The processes of splitting and merging of black holes obey the composition law generated by the Tsallis-Cirto δ=2 statistics. The same composition law expresses the full entropy of the Reissner-Nordström black hole via the entropies of its outer and inner horizons. He we apply this composition law to the entropy of the Kerr black hole. As distinct from Reissner-Nordström black hole, where the full entropy depends only on mass M and does not depend on its charge Q, the entropy of Kerr black hole is the sum of contributions from its mass M and angular momentum J, i. e. S (M, J) =S (M, 0) + 4πJ (J+1). Here S (M, 0) is the entropy of the Schwarzschild black hole. This demonstrates that when the Kerr black hole with J 1 absorbs or emits a massless particle with spin sᵦ= 1/2, its entropy changes by |ΔS| = 2π. We also considered the quantization of entropy suggested by the toy model, in which the black hole thermodynamics is represented by the ensemble of the Planck-scale black holes -- Planckons.
G. E. Volovik (Sun,) studied this question.
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