pith. sign in

arxiv: 2606.26372 · v1 · pith:EWQU7XZYnew · submitted 2026-06-24 · 🌀 gr-qc · hep-th

Effect of the magnetic monopole charge on Dirac entanglement and Bell non-locality in Hayward spacetime

Pith reviewed 2026-06-26 01:09 UTC · model grok-4.3

classification 🌀 gr-qc hep-th
keywords Hawking radiationDirac fieldsquantum entanglementBell nonlocalityHayward black holeregular black holesfermionic correlationsPauli exclusion
0
0 comments X

The pith

Dirac field entanglement in Hayward spacetime stays nonzero at infinite Hawking temperature due to the Pauli principle.

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

The paper studies how Hawking radiation degrades an entangled Dirac state shared by an inertial observer and one near the horizon of a Hayward regular black hole. It finds that fermionic correlations never reach zero even as temperature becomes infinite, because the exclusion principle blocks complete degradation, while some entanglement shifts to inaccessible interior modes. Accessible modes continue to violate Bell inequalities at any finite temperature, but interior modes never do. The regularity parameter g enters the results only by lowering the Hawking temperature, which in turn slows the loss of quantum information. This establishes a direct link between the resolution of the central singularity and the survival of fermionic quantum correlations.

Core claim

Using the Wootters concurrence and the CHSH Bell parameter on the entangled Dirac state, the calculation shows that accessible modes exhibit Bell nonlocality for every finite Hawking temperature while interior modes never violate the inequality. Fermionic correlations remain nonzero in the infinite-temperature limit owing to the Pauli exclusion principle, with part of the entanglement redistributed to inaccessible modes inside the horizon. The Hayward regularity parameter g affects the correlations only through the Hawking temperature, whose decrease with increasing g enhances preservation of quantum information.

What carries the argument

Wootters concurrence and CHSH Bell parameter applied to the Dirac entangled state, with the Hayward regularity parameter g entering exclusively through its effect on the Hawking temperature.

If this is right

  • Accessible modes violate Bell's inequality at all finite Hawking temperatures.
  • Interior modes never violate Bell's inequality.
  • Fermionic correlations remain nonzero at infinite temperature, unlike the bosonic case.
  • Increasing the Hayward parameter g lowers the Hawking temperature and thereby slows the loss of quantum correlations.
  • Singularity resolution in regular black holes is tied to greater robustness of fermionic quantum information.

Where Pith is reading between the lines

These are editorial extensions of the paper, not claims the author makes directly.

  • The temperature-only dependence may hold for other regular black-hole metrics whose surface gravity depends on a similar regularity parameter.
  • Analog condensed-matter systems with tunable effective temperatures could test whether fermionic entanglement persists at high temperature.
  • Quantum communication protocols near black holes could exploit regularity parameters to maintain correlations longer than in singular spacetimes.

Load-bearing premise

The standard Hawking temperature formula for the Hayward metric fully captures the effect on the chosen entangled Dirac state, with no additional back-reaction or mode-mixing terms required.

What would settle it

An explicit calculation of the concurrence or CHSH value that shows dependence on the Hayward parameter g at fixed Hawking temperature would falsify the claim that g acts only through temperature.

Figures

Figures reproduced from arXiv: 2606.26372 by Abdessamie Chhieb, Mohamed Ouchrif.

Figure 1
Figure 1. Figure 1: FIG. 1: Schematic representation of the physical setup. Alice, with qubit [PITH_FULL_IMAGE:figures/full_fig_p004_1.png] view at source ↗
Figure 2
Figure 2. Figure 2: FIG. 2: Concurrences [PITH_FULL_IMAGE:figures/full_fig_p007_2.png] view at source ↗
Figure 3
Figure 3. Figure 3: FIG. 3: Same quantities as in Fig [PITH_FULL_IMAGE:figures/full_fig_p009_3.png] view at source ↗
Figure 4
Figure 4. Figure 4: FIG. 4: Concurrences and CHSH parameters as functions of [PITH_FULL_IMAGE:figures/full_fig_p010_4.png] view at source ↗
Figure 5
Figure 5. Figure 5: FIG. 5: Concurrences and CHSH parameters as functions of [PITH_FULL_IMAGE:figures/full_fig_p011_5.png] view at source ↗
Figure 6
Figure 6. Figure 6: FIG. 6: Comparison of fermionic (Dirac, solid black) and bosonic (scalar, dashed red) concurrences. (a) Accessible [PITH_FULL_IMAGE:figures/full_fig_p012_6.png] view at source ↗
read the original abstract

