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Thermodynamics of Horndeski black holes with non-minimal derivative coupling
High Energy Physics - Theory · Submitted 22 Jul 2016
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim Our result indicates that this class of Horndeski black holes presents rich thermodynamic behaviors and critical phenomena.
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The abstract, sentence by sentence
We explore thermodynamic properties of a new class of Horndeski black holes whose action contains a non-minimal kinetic coupling of a massless real scalar and the Einstein tensor. Our treatment is based on the well-accepted consideration, where the cosmological constant is dealt with as thermodynamic pressure and the mass of black holes as thermodynamic enthalpy. We resort to a newly introduced intensive thermodynamic variable, i.e., the coupling strength of the scalar and tensor whose dimension is length square, and thus yield both the generalized first law of thermodynamics and the generalized Smarr relation. Our result indicates that this class of Horndeski black holes presents rich thermodynamic behaviors and critical phenomena. Especially in the case of the presence of an electric field, these black holes undergo two phase transitions. Once the charge parameter exceeds its critical value, or the cosmological parameter does not exceed its critical value, no phase transitions happen and the black holes are stable. As a by-product, we point out that the coupling strength acts as the thermodynamic pressure in the behavior of thermodynamics.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We explore thermodynamic properties of a new class of Horndeski black holes whose action contains a non-minimal kinetic coupling of a massless real scalar and the Einstein tensor. | contribution 0.99 | 0.84 | 0.05 | asserted 0.96 |
| s1 | Our treatment is based on the well-accepted consideration, where the cosmological constant is dealt with as thermodynamic pressure and the mass of black holes as thermodynamic enthalpy. | method 0.89 | 0.25 | 0.03 | asserted 1.00 |
| s2 | We resort to a newly introduced intensive thermodynamic variable, i.e., the coupling strength of the scalar and tensor whose dimension is length square, and thus yield both the generalized first law of thermodynamics and the generalized Smarr relation. | method 0.68 | 0.94 | 0.11 | asserted 1.00 |
| s3 | Our result indicates that this class of Horndeski black holes presents rich thermodynamic behaviors and critical phenomena. | result 0.73 | 0.89 | 0.47 | hedged possibility 0.89 |
| s4 | Especially in the case of the presence of an electric field, these black holes undergo two phase transitions. | result 1.00 | 0.88 | 0.14 | asserted 0.99 |
| s5 | Once the charge parameter exceeds its critical value, or the cosmological parameter does not exceed its critical value, no phase transitions happen and the black holes are stable. | result 0.96 | 0.87 | 0.14 | asserted 1.00 |
| s6 | As a by-product, we point out that the coupling strength acts as the thermodynamic pressure in the behavior of thermodynamics. | result 0.70 | 0.91 | 0.11 | asserted 0.99 |
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The paper
Original abstract
We explore thermodynamic properties of a new class of Horndeski black holes whose action contains a non-minimal kinetic coupling of a massless real scalar and the Einstein tensor. Our treatment is based on the well-accepted consideration, where the cosmological constant is dealt with as thermodynamic pressure and the mass of black holes as thermodynamic enthalpy. We resort to a newly introduced intensive thermodynamic variable, i.e., the coupling strength of the scalar and tensor whose dimension is length square, and thus yield both the generalized first law of thermodynamics and the generalized Smarr relation. Our result indicates that this class of Horndeski black holes presents rich thermodynamic behaviors and critical phenomena. Especially in the case of the presence of an electric field, these black holes undergo two phase transitions. Once the charge parameter exceeds its critical value, or the cosmological parameter does not exceed its critical value, no phase transitions happen and the black holes are stable. As a by-product, we point out that the coupling strength acts as the thermodynamic pressure in the behavior of thermodynamics.
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How the literature uses it
11 arXiv papers cite this in 15 sentences
Papers citing it · 6 sentences without a confident label
Cites it as background 8 papers
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Black holes solutions in a special Einstein-Horndeski gravity are derived in [ref] , while thermodynamics for black holes in Einstein-Horndeski is investigated in [ref] .
P-V criticality in the extended phase space of black holes in Einstein-Horndeski gravity · Introduction · 0.97
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Hairy black holes in Horndeski gravity have also been widely constructed and analyzed, including the radially dependent scalar field [ref] and time-dependent scalar field [ref] .
Rings and images of Horndeski hairy black hole illuminated by various thin accretions · Introduction · 0.92
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Therefore, the hairy black holes have been widely constructed and analyzed, including the radially dependent scalar field [ref] and time-dependent scalar field [ref] .
The effect of scalar hair on the charged black hole with the images from accretions disk · Introduction · 0.80
What it cites · 25 sentences without a confident label
Uses the method or tool of 5 papers
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[ref] , one can regard the mass of black holes as the thermodynamic enthalpy, [equation] The Bekenstein-Hawking entropy is one-fourth of the event horizon area, [equation] and the thermodynamic temperature can be calculated to be [equation] When the thermodynamic pressure $P$ is regarded as [equation] the extensive variable conjugate to it, i.e., the thermodynamic volume $V$ has the form, [equation]
Enthalpy and the Mechanics of AdS Black Holes · Scenario without charge · 0.85
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[ref] , one can regard the mass of black holes as the thermodynamic enthalpy, [equation] The Bekenstein-Hawking entropy is one-fourth of the event horizon area, [equation] and the thermodynamic temperature can be calculated to be [equation] When the thermodynamic pressure $P$ is regarded as [equation] the extensive variable conjugate to it, i.e., the thermodynamic volume $V$ has the form, [equation]
The cosmological constant and the black hole equation of state · Scenario without charge · 0.85
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[ref] , one can regard the mass of black holes as the thermodynamic enthalpy, [equation] The Bekenstein-Hawking entropy is one-fourth of the event horizon area, [equation] and the thermodynamic temperature can be calculated to be [equation] When the thermodynamic pressure $P$ is regarded as [equation] the extensive variable conjugate to it, i.e., the thermodynamic volume $V$ has the form, [equation]
Pressure and volume in the first law of black hole thermodynamics · Scenario without charge · 0.85
Cites as background 20 papers
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[ref] for the case of a negative cosmological constant.
Asymptotically locally AdS and flat black holes in Horndeski theory · Introduction · 0.86
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[ref] for the case of a negative cosmological constant.
Solutions in the scalar-tensor theory with nonminimal derivative coupling · Introduction · 0.86
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In particular, the thermodynamics of black holes in anti-de Sitter (AdS) spacetime [ref] has acquired great progress since the AdS/CFT duality plays a pivotal role in recent developments of theoretical physics [ref] .
Black Hole Thermodynamics · Introduction · 0.98
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