Recognition: unknown
Decrease of the entanglement entropy of the Hawking radiation induced by backreaction in the Bose-Einstein condensate
Pith reviewed 2026-05-10 11:03 UTC · model grok-4.3
The pith
Backreaction from analog Hawking radiation decreases its entanglement entropy in a Bose-Einstein condensate.
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
By deriving an explicit form of backreaction from the microscopic theory of the Bose-Einstein condensate in a step-like configuration and combining it with known Bogoliubov coefficients, the entanglement entropy of the analog Hawking radiation is computed and shown to decrease as expected due to the backreaction for sufficiently low energy modes over a wide range of the characterizing parameter.
What carries the argument
The backreaction term derived from the microscopic BEC Hamiltonian in the step-like configuration, combined with Bogoliubov coefficients to modify and compute the entanglement entropy of the Hawking radiation.
If this is right
- The entanglement entropy of the Hawking radiation decreases due to the inclusion of backreaction.
- This decrease occurs specifically for sufficiently low energy modes.
- The decrease holds over a wide range of the parameter describing the step-like configuration.
- The microscopic unitary theory of the BEC allows explicit reproduction of Page-curve-like behavior in the analog system.
Where Pith is reading between the lines
- This approach may allow similar analytic entropy calculations in other analog gravity setups that possess microscopic Hamiltonians.
- Experimental measurements of entanglement in BEC systems could directly test the predicted entropy decrease.
- The result suggests that backreaction effects can be tracked mode-by-mode to connect analog models with black hole unitarity.
Load-bearing premise
The backreaction derived from the microscopic theory can be combined directly with the Bogoliubov coefficients without higher-order corrections or breakdown of the approximations for the low-energy modes and parameter ranges considered.
What would settle it
A computation or BEC experiment that includes the backreaction and finds the entanglement entropy does not decrease (or increases) for the low-energy modes in the step-like configuration.
Figures
read the original abstract
We analytically study the effect of backreaction from analog Hawking radiation on its entanglement entropy in the Bose-Einstein condensate (BEC). The backreaction is expected to play an essential role in the decrease of the entanglement entropy and in realizing the Page curve. Since the BEC theory has microscopic Hamiltonian and thus exhibits unitarity, it is desirable to reproduce the Page curve explicitly by using the Hamiltonian. In order to analyze this in a concrete example, we study the BEC with a step-like configuration that has been extensively studied in the literature. By using the microscopic theory, we derive an explicit form of backreaction from analog Hawking radiation. Combining it with the known results of the Bogoliubov coefficients, we analytically compute the entanglement entropy of the Hawking radiation, and show that it decreases as expected due to the backreaction for sufficiently low energy modes over a wide range of the parameter characterizing the step-like configuration.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The manuscript analytically derives an explicit backreaction term from the microscopic Hamiltonian of a Bose-Einstein condensate with a step-like flow configuration. It combines this term with known analytic Bogoliubov coefficients for the unperturbed case to compute the entanglement entropy of the analog Hawking radiation, claiming an explicit decrease for sufficiently low-energy modes over a wide range of the step-like parameter.
Significance. If the central combination holds without uncontrolled corrections, the result supplies a concrete, Hamiltonian-based demonstration that backreaction reduces Hawking entanglement entropy in a unitary analog system, advancing explicit realizations of Page-curve behavior in analog gravity. The microscopic starting point and analytic control are strengths that distinguish it from purely effective-field treatments.
major comments (1)
- [The section combining the backreaction term with the Bogoliubov coefficients] The central claim rests on inserting the derived backreaction directly into the entanglement-entropy formula while retaining the pre-existing Bogoliubov coefficients. The manuscript must demonstrate quantitatively that the backreaction remains a small perturbation that does not appreciably shift the mode functions, effective horizon location, or the Bogoliubov transformation itself for the low-energy modes and parameter range considered; otherwise the analytic combination undercounts or overcounts the unitary evolution of the reduced density matrix.
minor comments (1)
- [Abstract and introduction] Clarify the precise definition of the step-like parameter and its range of validity in the abstract and introduction to aid readers unfamiliar with the prior literature on this configuration.
Simulated Author's Rebuttal
We thank the referee for the careful reading of our manuscript and the constructive feedback. We are pleased that the referee recognizes the potential significance of our Hamiltonian-based approach to analog Hawking radiation and the Page curve. We respond to the major comment below.
read point-by-point responses
-
Referee: The central claim rests on inserting the derived backreaction directly into the entanglement-entropy formula while retaining the pre-existing Bogoliubov coefficients. The manuscript must demonstrate quantitatively that the backreaction remains a small perturbation that does not appreciably shift the mode functions, effective horizon location, or the Bogoliubov transformation itself for the low-energy modes and parameter range considered; otherwise the analytic combination undercounts or overcounts the unitary evolution of the reduced density matrix.
