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REVIEW 1 major objections 1 references

Comment on "Ideal clocks -- a convenient fiction" by K. Lorek et al

T0 review · 1 major / 0 minor · reviewed 2026-07-02 · grok-4.3

Pith's one-line read The decay probability of a uniformly accelerated quantum clock excludes an unphysical cross-wedge term from earlier calculations.

desk verdict This is a narrow but direct correction that removes an unphysical cross-wedge term from the 2015 decay probability. read the letter →

arxiv 2607.00059 v1 pith:3AHFKURG submitted 2026-06-30 quant-ph gr-qc

classification quant-phgr-qc
keywords RindlerwedgesquantumclocksdecayprobabilitycausalconsistencyacceleratedframesUnruheffect
verification ladder T0 review T1 audit T2 compute T3 formal

The pith

A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.

The reading

This paper corrects an equation in a prior study of quantum clocks undergoing uniform acceleration. The original expression contained a term mixing amplitudes across spatially separated Rindler wedges, which are causally disconnected. Removing this term leaves only the thermal contributions that respect the separation of the wedges. Such a correction matters because any model of time in relativity must avoid implying influences between disconnected regions. The derivation reuses the conformal coordinates introduced in the original work.

What carries the argument

The Rindler conformal coordinates (τ, ξ) with the requirement to exclude cross-wedge terms to maintain the spatial separation of the wedges.

What would settle it

An independent calculation of the decay probability that either includes or excludes the cross-wedge term depending on whether the separation is enforced would test the correction.

Watch

Extended reading notes

Core claim

The corrected probability for the decay of the accelerated clock, derived in Rindler conformal coordinates (τ, ξ), contains solely the causally consistent thermal terms and omits the cross-wedge term |γ̄_{K 1}|^2.

Load-bearing premise

The assumption that the Rindler conformal coordinates can be used to derive the decay probability and that excluding the cross-wedge term is the proper way to enforce causal consistency.

Editorial extensions

If this is right

  • The decay probability aligns with expectations from the thermal Unruh radiation without extraneous contributions.
  • Models of ideal clocks in accelerated frames require enforcement of causal separation to remain physical.
  • Discussions of clock behavior in relativity should verify the absence of terms linking disconnected spacetime regions.

Reading between the lines

Editorial extensions of the paper, not claims the author makes directly.

  • This may require revisiting other calculations of quantum processes in Rindler spacetime that used similar expressions.
  • Testing could involve deriving the probability in alternative coordinate systems to confirm consistency.
  • Implications extend to how quantum information is handled across acceleration horizons.
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Editorial analysis

A structured set of objections, weighed in public.

Desk editor's note, referee report, simulated authors' rebuttal, and a circularity audit.

Referee Report

1 major / 0 minor

Summary. This comment paper identifies an oversight in Eq.(19) of Lorek et al. (Class. Quantum Grav. 32 175003, 2015), where the decay probability for a uniformly accelerated quantum clock included an unphysical cross-wedge term |¯γ_{K1}|^2 that violates the spatial separation of Rindler wedges. The authors re-derive the probability from the original paper's Rindler conformal coordinates (τ, ξ), retaining only the causally consistent thermal terms, and discuss implications for relativistic clock models.

Significance. If the correction holds, it removes a causal inconsistency from the model of accelerated quantum clocks, strengthening the physical consistency of relativistic quantum decay calculations in non-inertial frames. The reuse of the 2015 paper's exact coordinates provides a direct and parameter-free route to the fix, which is a methodological strength for such comments.

major comments (1)
  1. [Derivation of corrected probability (referenced in abstract)] The central claim rests on the corrected probability being derivable while excluding the cross-wedge term; however, without an explicit side-by-side display of the original Eq.(19) versus the new expression (including the intermediate steps from the (τ, ξ) coordinates), the support for the removal cannot be verified as load-bearing for the correction.

Simulated Author's Rebuttal

1 responses · 0 unresolved

We thank the referee for their careful reading of our comment and for the constructive suggestion regarding the presentation of the derivation. We address the single major comment below.

read point-by-point responses
  1. Referee: The central claim rests on the corrected probability being derivable while excluding the cross-wedge term; however, without an explicit side-by-side display of the original Eq.(19) versus the new expression (including the intermediate steps from the (τ, ξ) coordinates), the support for the removal cannot be verified as load-bearing for the correction.

    Authors: We agree that an explicit side-by-side comparison, together with the intermediate steps, would make the correction more transparent and easier to verify. In the revised manuscript we will add: (i) the original Eq.(19) from Lorek et al. reproduced verbatim, (ii) the corrected probability expression, and (iii) the key intermediate steps starting from the Rindler conformal coordinates (τ, ξ) that show how the unphysical cross-wedge term |¯γ_{K1}|^2 is excluded while only the causally consistent thermal contributions remain. revision: yes

Circularity Check

0 steps flagged · score 0.0 of 10

No significant circularity detected

full rationale

The paper identifies and removes an unphysical cross-wedge term from the original Eq.(19) by enforcing spatial separation of Rindler wedges, then re-derives the probability using the same conformal coordinates (τ, ξ) already employed in the 2015 work. This step follows directly from the geometry of the wedges and does not reduce any claimed prediction to a fitted parameter, self-definition, or load-bearing self-citation chain. The correction is presented as a straightforward consistency fix with no internal reduction to the paper's own inputs.

Assumptions & free parameters 0 free parameters · 0 assumptions · 0 invented entities

No free parameters, axioms, or invented entities are identifiable from the abstract alone.

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Cite this review

Pith. "Pith review of Comment on "Ideal clocks -- a convenient fiction" by K. Lorek et al." pith.science (2026). https://pith.science/paper/3AHFKURG

@misc{pith2026260700059,
  author       = {Pith},
  title        = {Pith review of: Comment on "Ideal clocks -- a convenient fiction" by K. Lorek et al},
  year         = {2026},
  howpublished = {\url{https://pith.science/paper/3AHFKURG}},
  note         = {Machine review of arXiv:2607.00059}
}
abstract

We correct a subtle oversight in Eq.(19) of K. Lorek et al. [Class. Quantum Grav. 32 175003 (2015)] concerning the decay probability of a uniformly accelerated quantum clock. The original expression included unphysical cross-wedge term ($|\bar{\gamma}_{K 1}|^2$) violating the spatial separation of Rindler wedges. We derive the corrected probability using the paper's Rindler conformal coordinates $(\tau, \xi)$, retaining only causally consistent thermal terms, and discuss implications for relativistic clock models.

Discussion (0). Continue with ORCID to comment.

Reference graph

Works this paper leans on

1 extracted references · 1 canonical work pages

  1. [1]

    Ideal clocks - a convenient fiction

    [1] K. Lorek, J. Louko and A. Dragan, “Ideal clocks - a convenient fiction,” Class. Quant. Grav.32, no.17, 175003 (2015) [arXiv:1503.01025 [quant-ph]]. 5

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Reviewed July 2, 2026 · model on record in the stance chip above.