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Condensation of area quanta ensembles with quantum statistics in Schwarzschild spacetimes

Ryley McGovern, Seth Major*, Trevor Scheuing, and Thomas Takis

  • *Contact author: smajor@hamilton.edu

Phys. Rev. D 113, 046021 – Published 26 February, 2026

DOI: https://doi.org/10.1103/tkl8-lfmf

Abstract

Near-horizon (equivalently high acceleration) observers in spherically symmetric black hole spacetimes have a particularly simple form of the quasilocal energy. Using this energy and indistinguishable area quanta satisfying quantum statistics, a statistical mechanical description of the Schwarzschild black hole geometry for uniformly accelerating observers is developed. The resulting model has several phases including one with highly excited states, Bose-Einstein condensates, condensates distinct from the usual Bose gas, and degenerate Fermi gases. In the large area limit, relevant for comparison to the Bekenstein-Hawking entropy, the new condensed state is favored over Bose-Einstein condensation and the degenerate Fermi gas. The entropies of the phases, and the entropy of mixing, are computed. The resulting low-entropic condensed state, in which the quanta are essentially all in the lowest Bose energy state, provides the framework for the quantization of near-horizon geometric fluctuations, which is explored in S. Major et al. [arXiv:2601.08794].

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References (48)

  1. J. Bekenstein, Phys. Rev. D 7, 2333 (1973).
  2. R. D. Sorkin, in Tenth International Conference on General Relativity and Gravitation, edited by B. Bertotti, F. de Felice, and A. Pascolini (Consiglio Nazionale Delle Ricerche, Italy, 1983), Vol. 2, p. 734.
  3. L. Bombelli, R. K. Koul, J. H. Lee, and R. D. Sorkin, Phys. Rev. D 34, 373 (1986).
  4. A. Strominger and C. Vafa, Phys. Lett. B 379, 99 (1996).
  5. An observable signature associated to these fluctuations is explored in [6].

  6. S. Major, D. Rodriguez, and T. Takis, arXiv:2601.08794.
  7. A. Ghosh, K. Noui, and A. Perez, Phys. Rev. D 89, 084069 (2014).
  8. O. Asin, J. B. Achour, M. Geiller, K. Noui, and A. Perez, Phys. Rev. D 91, 084005 (2015).
  9. K. Krasnov, Phys. Rev. D 55, 3505 (1997).
  10. K. Krasnov, Gen. Relativ. Gravit. 30, 53 (1998).
  11. C. Rovelli, Phys. Rev. Lett. 77, 3288 (1996).
  12. C. Rovelli, Helv. Phys. Acta 69, 582 (1996).
  13. A. Ashtekar, J. Baez, A. Corichi, and K. Krasnov, Phys. Rev. Lett. 80, 904 (1998).
  14. A. Ashtekar, J. Baez, and K. Krasnov, Adv. Theor. Math. Phys. 4, 1 (2000).
  15. I. Agullo, J. F. Barbero G., E. F. Borja, J. Diaz-Polo, and E. J. S. Villaseñor, Phys. Rev. D 82, 084029 (2010).
  16. A. Perez, Rep. Prog. Phys. 80, 126901 (2017).
  17. S. Major and K. Setter, Classical Quantum Gravity 18, 5293 (2001); 18, 5125(E) (2001).
  18. C. Rovelli and L. Smolin, Phys. Rev. D 52, 5743 (1995).
  19. J. Engle, K. Noui, and A. Perez, Phys. Rev. Lett. 105, 031302 (2010).
  20. J. Engle, K. Noui, A. Perez, and D. Pranzetti, Phys. Rev. D 82, 044050 (2010).
  21. C. Rovelli and L. Smolin, Nucl. Phys. B442, 593 (1995); B456, 753(E) (1995).
  22. A. Ashtekar, J. Lewendowski, A. Ashtekar, and J. Lewendowski, Classical Quantum Gravity 14, A55 (1997).
  23. There may be vertices that lie in the surface but these are neglected here.

  24. Classically, the theory is equivalent to general relativity for all values of the parameter γ [25]. However, in the kinematical state space of LQG the Hilbert spaces Hγ for different γ’s are unitarily inequivalent representations [26].

  25. A. Ashtekar and J. Pullin, Loop Quantum Gravity: The First 30 Years (World Scientific, Singapore, 2017).
  26. C. Rovelli and T. Thiemann, Phys. Rev. D 57, 1009 (1998).
  27. E. Frodden, A. Ghosh, and A. Perez, Phys. Rev. D 87, 121503(R) (2013).
  28. S. Major, Phys. Rev. D 105, 104050 (2022).
  29. The corrections in the high-g limit are ln(g2A)4g+O(1/g).

  30. C. Rovelli and S. Speziale, Phys. Rev. D 67, 064019 (2003).
  31. M. Varadarajan, arXiv:2601.01198.
  32. J. Alfaro, H. A. Morales-Técotl, and L. F. Urrutia, Phys. Rev. D 65, 103509 (2002).
  33. A. Addazi et al., Prog. Part. Nucl. Phys. 125, 103948 (2022).
  34. F. Girelli, F. Hinterleitner, and S. Major, SIGMA 8, 098 (2012).
  35. S. Liberati, Classical Quantum Gravity 30, 133001 (2013).
  36. V. Hisain and J. Louko, Phys. Rev. Lett. 116, 061301 (2016).
  37. J. Collins, A. Perez, D. Sudarsky, L. Urrutia, and H. Vucetich, Phys. Rev. Lett. 93, 191301 (2004).
  38. The integral approximation for the correction is 14(πγ)3α(31)(x+α)2ex1dx2.02,where α=22πγ.

  39. S. Major, Classical Quantum Gravity 16, 3859 (1999).
  40. O. Dreyer, Phys. Rev. Lett. 90, 081301 (2003).
  41. H.-P. Nollert, Phys. Rev. D 47, 5253 (1993).
  42. S. Hod, Phys. Rev. Lett. 81, 4293 (1998).
  43. S. Major, q-quantum gravity, Ph.D. dissertation, The Pennsylvania State University, PennState, 1997.
  44. V. Husain and S. Major, Nucl. Phys. B500, 381 (1997).
  45. S. Speziale, Towards the graviton and the photon from spinfoams, Ph.D. dissertation, Sapienza University of Rome, Rome, 2004.
  46. K. Meissner, Classical Quantum Gravity 21, 5245 (2004).
  47. M. Domagala and J. Lewandowski, Classical Quantum Gravity 21, 5233 (2004).
  48. See page 28 and footnote 15 in the review [16].

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