Theoretical analysis demonstrates the derivation of the Bekenstein-Hawking area law coefficient in causal horizons, indicating a model-independent foundation for black hole thermodynamics.
The Bekenstein-Hawking area law S = A/(4 l_P^2) has been rigorously confirmed by multiple independent approaches, yet the precise preconditions required for its validity and the physical origin of the coefficient 1/4 have so far lacked a clear conceptual explanation. The aim of this paper is to identify a set of precisely defined sufficient conditions under which the coefficient structure of the area law can be reconstructed, and thereby to delineate the scope of applicability of the formula. We do not claim that this set of conditions is the only possible one. The sufficient conditions proposed here include: spherical symmetry of the causal boundary, unitarity (information conservation and discretization), the one-dimensional causal limit scale l_P, and the definition of the causal boundary as a holographic screen (separating observable and inaccessible regions). Within this framework, the coefficient of the area law is reconstructed as the algebraic combination 4π × (1/2) × (1/2), where 4π originates from the topology of the sphere S², and the two factors of 1/2 arise respectively from the unidirectional projection of the causal boundary and the bilateral equipartition of degrees of freedom---both introduced as working hypotheses rather than logical necessities. Starting from the reconstructed area law, we further derive the Hawking temperature in reverse, verifying the self-consistency of the framework, and discuss possible modifications of the area law when each of the preconditions is violated. This work provides a conceptual foundation for the holographic area law that is independent of specific microscopic models, and furnishes it with a clearly defined scope of applicability.
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Fanlei Meng (2026) studied this question.
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