REVIEW 2 major objections 2 minor 4 cited by
Explicit and covariant formula for thermodynamic volume in extended black hole thermodynamics
T0 review · 2 major / 2 minor · reviewed 2026-05-21 · grok-4.3
Pith's one-line read Thermodynamic volume in extended black hole thermodynamics receives an explicit covariant formula from action variation.
desk verdict This paper derives an explicit covariant formula for thermodynamic volume from action variation and splits it into Lagrangian and field-response pieces, but boundary terms during coupling variation could complicate the clean decomposition. read the letter →
The pith
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
The reading
What carries the argument
Variation of the action with respect to the metric and coupling constants, which produces the decomposition of the thermodynamic volume into explicit Lagrangian and field-response contributions.
What would settle it
Apply the derived formula to the Schwarzschild-AdS black hole and check whether the resulting V exactly matches the known thermodynamic volume obtained from the first law.
Extended reading notes
Core claim
The central claim is that an explicit covariant formula for the thermodynamic volume V exists and follows directly from the action variation. The formula shows that V and the conjugate quantities to other couplings each split into two contributions: one from the explicit coupling dependence in the Lagrangian and one from the adjustment of the fundamental dynamical fields. This resolves the conceptual gap in which V previously had no independent first-principles definition.
Load-bearing premise
The first law of extended thermodynamics must arise directly from varying the action with respect to both the metric and the couplings without extra boundary terms or gauge choices that would spoil the universal split.
Editorial extensions
If this is right
- The thermodynamic volume can now be computed directly from the Lagrangian for any black hole solution.
- Conjugate quantities for other couplings obey the same explicit-plus-response decomposition.
- The physical origin of the thermodynamic volume is identified as a combination of explicit and implicit dependencies in the theory.
- Extended black hole thermodynamics gains a uniform variational foundation shared by all its thermodynamic quantities.
Reading between the lines
- The formula may permit direct volume calculations in theories with higher-curvature terms or additional matter fields where indirect methods become unreliable.
- The split could link to holographic dictionary entries in which the thermodynamic volume corresponds to a specific boundary operator.
- Verification in rotating or charged black holes would test whether the decomposition remains universal beyond the static cases already checked.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The manuscript derives an explicit, covariant formula for the thermodynamic volume V in extended black hole thermodynamics. Starting from the variation of the gravitational action with respect to both the metric and the coupling constants (including the cosmological constant, with P = -Λ/8π), the authors obtain the first law including the V δP term and show that V decomposes universally into an explicit-coupling contribution from the Lagrangian plus a contribution from the response of the dynamical fields. The result is claimed to hold for general diffeomorphism-invariant theories and is illustrated with examples.
Significance. If the derivation is free of overlooked boundary contributions, the work supplies a first-principles, covariant origin for V that places it on the same footing as M, T, S, and J. This resolves a conceptual gap in extended thermodynamics and provides a general decomposition that applies to higher-curvature and other modified gravities, strengthening the theoretical basis of the framework.
major comments (2)
- [§3.1, Eq. (18)] §3.1, Eq. (18): the on-shell variation with respect to the coupling constant is presented as yielding a clean bulk decomposition, but the manuscript does not explicitly compute or cancel the possible surface terms that arise from the generalized Gibbons-Hawking boundary term when the cosmological constant is varied. A concrete demonstration that these terms vanish or do not affect the V δP contribution is required for the claimed universality and covariance.
- [§4.2] §4.2, Schwarzschild-AdS example: the derived V is stated to recover the known (4/3)π r_h³ result, yet the intermediate steps showing how the explicit-coupling and field-response pieces separately contribute are omitted. Including these steps would confirm that the decomposition is not an artifact of the final identification.
minor comments (2)
- [§2] The notation for the extended first law uses both δ and tilde-δ without a clear statement of the distinction in the main text; a brief clarification in §2 would aid readability.
- Reference to the original extended thermodynamics papers (e.g., Kastor et al.) is present but could be expanded with a short discussion of how the new formula relates to the earlier implicit definitions.
Simulated Author's Rebuttal
We thank the referee for their careful reading of the manuscript and for the constructive comments that help clarify and strengthen our results. We have revised the paper to address both major points raised.
read point-by-point responses
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Referee: [§3.1, Eq. (18)] the on-shell variation with respect to the coupling constant is presented as yielding a clean bulk decomposition, but the manuscript does not explicitly compute or cancel the possible surface terms that arise from the generalized Gibbons-Hawking boundary term when the cosmological constant is varied. A concrete demonstration that these terms vanish or do not affect the V δP contribution is required for the claimed universality and covariance.
Authors: We agree that an explicit treatment of possible surface terms is necessary to fully substantiate the universality and covariance of the formula. In the revised manuscript we have added a dedicated calculation in §3.1 that evaluates the variation of the generalized Gibbons-Hawking boundary term with respect to the cosmological constant. We demonstrate that these surface contributions cancel on-shell once the appropriate asymptotic boundary conditions and the diffeomorphism invariance of the theory are imposed, leaving the bulk term unaffected. This explicit verification is now included to support the claimed decomposition. revision: yes
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Referee: [§4.2] the derived V is stated to recover the known (4/3)π r_h³ result, yet the intermediate steps showing how the explicit-coupling and field-response pieces separately contribute are omitted. Including these steps would confirm that the decomposition is not an artifact of the final identification.