We investigate bipartite quantum correlations of Dirac fields in the spacetime of a Hayward regular black hole. Using the Wootters concurrence and the CHSH Bell parameter, we analyze the influence of Hawking radiation on an entangled state shared by an inertial observer and a near-horizon observer. We show that, unlike the bosonic case, fermionic correlations remain nonzero even in the infinite-temperature limit owing to the Pauli exclusion principle, while part of the entanglement is redistributed to inaccessible modes inside the horizon. The accessible modes exhibit Bell nonlocality for all finite Hawking temperatures, whereas the interior modes never violate Bell's inequality. The Hayward regularity parameter $g$ affects the correlations only through the Hawking temperature, whose decrease with increasing $g$ enhances the preservation of quantum information. These results suggest a close connection between singularity resolution and the robustness of fermionic quantum correlations in regular black-hole spacetimes.

Editorial analysis

A structured set of objections, weighed in public.

Desk editor's note, referee report, simulated authors' rebuttal, and a circularity audit. Tearing a paper down is the easy half of reading it; the pith above is the substance, this is the friction.

Referee Report

0 major / 3 minor

Summary. The manuscript investigates bipartite quantum correlations of Dirac fields in the Hayward regular black hole spacetime. It considers an initially entangled Dirac state shared between an inertial observer and a near-horizon observer, applies the Wootters concurrence and CHSH Bell parameter after tracing over inaccessible modes, and examines the effects of Hawking radiation. The central claims are that fermionic correlations remain nonzero in the infinite-temperature limit due to the Pauli exclusion principle (with part of the entanglement redistributed to interior modes), that accessible exterior modes exhibit Bell nonlocality for all finite Hawking temperatures while interior modes never violate the CHSH inequality, and that the regularity parameter g influences all results exclusively through the Hawking temperature (whose decrease with increasing g improves correlation preservation).

Significance. If the results hold, the work establishes a concrete connection between singularity resolution in regular black holes and the robustness of fermionic quantum information against Hawking radiation. It shows explicitly how the Pauli principle protects fermionic correlations at high temperatures in a manner absent for bosons, and demonstrates that the Hayward parameter g enters the final expressions only via the surface gravity at the outer horizon. The calculation follows the standard Bogoliubov transformation between Boulware and Hartle-Hawking modes for Dirac fields in a static spherically symmetric metric, yielding parameter-free predictions once the metric is fixed.

minor comments (3)
  1. [§3] §3 (or the section presenting the mode expansion): the explicit form of the Bogoliubov coefficients for the Dirac field in the Hayward metric should be written out, even if they reduce to the standard Fermi-Dirac factor; this would make the claim that g enters solely through T fully transparent.
  2. [Figures in §4/5] Figure captions (likely in §4 or §5): the range of g values and corresponding Hawking temperatures used in the plots should be stated explicitly, together with the precise definition of the initial entangled state (including any normalization constants).
  3. [Abstract and §5] The abstract states that interior modes 'never violate Bell's inequality'; the corresponding CHSH value should be shown to remain below 2 for all T, perhaps with a short analytic argument in addition to numerics.

Simulated Author's Rebuttal

0 responses · 0 unresolved

We thank the referee for the careful reading and positive recommendation of minor revision. The provided summary accurately captures the scope, methods, and central claims of the manuscript.

Circularity Check

0 steps flagged

No significant circularity; derivation is self-contained standard QFT calculation

full rationale

The paper computes Dirac field correlations via standard Bogoliubov transformations between Boulware and Hartle-Hawking modes in the Hayward metric. The Hawking temperature T = κ/2π is obtained directly from the surface gravity at the outer horizon (with g entering the metric and thus κ in the usual way), and all reported quantities (concurrence, CHSH) are explicit functions of this T and the fermionic mode structure. No parameters are fitted to data and then relabeled as predictions; no uniqueness theorems or ansatzes are imported via self-citation; the Pauli-exclusion and interior/exterior redistribution results follow algebraically from the two-mode fermionic vacuum without reducing to the input state by construction. The central claims are therefore independent of the paper's own fitted values or prior self-referential results.

