Abstract

In loop quantum gravity, the number NΓ(A,γ)N_Γ(A,γ) of microstates of a black hole for a given discrete geometry ΓΓ depends on the so-called Barbero-Immirzi parameter γγ. Using a suitable analytic continuation of γγ to complex values, we show that the number NΓ(A,±i)N_Γ(A,\pm i) of microstates behaves as exp⁡(A/(4ℓPl2))\exp(A/(4\ell_\text{Pl}^2)) for large area AA in the large spin semiclassical limit. Such a correspondence with the semiclassical Bekenstein-Hawking entropy law points towards an unanticipated and remarkable feature of the original complex Ashtekar variables for quantum gravity.

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