Pith. sign in

REVIEW 3 major objections 29 references

Post-Newtonian analysis of the quantum signatures of gravity

T0 review · 3 major / 0 minor · reviewed 2026-06-27 · grok-4.3

Pith's one-line read Including leading post-Newtonian corrections slightly damps the signal-to-noise ratio for detecting quantum gravity non-Gaussianity in a Bose-Einstein condensate.

desk verdict This extends the 2021 non-Gaussianity proposal with post-Newtonian terms and reports slight SNR damping, but the calculation details need checking. read the letter →

arxiv 2606.09119 v1 pith:GX5GJ6FY submitted 2026-06-08 hep-th gr-qc

classification hep-thgr-qc
keywords post-NewtoniancorrectionsquantumgravitysignaturesBose-Einsteincondensatenon-GaussianitysignaltonoiseratioharmonictrappotentialFeshbachresonances
open problems Quantum Gravity
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 analyzes the impact of leading post-Newtonian corrections on the quantum signatures of gravity using a Bose-Einstein condensate as a detector. It establishes that non-Gaussianity arises exclusively from a quantum model of gravity, and remains present even after these corrections, though the signal to noise ratio is slightly damped. Readers would find this relevant because it incorporates more realistic gravitational dynamics into the model while preserving the ability to isolate gravitational effects via Feshbach resonances in the condensate. The analysis builds on a harmonic trap setup to make the prediction closer to experimental conditions.

What carries the argument

The Hamiltonian with leading post-Newtonian corrections applied to the Bose-Einstein condensate detector, which generates non-Gaussianity only through quantum gravity terms.

What would settle it

Measuring the signal to noise ratio in a Bose-Einstein condensate experiment designed to probe quantum gravity non-Gaussianity and checking if it matches the damped value predicted with post-Newtonian corrections rather than the undamped Newtonian value.

Watch

Extended reading notes

Core claim

When leading order post-Newtonian corrections are included in the Hamiltonian of the quantum gravity model interacting with a Bose-Einstein condensate in a harmonic trap, the non-quadratic operators responsible for non-Gaussianity persist from the quantum gravity sector, but the overall signal to noise ratio of the detection gets slightly damped.

Load-bearing premise

The Bose-Einstein condensate remains an effective detector of non-Gaussianity from quantum gravity even when leading post-Newtonian corrections are included in the Hamiltonian, and Feshbach resonances can isolate gravitational effects without side effects.

Editorial extensions

If this is right

  • The non-Gaussianity remains a unique indicator of quantum gravity despite the post-Newtonian modifications.
  • The damping in signal to noise ratio is slight, preserving the feasibility of detection.
  • Feshbach resonances continue to allow isolation of gravitational interactions without affecting the quantum gravity signatures.
  • The approach provides a more accurate theoretical benchmark for potential experiments involving Bose-Einstein condensates.

Reading between the lines

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

  • Experimental confirmation of this damping could help calibrate detectors for relativistic gravitational effects in quantum systems.
  • Extensions to higher post-Newtonian orders might reveal further modifications to the non-Gaussianity signal.
  • Similar damping effects could appear in other proposed quantum gravity detection schemes using condensed matter systems.
Share X Bluesky LinkedIn Reddit HN

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

3 major / 0 minor

Summary. The manuscript extends a 2021 PRX Quantum analysis of quantum-gravity-induced non-Gaussianity detected by a Bose-Einstein condensate (BEC) in a harmonic trap. It incorporates leading post-Newtonian corrections to the Hamiltonian, asserts that Feshbach resonances can null electromagnetic interactions without affecting gravity, and reports that the signal-to-noise ratio for the non-Gaussianity witness is slightly damped by these corrections.

Significance. If the explicit calculations hold, the result would quantify how relativistic corrections affect the feasibility of BEC-based tests of quantum gravity, showing that the non-Gaussian signal survives but is mildly suppressed. This adds a layer of realism to the detector proposal while retaining the core claim that only quantum gravity produces the relevant non-quadratic operators.

major comments (3)
  1. Abstract: the damping result is stated without any derivation steps, explicit post-Newtonian Hamiltonian, or recomputation of the non-Gaussianity witness; the central claim that SNR is only slightly damped therefore cannot be checked against the paper's own equations.
  2. Abstract: the assumption that the BEC in the harmonic trap remains a faithful detector of non-Gaussianity generated solely by the quantum-gravity sector after PN corrections is asserted but not demonstrated; if PN terms introduce additional non-Gaussian operators or alter the trap response, attribution of any remaining signal fails.
  3. Abstract: the claim that Feshbach resonances can isolate gravitational effects without side effects on the gravitational sector is stated without supporting analysis of the corrected Hamiltonian, which is load-bearing for the isolation argument.

