GUP parameter and black hole temperature
Elias C.Vagenas, Salwa M. Alsaleh, Ahmed Farag Ali

TL;DR
This paper derives the GUP parameter by comparing the GUP-deformed black hole temperature with the quantum-corrected Hawking temperature, revealing its dependence on the black hole mass and Planck mass.
Contribution
It introduces a method to determine the GUP parameter considering both linear and quadratic momentum terms, linking it to black hole and quantum corrections.
Findings
GUP parameter depends on the ratio of Planck mass to black hole mass
Equating temperature corrections yields a specific GUP parameter value
The GUP parameter is not a pure number but mass-dependent
Abstract
Motivated by a recent work of Scardigli, Lambiase and Vagenas (SLV), we derive the GUP parameter, i.e. , when the GUP has a linear and quadratic term in momentum. The value of the GUP parameter is obtained by conjecturing that the GUP-deformed black hole temperature of a Schwarzschild black hole and the modified Hawking temperature of a quantum-corrected Schwarzschild black hole are the same. The leading term in both cases is the standard Hawking temperature and since the corrections are considered as thermal, the modified and deformed expressions of temperature display a slight shift in the Hawking temperature. Finally, by equating the first correction terms, we obtain a value for the GUP parameter. In our analysis, the GUP parameter is not a pure number but depends on the ratio with to be the Planck mass and the black hole mass.
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