Massive fields in null-shifted Rindler wedges produce non-thermal spectra for accelerated observers, as mass eliminates the exponential Bogoliubov mixing that creates thermality.
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8 Pith papers cite this work. Polarity classification is still indexing.
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UNVERDICTED 8representative citing papers
A corner in the Euclidean black hole geometry enables direct derivation of the Wald entropy formula in F(R_abcd) gravity and the ADM Hamiltonian conjugate to the horizon Killing vector as the conjugate variable to inverse temperature.
Modular channels induce universal thermal filtering that explains Unruh and Page phenomena, reinterprets entanglement first law as Clausius relation to derive Einstein equations, and proposes MCFC linking causal screen area to filtered information storage.
Combining regular black hole metrics with memory burden suppresses evaporation and opens a 10^6-10^8 g PBH mass window that can comprise all dark matter.
Computes density of states for inverted harmonic oscillator on circle via stationary phase approximation to demonstrate semi-classical thermalization from Lyapunov instability.
An RG-improved Schwarzschild-like black hole yields a multipole-independent SCC ratio at the 6% level, a bell-shaped Hawking temperature, and remains the most Schwarzschild-like among regular black hole models while shadow-degenerate with Hayward and Bonanno-Reuter at the 1% level.
Dark matter halos suppress Hawking temperature and emission rates in regular black holes while enabling a range of horizon radii with positive specific heat capacity and a Davies-type phase transition.
Euler-Heisenberg coupling and surrounding matter fields modify the temperature profile, stability structure, and critical point location of AdS black holes, while changing Hawking radiation sparsity, photon sphere, and shadow size.
citing papers explorer
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Thermality Breakdown in Null-Shifted Rindler Wedges
Massive fields in null-shifted Rindler wedges produce non-thermal spectra for accelerated observers, as mass eliminates the exponential Bogoliubov mixing that creates thermality.
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Black hole thermodynamics is around the corner
A corner in the Euclidean black hole geometry enables direct derivation of the Wald entropy formula in F(R_abcd) gravity and the ADM Hamiltonian conjugate to the horizon Killing vector as the conjugate variable to inverse temperature.
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Modular Channels, Thermal Filtering and the Spectral Emergence of Spacetime
Modular channels induce universal thermal filtering that explains Unruh and Page phenomena, reinterprets entanglement first law as Clausius relation to derive Einstein equations, and proposes MCFC linking causal screen area to filtered information storage.
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Memory burden effect of regular primordial black holes
Combining regular black hole metrics with memory burden suppresses evaporation and opens a 10^6-10^8 g PBH mass window that can comprise all dark matter.
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Semi-classical Imprint of Horizon Induced Instability
Computes density of states for inverted harmonic oscillator on circle via stationary phase approximation to demonstrate semi-classical thermalization from Lyapunov instability.
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Renormalization-group improved Schwarzschild black hole: shadow, ringdown, and strong cosmic censorship
An RG-improved Schwarzschild-like black hole yields a multipole-independent SCC ratio at the 6% level, a bell-shaped Hawking temperature, and remains the most Schwarzschild-like among regular black hole models while shadow-degenerate with Hayward and Bonanno-Reuter at the 1% level.
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Hawking Temperature, Sparsity and Energy Emission Rate of Dark Matter Halo Regular Black Holes
Dark matter halos suppress Hawking temperature and emission rates in regular black holes while enabling a range of horizon radii with positive specific heat capacity and a Davies-type phase transition.
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Thermodynamic and Radiative Properties of Euler-Heisenberg AdS Black Holes Surrounded by Quintessence and Dark Matter with a Cloud of Strings
Euler-Heisenberg coupling and surrounding matter fields modify the temperature profile, stability structure, and critical point location of AdS black holes, while changing Hawking radiation sparsity, photon sphere, and shadow size.