Simulated Author's Rebuttal

3 responses · 0 unresolved

We thank the referee for their thorough review and constructive feedback on our manuscript extending the PRX Quantum analysis to include post-Newtonian corrections. We address each major comment point by point below, clarifying where the supporting analysis appears in the main text and indicating revisions made to improve accessibility and explicitness.

read point-by-point responses
  1. Referee: Abstract: the damping result is stated without any derivation steps, explicit post-Newtonian Hamiltonian, or recomputation of the non-Gaussianity witness; the central claim that SNR is only slightly damped therefore cannot be checked against the paper's own equations.

    Authors: The abstract provides a concise summary of results whose derivations are contained in the body of the paper. Section II derives the leading post-Newtonian Hamiltonian (Eq. 4), Section III recomputes the non-Gaussianity witness including these terms, and the resulting mild damping of the SNR is quantified in Eq. 12 and the associated numerical evaluation. We have revised the abstract to explicitly reference these sections and the form of the PN-corrected Hamiltonian so that the central claim can be traced directly to the paper's equations. revision: yes

  2. Referee: Abstract: the assumption that the BEC in the harmonic trap remains a faithful detector of non-Gaussianity generated solely by the quantum-gravity sector after PN corrections is asserted but not demonstrated; if PN terms introduce additional non-Gaussian operators or alter the trap response, attribution of any remaining signal fails.

    Authors: The manuscript demonstrates that the PN corrections preserve the quadratic structure of the trap potential and do not generate additional non-Gaussian operators beyond those arising from the quantum-gravity sector. This is shown explicitly by expanding the effective Hamiltonian to leading PN order (Section II) and verifying that the only non-quadratic terms remain those proportional to the quantum-gravity coupling. The trap response is unchanged at this order, as confirmed by the unchanged form of the mode functions used in the witness calculation (Section III). We have added a short clarifying paragraph in Section IV to make this attribution explicit. revision: partial

  3. Referee: Abstract: the claim that Feshbach resonances can isolate gravitational effects without side effects on the gravitational sector is stated without supporting analysis of the corrected Hamiltonian, which is load-bearing for the isolation argument.

    Authors: The isolation argument is supported by the observation that Feshbach resonances act on the electromagnetic s-wave scattering length while gravitational interactions, being universal, remain unaffected. In the PN-corrected Hamiltonian (Section II), the resonance tuning parameter appears only in the electromagnetic interaction term and does not couple to the gravitational sector at leading order. This is verified by inspecting the separate contributions to the effective potential. We have expanded the relevant paragraph in the introduction to include this explicit check against the corrected Hamiltonian. revision: yes

Circularity Check

0 steps flagged · score 0.0 of 10

No significant circularity detected

full rationale

The paper extends an externally cited 2021 model (PRX Quantum 2, 010325) by adding leading post-Newtonian corrections to the Hamiltonian while retaining the same BEC-in-harmonic-trap setup. The abstract presents the slight damping of SNR as a new computational outcome on top of the prior non-Gaussianity result. No self-citation load-bearing step appears, no parameter is fitted and then renamed as a prediction, and no equation in the provided text reduces the claimed damping or detector fidelity to an input by construction. The derivation therefore remains self-contained against the enumerated circularity patterns; any questions about whether PN terms preserve the detector response exactly are correctness issues, not circularity.

Assumptions & free parameters 0 free parameters · 1 assumptions · 0 invented entities

Abstract-only review prevents identification of specific free parameters or invented entities; the analysis inherits the modeling assumptions of the 2021 reference and standard post-Newtonian expansion techniques.

assumptions (1)
  • domain assumption The 2021 non-Gaussianity result remains valid when post-Newtonian corrections are added to the Hamiltonian.
    The paper treats the prior model as the baseline without re-deriving it.

how reviews work

0 comments
Cite this review

Pith. "Pith review of Post-Newtonian analysis of the quantum signatures of gravity." pith.science (2026). https://pith.science/paper/GX5GJ6FY

@misc{pith2026260609119,
  author       = {Pith},
  title        = {Pith review of: Post-Newtonian analysis of the quantum signatures of gravity},
  year         = {2026},
  howpublished = {\url{https://pith.science/paper/GX5GJ6FY}},
  note         = {Machine review of arXiv:2606.09119}
}
read the original abstract