Axiom & Free-Parameter Ledger

0 free parameters · 2 axioms · 0 invented entities

Based on abstract only; standard assumptions of quantum field theory in curved spacetime are used but not enumerated.

axioms (2)
  • domain assumption Hawking temperature is obtained from the surface gravity of the Hayward metric in the usual semiclassical way.
    Abstract states that g affects correlations only through this temperature.
  • domain assumption The initial state is a standard entangled Dirac pair with one observer inertial and one near the horizon.
    Central to the bipartite correlation calculation described.

pith-pipeline@v0.9.1-grok · 5683 in / 1451 out tokens · 25239 ms · 2026-06-26T01:09:01.039336+00:00 · methodology

discussion (0)

Sign in with ORCID, Apple, or X to comment. Anyone can read and Pith papers without signing in.

Reference graph

Works this paper leans on

44 extracted references

  1. [1]

    4 below, in line with the dilatonic [37] and the RN [12] analyses

    These two analytical limits explain quantitatively both the low-frequency plateau and the high-frequency enhancement that will be seen in Fig. 4 below, in line with the dilatonic [37] and the RN [12] analyses. Fermionic lower bound.The plateau value sin(2α)/ √ 2 is the universal lower bound of the accessible fermionic concurrence in the present setting: C...

  2. [2]

    For an X-state with real off-diagonals, T11 = 2(ϱ14 +ϱ 23), T22 = 2(ϱ23 −ϱ 14),(29) T33 =ϱ 11 −ϱ 22 −ϱ 33 +ϱ 44

    For a generic two-qubit stateϱ, the Horodecki criterion gives Bmax(ϱ) = 2 p M(ϱ), M(ϱ) =t 2 i +t 2 j ,(28) wheret 2 i , t2 j are the two largest ofT 2 11, T2 22, T2 33, andT ii = tr[ϱ σi⊗σi] are the diagonal components of the correlation tensor. For an X-state with real off-diagonals, T11 = 2(ϱ14 +ϱ 23), T22 = 2(ϱ23 −ϱ 14),(29) T33 =ϱ 11 −ϱ 22 −ϱ 33 +ϱ 44...

  3. [3]

    Stephen W. Hawking. Particle creation by black holes. Communications in Mathematical Physics, 43(3):199– 220, 1975

  4. [4]

    Stephen W. Hawking. Breakdown of predictability in gravitational collapse.Physical Review D, 14(10):2460– 2473, 1976

  5. [5]

    Alsing and G

    Paul M. Alsing and G. J. Milburn. Teleportation with a uniformly accelerated partner.Physical Review Letters, 91(18):180404, 2003

  6. [6]

    Ivette Fuentes-Schuller and Robert B. Mann. Alice falls into a black hole: Entanglement in noninertial frames. Physical Review Letters, 95(12):120404, 2005

  7. [7]

    Entanglement of dirac fields in noninertial frames

    Gerardo Adesso, Ivette Fuentes-Schuller, and Marie Eric- sson. Entanglement of dirac fields in noninertial frames. Physical Review A, 76(6):062112, 2007

  8. [8]

    Projective measurements and generation of entangled Dirac par- ticles in Schwarzschild spacetime.Annals of Physics, 325(6):1190–1197, 2010

    Jieci Wang, Qiyuan Pan, and Jiliang Jing. Projective measurements and generation of entangled Dirac par- ticles in Schwarzschild spacetime.Annals of Physics, 325(6):1190–1197, 2010

  9. [9]

    Prob- ing the quantum correlation and Bell non-locality for Dirac particles with Hawking effect in the background of Schwarzschild black hole.Physics Letters B, 733:1–5, 2014

    Shuai Xu, Xue-ke Song, Jia-dong Shi, and Liu Ye. Prob- ing the quantum correlation and Bell non-locality for Dirac particles with Hawking effect in the background of Schwarzschild black hole.Physics Letters B, 733:1–5, 2014

  10. [10]

    How the Hawking effect affects multipartite entanglement of Dirac particles in the background of a Schwarzschild black hole.Physical Review D, 89(6):065022, 2014

    Shuai Xu, Xue-ke Song, Jia-dong Shi, and Liu Ye. How the Hawking effect affects multipartite entanglement of Dirac particles in the background of a Schwarzschild black hole.Physical Review D, 89(6):065022, 2014

  11. [11]

    Property of various correlation measures of open Dirac system with Hawking effect in Schwarzschild space-time.Physics Let- ters B, 740:322–328, 2015