Authors: We agree that a quantitative demonstration of the perturbative nature of the backreaction is necessary to justify retaining the unperturbed Bogoliubov coefficients. In the revised manuscript, we will include an additional analysis estimating the magnitude of the backreaction-induced corrections to the mode functions and the effective horizon position. For the low-energy modes and the parameter range of the step-like flow where the decrease in entanglement entropy is observed, these corrections are shown to be small, of order O( (Hawking flux / background energy density) ), which is much less than unity. This supports the validity of our analytic combination without uncontrolled corrections to the unitary evolution. revision: yes
Circularity Check
No significant circularity; derivation remains self-contained
full rationale
The paper first derives an explicit backreaction term directly from the microscopic BEC Hamiltonian for the step-like flow. This term is then inserted into the entanglement entropy expression that already employs the standard analytic Bogoliubov coefficients obtained from prior literature on the non-backreacted case. The observed decrease for low-energy modes is an explicit computational result of that insertion rather than a definitional identity, a fitted parameter renamed as a prediction, or a reduction to any self-citation chain. No equations are shown to be equivalent by construction, and the cited Bogoliubov coefficients are external, falsifiable results independent of the present backreaction derivation.
Axiom & Free-Parameter Ledger
axioms (2)
- domain assumption The BEC system is described by a microscopic Hamiltonian that is unitary.
- domain assumption The step-like density profile creates a valid analog black hole horizon whose radiation can be treated with Bogoliubov methods.
Reference graph
Works this paper leans on
-
[1]
Breakdown of Predictability in Gravitat ional Collapse,
S. W. Hawking, “Breakdown of Predictability in Gravitat ional Collapse,” Phys. Rev. D 14 (1976), 2460-2473
1976
-
[2]
A. Almheiri, T. Hartman, J. Maldacena, E. Shaghoulian an d A. Tajdini, “The entropy of Hawking radiation,” Rev. Mod. Phys. 93, no.3, 035002 (2021) [arXiv:2006.06872 [hep-th]]
-
[3]
Seeing Page Curves and Islands with Blinders On,
H. Geng, A. Karch, C. Perez-Pardavila, S. Raju, L. Randal l and M. Riojas, “Seeing Page Curves and Islands with Blinders On,” [arXiv:2602.06543 [h ep-th]]
-
[4]
Geng, SciPost Phys.19, no.6, 146 (2025) [arXiv:2312.13336 [hep-th]]
H. Geng, “Graviton mass and entanglement islands in low s pacetime dimensions,” SciPost Phys. 19, no.6, 146 (2025) [arXiv:2312.13336 [hep-th]]
-
[5]
Geng, (2025), arXiv:2502.08703 [hep-th]
H. Geng, “The mechanism behind the information encoding for islands,” JHEP 03, 037 (2026) [arXiv:2502.08703 [hep-th]]
-
[6]
Experimental black hole evaporation,
W. G. Unruh, “Experimental black hole evaporation,” Phy s. Rev. Lett. 46 (1981), 1351-1353
1981
-
[7]
J. Macher and R. Parentani, “Black/White hole radiation from dispersive theories,” Phys. Rev. D 79 (2009), 124008 [arXiv:0903.2224 [hep-th]]
-
[8]
Bogoliubov Theor y of acoustic Hawking radiation in Bose-Einstein Condensates,
A. Recati, N. Pavloff and I. Carusotto, “Bogoliubov Theor y of acoustic Hawking radiation in Bose-Einstein Condensates,” Phys. Rev. A 80 (2009), 043603 [arXiv:0907.4305 [cond- mat.quant-gas]]. 25
-
[9]
Average entropy of a subsystem,
D. N. Page, “Average entropy of a subsystem,” Phys. Rev. L ett. 71 (1993), 1291-1294 [arXiv:gr- qc/9305007 [gr-qc]]; D. N. Page, “Information in black hole radiation,” Phys. Rev . Lett. 71 (1993), 3743-3746 [arXiv:hep-th/9306083 [hep-th]]
-
[10]
Quan tum back-reaction in dilute Bose-Einstein condensates,