Authors: We concur that displaying the separate contributions improves transparency. The revised §4.2 now contains the intermediate expressions: the explicit-coupling piece is isolated as the direct variation of the cosmological-constant term in the Lagrangian, while the field-response piece is obtained from the on-shell metric variation. Their sum is shown to reproduce exactly (4/3)π r_h³, confirming that the decomposition is intrinsic to the general formula rather than an artifact of the final result. revision: yes
Circularity Check
Derivation of V from action variation is independent and self-contained
full rationale
The paper derives an explicit covariant expression for the thermodynamic volume directly from the on-shell variation of the action with respect to both the metric and the coupling constants (including Λ). This produces the first law as an output, with V identified as the coefficient of δP in the resulting identity, decomposed into explicit Lagrangian dependence plus dynamical field response. No step reduces the claimed formula to a prior definition of V by construction, no parameters are fitted to data and relabeled as predictions, and no load-bearing uniqueness theorem or ansatz is imported via self-citation. The central result follows from the action principle under the stated assumptions about boundary terms; it is therefore not equivalent to its inputs and receives a non-circularity finding.
Assumptions & free parameters
assumptions (2)
- domain assumption The first law of extended black hole thermodynamics follows from varying the gravitational action with respect to both dynamical fields and coupling constants.
- standard math The theory is diffeomorphism invariant so that the resulting volume expression is covariant.
Cite this review
Pith. "Pith review of Explicit and covariant formula for thermodynamic volume in extended black hole thermodynamics." pith.science (2026). https://pith.science/paper/NCYU5PLH
@misc{pith2026251201916,
author = {Pith},
title = {Pith review of: Explicit and covariant formula for thermodynamic volume in extended black hole thermodynamics},
year = {2026},
howpublished = {\url{https://pith.science/paper/NCYU5PLH}},
note = {Machine review of arXiv:2512.01916}
}
abstract
In extended black hole thermodynamics, the cosmological constant and other couplings are treated as thermodynamic variables, yielding the first law $\tilde{\delta}M = T\tilde{\delta}S+\Omega\tilde{\delta}J +\mathcal{V} \tilde{\delta}P+\cdots$, where $P\equiv -\frac{\Lambda}{8\pi}$. A long-standing conceptual gap in this framework is that, unlike $M$, $T$, $S$, $\Omega$, and $J$, the thermodynamic volume $\mathcal{V} $ lacks a first-principles definition and can only be deduced from other thermodynamic quantities. This deficiency indicates that the underlying origin of $\mathcal{V} $ remains poorly understood. In this paper, we resolve this issue and provide an explicit, covariant formula for $\mathcal{V} $. We demonstrate that $\mathcal{V} $ (and the conjugate quantities of other couplings) universally decomposes into two contributions: one arising from the explicit coupling dependence of the Lagrangian, and the other from the response of the fundamental dynamical fields. This clarifies the physical meaning of the thermodynamic volume and places it on the same footing as other intrinsic thermodynamic quantities.
Lean theorems connected to this paper
-
IndisputableMonolith/Cost/FunctionalEquation.leanwashburn_uniqueness_aczel unclear?
unclearRelation between the paper passage and the cited Recognition theorem.
We demonstrate that V (and the conjugate quantities of other couplings) universally decomposes into two contributions: one arising from the explicit coupling dependence of the Lagrangian, and the other from the response of the fundamental dynamical fields.
-
IndisputableMonolith/Foundation/RealityFromDistinction.leanreality_from_one_distinction unclear?
unclearRelation between the paper passage and the cited Recognition theorem.
the extended version of Eq.(14) becomes ... V_i = V(1)_i + V(2)_i with V(1)_i = -∫ L_i ξ_t ·ϵ and V(2)_i = ∫ F[δϕ/δα_i] ξ_t ·ϵ
What do these tags mean?
- matches
- The paper's claim is directly supported by a theorem in the formal canon.
- supports
- The theorem supports part of the paper's argument, but the paper may add assumptions or extra steps.
- extends
- The paper goes beyond the formal theorem; the theorem is a base layer rather than the whole result.
- uses
- The paper appears to rely on the theorem as machinery.
- contradicts
- The paper's claim conflicts with a theorem or certificate in the canon.
- unclear
- Pith found a possible connection, but the passage is too broad, indirect, or ambiguous to say the theorem truly supports the claim.
Forward citations
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Reference graph
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In this case, the sym- plectic currentw[δϕ,L ξϕ]≡δC[L ξϕ]− LξC[δϕ] must be added to Eq.(10)[27, 45, 46]
For readers wishing to retain thedCterm, a well- established technique is available. In this case, the sym- plectic currentw[δϕ,L ξϕ]≡δC[L ξϕ]− LξC[δϕ] must be added to Eq.(10)[27, 45, 46]. This cleverly transforms thedCterm into aδCterm, which can be absorbed into δM(the key ...
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