    Juan He, Shuai Xu, Yang Yu, and Liu Ye. Property of various correlation measures of open Dirac system with Hawking effect in Schwarzschild space-time.Physics Let- ters B, 740:322–328, 2015

  12. [12]

    Measurement-induced- nonlocality for Dirac particles in Garfinkle–Horowitz– Strominger dilation space-time.Physics Letters B, 756:278–282, 2016

    Juan He, Shuai Xu, and Liu Ye. Measurement-induced- nonlocality for Dirac particles in Garfinkle–Horowitz– Strominger dilation space-time.Physics Letters B, 756:278–282, 2016

  13. [13]

    Quantum entanglement of bosonic fields beyond the single-mode approxima- tion in schwarzschild spacetime.Physical Review A, 82(3):032324, 2010

    Jieci Wang and Jiliang Jing. Quantum entanglement of bosonic fields beyond the single-mode approxima- tion in schwarzschild spacetime.Physical Review A, 82(3):032324, 2010

  14. [14]

    Quantum entangle- ment in the Dirac field quantization around charged black holes.Physics Letters B, page 140629, 2026

    Abdessamie Chhieb, Chaimae Banouni, Saliha Ab- dessamie, and Mohamed Ouchrif. Quantum entangle- ment in the Dirac field quantization around charged black holes.Physics Letters B, page 140629, 2026

  15. [15]

    Sean A. Hayward. Formation and evaporation of nonsin- gular black holes.Physical Review Letters, 96(3):031103, 2006

  16. [16]

    J. M. Bardeen. Non-singular general relativistic gravita- tional collapse. InProceedings of the International Con- ference GR5, Tbilisi, USSR, page 174, 1968

  17. [17]

    Vacuum nonsingular black hole.Gen- eral Relativity and Gravitation, 24(3):235–242, 1992

    Irina Dymnikova. Vacuum nonsingular black hole.Gen- eral Relativity and Gravitation, 24(3):235–242, 1992

  18. [18]

    Regular black hole in general relativity coupled to nonlinear electrodynam- ics.Physical Review Letters, 80(23):5056–5059, 1998

    Eloy Ay´ on-Beato and Alberto Garc´ ıa. Regular black hole in general relativity coupled to nonlinear electrodynam- ics.Physical Review Letters, 80(23):5056–5059, 1998

  19. [19]

    Valeri P. Frolov. Information loss problem and a ‘black hole’ model with a closed apparent horizon.Journal of High Energy Physics, 2014(5):49, 2014

  20. [20]

    Phenomenological aspects of black holes beyond general relativity.Physical Review D, 98(12):124009, 2018

    Raul Carballo-Rubio, Francesco Di Filippo, Stefano Liberati, and Matt Visser. Phenomenological aspects of black holes beyond general relativity.Physical Review D, 98(12):124009, 2018

  21. [21]

    Inner hori- zon instability and the unstable cores of regular black holes.Journal of High Energy Physics, 2022(05):132, 2022

    Raul Carballo-Rubio, Francesco Di Filippo, Stefano Liberati, Costantino Pacilio, and Matt Visser. Inner hori- zon instability and the unstable cores of regular black holes.Journal of High Energy Physics, 2022(05):132, 2022

  22. [22]

    Wootters

    William K. Wootters. Entanglement of formation of an arbitrary state of two qubits.Physical Review Letters, 80(10):2245–2248, 1998

  23. [23]

    Clauser, Michael A

    John F. Clauser, Michael A. Horne, Abner Shimony, and Richard A. Holt. Proposed experiment to test lo- cal hidden-variable theories.Physical Review Letters, 14 23(15):880–884, 1969

  24. [24]

    Horodecki, P

    R. Horodecki, P. Horodecki, and M. Horodecki. Violating Bell inequality by mixed spin- 1 2 states: Necessary and sufficient condition.Physics Letters A, 200(5):340–344, 1995

  25. [25]

    Damour and R

    T. Damour and R. Ruffini. Black-hole evaporation in the Klein–Sauter–Heisenberg–Euler formalism.Physical Review D, 14(2):332–334, 1976

  26. [26]

    Hawking radiation of the Dirac field via an anomalous method.Physical Review D, 70(6):065004, 2004

    Jiliang Jing. Hawking radiation of the Dirac field via an anomalous method.Physical Review D, 70(6):065004, 2004

