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Quantum evaporation rates for Standard Model particles in de Sitter black holes

Compute the quantum evaporation rates for Standard Model fields for both near-extremal Reissner–Nordström–de Sitter and Kerr–de Sitter black holes, incorporating the Bunch–Davies thermal environment and near-horizon Schwarzian corrections, and quantify emission versus absorption across the lukewarm equilibrium line.

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Background

The paper develops a quantum evolution framework for near-extremal, small de Sitter black holes using a one-dimensional Schwarzian effective theory at the AdS2 throat, coupled to far-horizon de Sitter quantum fields prepared in the Bunch–Davies vacuum. It computes energy transfer rates for massless, uncharged s-wave scalars and shows significant deviations from Hawking’s semiclassical predictions, including suppressed emission when the black hole is hotter than the cosmological horizon and constant-rate absorption in the colder regime.

Extending these results to realistic particle content requires treating Standard Model degrees of freedom (spin, charge, statistics, and interactions) in the near-extremal Schwarzian framework and properly coupling them to the thermal de Sitter environment. This would provide quantitative predictions for the quantum-corrected evaporation and absorption dynamics of charged and rotating de Sitter black holes beyond the toy scalar model studied here.

References

Let us conclude the paper with some open problems. The natural next order question is to compute the quantum evaporation rates for Standard Model particles for both charged and rotating black holes in de Sitter.

Quantum evolution of de Sitter black holes near extremality (2510.18035 - Bhattacharjee et al., 20 Oct 2025) in Section 6, Subsection "Future directions"