamiltonian.
On Quantum Statistical Mechanics of a Schwarzschild Black Hole · Discussion · 0.92
Cites as background 9 papers
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As we begin with the quantum theory, the available knowledge at our disposal and relevant in this context are the quantum geometric area operators and area spectrum in LQG [ref] and the theory of QIH [ref] .
Quantum Theory of Gravity I: Area Operators · Model Hamiltonian and Energy spectrum of QIH · 1.00
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As we begin with the quantum theory, the available knowledge at our disposal and relevant in this context are the quantum geometric area operators and area spectrum in LQG [ref] and the theory of QIH [ref] .
Quantum Geometry and Black Hole Entropy · Model Hamiltonian and Energy spectrum of QIH · 1.00
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As we begin with the quantum theory, the available knowledge at our disposal and relevant in this context are the quantum geometric area operators and area spectrum in LQG [ref] and the theory of QIH [ref] .
Quantum Geometry of Isolated Horizons and Black Hole Entropy · Model Hamiltonian and Energy spectrum of QIH · 1.00
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