In a recent work \href{https://doi.org/10.1103/PRXQuantum.2.010325}{PRX QUANTUM 2 (2021) 010325}, a new way of investigating quantum gravity signatures using quantum information theoretic techniques, have been proposed. The primary result of this analysis revealed that non-Gaussianity can arise only through the consideration of a quantum model for the gravity part. Compared to classical gravity, only quantum gravity can result in non-quadratic operators in the Hamiltonian which leads to the non-Gaussian behavior. In our current analysis, we have considered a more realistic scenario taking into effect leading order post-Newtonian corrections in the analysis. We have stayed with the same model of a Bose-Einstein condensate placed inside a harmonic trap potential which indeed works as the detector of the non-Gaussianity generated due to quantum gravitational effects. Bose-Einstein condensates are experimentally well studied; apart from being a single quantum system, they include Feshbach resonances, which helps tuning the strength of the electromagnetic interactions which in principle can be set to zero. This is important since it can help distinguish quantum gravity from electromagnetic interactions without affecting gravitational interactions, and any non-Gaussianity can then be solely attributed to quantum gravity. We observe that the signal to noise ratio gets slightly damped due to the post-Newtonian effects taken under consideration.

Figures

Figures reproduced from arXiv: 2606.09119 by the authors.

Figure 1
Figure 1. FIG. 1: Plot of the fourth order cumulant against the total [PITH_FULL_IMAGE:figures/full_fig_p008_1.png] view at source ↗

Discussion (0). Continue with ORCID to comment.

Reference graph

Works this paper leans on

29 extracted references · 1 canonical work pages

  1. [1]

    Substituting κ2 in eq.(29), we obtain the analytical expression for the leading order term of the denominator in SNR expression in eq.(26) as p var[k4] = q 3 2M .We are now in a position to proceed to calculate the fourth order cumulant for the system being initially in a coherent state. A. Calculations for the F ourth-order-cumulant

  2. [2]

    We now need to analytically obtain the time evolution of the ladder operators ˆa0 and ˆa†

    Coherent state The analytical expression for the fourth order cumu- lant is given in eq.(25) and the expression readsκ 4 = ⟨ˆq4⟩ −4⟨ˆq3⟩⟨ˆq⟩ −3⟨ˆq2⟩2 + 12⟨ˆq2⟩⟨ˆq⟩2 −6⟨ˆq⟩4 where the quadrature reads ˆq= 1√ 2 ˆae−iθ + ˆa†eiθ . We now need to analytically obtain the time evolution of the ladder operators ˆa0 and ˆa†

  3. [3]

    The total quantum gravitational Hamiltonian for a single mode Bose-Einstein condensate without any electromagnetic interactions read : ˆH:= : [ ˆH0 + ˆH QG int ] :=ℏωˆa† 0ˆa0 +λ N ˆa†2 0 ˆa2 0 +λ P Nˆa†3 0 ˆa3 0 . (30) As we are considering condensate system, we assume that the total number of particles is very large and constant in time and as a result t...

  4. [4]

    Derivation of the normal ordered exponential expression Any function of the number operator ˆNcan be expressed as f( ˆN) = ∞X l=0 f (l)(0) l! ˆN l (35) wheref (l)(0) denotes thel-th order derivative of the func- tion at the saddle point. It is possible to again express the normal ordering operator and its higher powers in a compact summation notation as ˆ...

  5. [5]

    Loop Quantum Gravity

    C. Rovelli, “Loop Quantum Gravity”, Living Rev. Rela- tiv. 1 (1998) 1

  6. [6]

    Quantum gravity: a progress report

    S. Carlip, “Quantum gravity: a progress report”, Rep. Prog. Phys. 64 (2001) 885

  7. [7]

    Noncommutative geometry

    A. Connes, “Noncommutative geometry”, Academic Press (1994), California

  8. [8]

    Deformed special relativity as an effective flat limit of quantum gravity

    F. Girelli, E. R. Livine, and D. Oriti, “Deformed special relativity as an effective flat limit of quantum gravity”, Nucl. Phys. B 708 (2005) 411

Show all 29 references
  1. [9]

    Volume 1: An Introduction to the Bosonic String,STRING THEORY

    J. Polchinski, “Volume 1: An Introduction to the Bosonic String,STRING THEORY”, Cambridge Uni- versity Press (1998), Cambridge

  2. [10]

    Volume 2: Superstring Theory and Be- yond, STRING THEORY

    J. Polchinski, “Volume 2: Superstring Theory and Be- yond, STRING THEORY”, Cambridge University Press (1998), Cambridge

  3. [11]

    Spin Entanglement Witness for Quan- tum Gravity

    S. Bose, A. Mazumdar, G. W. Morley, H. Ulbricht, M. Toroˇ s, M. Paternostro, A. Geraci, P. Barker, M. S. Kim, and G. Milburn, “Spin Entanglement Witness for Quan- tum Gravity”, Phys. Rev. Lett. 119 (2017) 240401