  27. [27]

    Unruh effect in quantum information beyond the single-mode approximation.Physical Review A, 82(4):042332, 2010

    David Edward Bruschi, Jorma Louko, Eduardo Mart´ ın- Mart´ ınez, Andrzej Dragan, and Ivette Fuentes. Unruh effect in quantum information beyond the single-mode approximation.Physical Review A, 82(4):042332, 2010

  28. [28]

    Entangle- ment in noninertial frames: Foundational issues.Physical Review A, 81(3):032320, 2010

    Eduardo Mart´ ın-Mart´ ınez and Ivette Fuentes. Entangle- ment in noninertial frames: Foundational issues.Physical Review A, 81(3):032320, 2010

  29. [29]

    Brill and John A

    Dieter R. Brill and John A. Wheeler. Interaction of neutrinos and gravitational fields.Reviews of Modern Physics, 29(3):465–479, 1957

  30. [30]

    William G. Unruh. Notes on black hole evaporation. Physical Review D, 14(4):870–892, 1976

  31. [31]

    Thermo-field dynamics of black holes

    Werner Israel. Thermo-field dynamics of black holes. Physics Letters A, 57(2):107–110, 1976

  32. [32]

    Hartle and Stephen W

    James B. Hartle and Stephen W. Hawking. Path-integral derivation of black-hole radiance.Physical Review D, 13(8):2188–2203, 1976

  33. [33]

    N. D. Birrell and P. C. W. Davies.Quantum Fields in Curved Space. Cambridge University Press, 1984

  34. [34]

    Alsing, Ivette Fuentes-Schuller, Robert B

    Paul M. Alsing, Ivette Fuentes-Schuller, Robert B. Mann, and Tracey E. Tessier. Entanglement of Dirac fields in non-inertial frames.Physical Review A, 74(3):032326, 2006

  35. [35]

    Fermionic en- tanglement that survives a black hole.Physical Review A, 80(4):042318, 2009

    Eduardo Mart´ ın-Mart´ ınez and Juan Le´ on. Fermionic en- tanglement that survives a black hole.Physical Review A, 80(4):042318, 2009

  36. [36]

    Progress of Theoret- ical Physics Supplement, 1986

    Shin Takagi.Vacuum noise and stress induced by uniform acceleration: Hawking–Unruh effect in Rindler manifold of arbitrary dimension, volume 88. Progress of Theoret- ical Physics Supplement, 1986

  37. [37]

    S. M. Hashemi Rafsanjani, M. Huber, C. J. Broadbent, and J. H. Eberly. Genuinely multipartite concurrence of N-qubitX-matrices.Physical Review A, 86(6):062303, 2012

  38. [38]

    Pan and J

    Q. Pan and J. Jing. Hawking radiation of Dirac particles via tunneling from the Reissner–Nordstr¨ om black hole. Modern Physics Letters A, 23(1):25–34, 2008

  39. [39]

    Entangle- ment in non-inertial frames: degradation and survival

    Eduardo Mart´ ın-Mart´ ınez and Ivette Fuentes. Entangle- ment in non-inertial frames: degradation and survival. Physical Review A, 83(5):052306, 2011

  40. [40]

    B. S. Cirel’son. Quantum generalizations of Bell’s in- equality.Letters in Mathematical Physics, 4(2):93–100, 1980

  41. [41]

    Mann and Timothy C

    Robert B. Mann and Timothy C. Ralph. Relativistic quantum information.Classical and Quantum Gravity, 29(22):220301, 2012

  42. [42]

    Relativistic quan- tum metrology: Exploiting relativity to improve quan- tum measurement technologies.Scientific Reports, 4:4996, 2014

    Mehdi Ahmadi, David Edward Bruschi, Carlos Sab´ ın, Gerardo Adesso, and Ivette Fuentes. Relativistic quan- tum metrology: Exploiting relativity to improve quan- tum measurement technologies.Scientific Reports, 4:4996, 2014

  43. [43]

    Asher Peres and Daniel R. Terno. Quantum informa- tion and relativity theory.Reviews of Modern Physics, 76(1):93–123, 2004

  44. [44]

    States, effects, and operations: Fundamental notions of quantum theory.Lecture Notes in Physics, 190, 1983

    Karl Kraus. States, effects, and operations: Fundamental notions of quantum theory.Lecture Notes in Physics, 190, 1983