The Black Hole's Thermodynamic Compass ✛ ✎

Original: "Entropy dynamics in gravitational collapse: From Minkowski breaking to de Sitter thermodynamics"
arXiv:2607.24349v1 · 2026-07-27 · arXiv non-exclusive · independent analysis · 2 min
The sign of the Hubble parameter in a de Sitter core, expansion or contraction, acts like a compass needle, determining whether gravitational entropy becomes positive or negative, thereby uniting two theories of collapse.

In 1973, Jacob Bekenstein proposed that black hole possess entropy — a measure of hidden disorder. Stephen Hawking later confirmed this by adding radiation, but the microscopic origin of entropy remained obscure. New research offers an answer: inside a black hole there is no singularity, but a dynamic de Sitter core — a tiny universe that expands or contracts. This core acts as a thermodynamic compass.

The compass needle is the sign of the expansion of the universe \(H\), which measures the expansion rate of space. If \(H > 0\), the core expands — the compass points to positive entropy. If \(H < 0\), the core contracts — the needle turns, and entropy becomes negative. Thus, a single sign determines the thermodynamic 'polarity' of the entire interior region.

In the expanding core scenario (OCK scenario), an inner Cauchy horizon forms — an additional boundary carrying its own share of entropy. For the typical case with integer parameter \(n=3\), this share reaches 59% of the outer horizon's entropy. As collapse proceeds, the number \(n\) decreases, the inner horizon shrinks, and the accumulated entropy is released, like sand pouring out of a broken compass.

The opposite scenario (black hole) contains a contracting core. Here, the compass points to negative entropy, which exactly compensates the outer horizon's entropy: the total entropy of the object is zero. This does not violate second law of thermodynamics — over time, the negative contribution disappears and entropy increases.

Both pictures, expansion and contraction, satisfy thermodynamics, but are separated by a classical barrier. When collapse reaches the 'Minkowski violation' point (disappearance of flat space at the center), the classical description breaks down. The subsequent transition between phases is a quantum jump, and its probability is exponentially small due to the huge entropy difference. The integer nature of the parameter \(n\) hints at a quantized entropy spectrum: \(\Delta S\) is quantized, like steps on a staircase.

Thus, the Hubble compass not only points the way but turns collapse into a story of quantum leaps. Perhaps gravitational waves from black hole mergers will one day capture these stepwise releases, confirming that inside the horizon lies not a point, but an entire universe with its own thermodynamic arrow.

For an astrophysical black hole of 10 M☉, the semiclassical description of collapse breaks down at n ~ 0.01—well before the classical Minkowski violation (n=0). In this regime, the inner horizon’s temperature surpasses the Planck temperature, and the geometry turns into a quantum foam.

S_{\mathrm{dS}} = \operatorname{sgn}(H) \frac{A}{4} = \operatorname{sgn}(H) \frac{\pi}{H^2}
The sign of entropy is determined by the sign of the Hubble parameter H; expansion yields positive entropy, contraction yields negative.
Scientists
Jacob BekensteinStephen HawkingFritz ZwickyKarl SchwarzschildSubrahmanyan ChandrasekharRainer Weiss
Concepts
black hole entropy black hole thermodynamics wald entropy entropic shadow hawking area law innermost stable circular orbit logarithmic correction entropic gravity horizon area inner horizon mass inflation hawking radiation mechanism de sitter space schwarzschild metric syk model modified gravity singularities kerr metric Accretion disk ringdown critical collapse