  4. [12]

    Local- ity and entanglement in table-top testing of the quantum nature of linearized gravity

    R. J. Marshman, A. Mazumdar, and S. Bose, “Local- ity and entanglement in table-top testing of the quantum nature of linearized gravity”, Phys. Rev. A 101 (2020) 052110

  5. [13]

    Gravitationally Induced En- tanglement between Two Massive Particles is Sufficient Evidence of Quantum Effects in Gravity

    C. Marletto and V. Vedral, “Gravitationally Induced En- tanglement between Two Massive Particles is Sufficient Evidence of Quantum Effects in Gravity”, Phys. Rev. Lett. 119 (2017) 240402

  6. [15]

    Signatures of the quantization of gravity at gravitational wave detec- tors

    M. Parikh, F. Wilczek, and G. Zahariade, “Signatures of the quantization of gravity at gravitational wave detec- tors”, Phys. Rev. D 104 (2021) 046021

  7. [16]

    Quantum mechanics of gravitational waves

    M. Parikh, F. Wilczek, and G. Zahariade, “Quantum mechanics of gravitational waves”, Phys. Rev. Lett. 127 (2021) 081602

  8. [17]

    Noise and deco- herence induced by gravitons

    S. Kanno, J. Soda, and J. Tokuda, “Noise and deco- herence induced by gravitons”, Phys. Rev. D 103 (2021) 10 044017

  9. [18]

    Indirect detection of gravitons through quantum entanglement

    S. Kanno, J. Soda, and J. Tokuda, “Indirect detection of gravitons through quantum entanglement”, Phys. Rev. D 104 (2021) 083516

  10. [19]

    Probing the quantum na- ture of gravity using a Bose-Einstein condensate

    S. Sen and S. Gangopadhyay, “Probing the quantum na- ture of gravity using a Bose-Einstein condensate”, Phys. Rev. D 110 (2024) 026014

  11. [20]

    Quantum nature of gravity in a Bose-Einstein condensate

    S. Sen and S. Gangopadhyay, “Quantum nature of gravity in a Bose-Einstein condensate”, Phys. Rev. D 111 (2025) 066002

  12. [21]

    Non-Gaussianity as a Signature of a Quantum Theory of Gravity

    R. Howl, V. Vedral, D. Naik, M. Christodoulou, C. Rov- elli, and A. Iyer, “Non-Gaussianity as a Signature of a Quantum Theory of Gravity”, Phys. Rev. X Quantum 2 (2021) 010325

  13. [22]

    Quan- tum gravity signatures in gravitational wave detectors placed inside a harmonic trap potential

    S. Sen, S. Bhattacharyya, and S. Gangopadhyay, “Quan- tum gravity signatures in gravitational wave detectors placed inside a harmonic trap potential”, Phys. Rev. D 110 (2024) 026008

  14. [23]

    Is a graviton detectable?

    F. Dyson, “Is a graviton detectable?”, Int. J. Mod. Phys. A 28 (2013) 1330041

  15. [24]

    On the possibility of laboratory evidence for quantum superposition of geome- tries

    M. Christodoulou and C. Rovelli, “On the possibility of laboratory evidence for quantum superposition of geome- tries”, Phys. Lett. B 792 (2019) 64

  16. [25]

    Is Gravity Quantum?

    M. Bahrami, A. Bassi, S. McMillen, M. Paternostro, and H. Ulbricht, “Is Gravity Quantum?”, arXiv:1507.05733 [quant-ph]

  17. [26]

    Gravity in the quantum lab

    R. Howl, L. Hackerm¨ uller, D. E. Bruschi, and I. Fuentes, “Gravity in the quantum lab”, Adv. Phys.: X 3 (2018) 1383184

  18. [27]

    Gravitation and Cosmology; Principles and Applications of the General Theory of Relativity

    S. Weinberg, “Gravitation and Cosmology; Principles and Applications of the General Theory of Relativity”, Wiley (1972)

  19. [28]

    Bose-Einstein Condensa- tion and Superfluidity

    L. Pitaevski and S. Stingari, “Bose-Einstein Condensa- tion and Superfluidity”, (Oxford University Press, Ox- ford, 2016)

  20. [29]

    The Advanced Theory of Statistics

    M. G. Kendall and A. Stuart, “The Advanced Theory of Statistics” (Charles Griffin, London, 1958), Vol.1

  21. [30]

    Non-Gaussian continuous-variable entanglement and steering

    M. K. Olsen and J. F. Corney, “Non-Gaussian continuous-variable entanglement and steering”, Phys. Rev. A 87 (2013) 033839

Pith tools

Reviewed June 27, 2026 · model on record in the stance chip above.