R. Schutzhold, M. Uhlmann, Y. Xu and U. R. Fischer, “Quan tum back-reaction in dilute Bose-Einstein condensates,” Phys. Rev. D 72, 105005 (2005) [arXiv:cond-mat/0503581 [cond- mat.other]]
-
[11]
U. R. Fischer, “Dynamical aspects of analogue gravity: The Backreaction of quantum fluctua- tions in dilute Bose-Einstein condensates,” Lect. Notes Ph ys. 718, 93-113 (2007) [arXiv:cond- mat/0512537 [cond-mat.other]]
-
[12]
The infor mation loss problem: an analogue gravity perspective,
S. Liberati, G. Tricella and A. Trombettoni, “The infor mation loss problem: an analogue gravity perspective,” Entropy 21, no.10, 940 (2019) [arXiv:1908.01036 [gr-qc]]
-
[13]
Backreaction in an analogue black hole experiment,
S. Patrick, H. Goodhew, C. Gooding and S. Weinfurtner, “ Backreaction in an analogue black hole experiment,” Phys. Rev. Lett. 126, no.4, 041105 (2021) [arXiv:1905.03045 [gr-qc]]
-
[14]
Back-rea ction in canonical analogue black holes,
S. Liberati, G. Tricella and A. Trombettoni, “Back-rea ction in canonical analogue black holes,” Appl. Sciences 10 (2020) no.24, 8868 [arXiv:2010.09966 [gr-qc]]
-
[15]
Low frequency analogue Hawking radiation: The Bogoliubov- de Gennes model,
A. Coutant and S. Weinfurtner, “Low frequency analogue Hawking radiation: The Bogoliubov- de Gennes model,” Phys. Rev. D 97 (2018) no.2, 025006 [arXiv:1707.09664 [gr-qc]]
-
[16]
Tripartite Entanglement of Hawk ing Radiation in Dispersive Model,
Y. Nambu and Y. Osawa, “Tripartite Entanglement of Hawk ing Radiation in Dispersive Model,” Phys. Rev. D 103 (2021), 125007 [arXiv:2101.11764 [gr-qc]]
-
[17]
Finite-Temper ature Models of Bose-Einstein Conden- sation
Proukakis, Nick P., and Brian Jackson. “Finite-Temper ature Models of Bose-Einstein Conden- sation.” Journal of Physics B: Atomic, Molecular and Optica l Physics, vol. 41, no. 20, Oct. 2008, p. 203002
2008
-
[18]
Quantum nonlinear effects in the number-conserving analog gravity of Bose-Einstein condensates,
K. Pal and U. R. Fischer, “Quantum nonlinear effects in the number-conserving analog gravity of Bose-Einstein condensates,” Phys. Rev. D 110, no.11, 116022 (2024) [arXiv:2410.13596 [gr- qc]]
-
[19]
Spacetime analogue of Bose-Einstein condensates: Bogoliubov-de Gennes formu lation,
Y. Kurita, M. Kobayashi, T. Morinari, M. Tsubota and H. I shihara, “Spacetime analogue of Bose-Einstein condensates: Bogoliubov-de Gennes formu lation,” Phys. Rev. A 79 (2009), 043616 [arXiv:0810.3088 [cond-mat.other]]
-
[20]
J. Macher and R. Parentani, “Black hole radiation in Bos e-Einstein condensates,” Phys. Rev. A 80 (2009), 043601 [arXiv:0905.3634 [cond-mat.quant-gas]]
-
[21]
A. Fabbri and C. Mayoral, “Step-like discontinuities i n Bose-Einstein condensates and Hawking radiation: the hydrodynamic limit,” Phys. Rev. D 83 (2011), 124016 [arXiv:1004.4876 [gr-qc]]
-
[22]
Step-like discon tinuities in Bose-Einstein condensates and Hawking radiation: dispersion effects,
C. Mayoral, A. Fabbri and M. Rinaldi, “Step-like discon tinuities in Bose-Einstein condensates and Hawking radiation: dispersion effects,” Phys. Rev. D 83 (2011), 124047[arXiv:1008.2125 [gr-qc]]. 26
-
[23]
Evanescent Mod es and Step-like Acoustic Black Holes,
J. B. Curtis, G. Refael and V. Galitski, “Evanescent Mod es and Step-like Acoustic Black Holes,” Annals Phys. 407 (2019), 148-165 [arXiv:1801.01607 [cond-mat.quant-gas] ]
-
[24]
Particle creation and entanglem ent in a dispersive model with step velocity profile,
Y. Osawa and Y. Nambu, “Particle creation and entanglem ent in a dispersive model with step velocity profile,” Phys. Rev. D 107 (2023) no.10, 105005 [arXiv:2204.08684 [gr-qc]]. 27
discussion (0)
Sign in with ORCID, Apple, or X to comment. Anyone can read and Pith papers without signing in.