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The Fisher Information Sector of Perelman's Functionals on Black Hole Spatial Slices

Information Geometry Meets Black Hole Physics

The Fisher Information Sector of Perelman's Functionals on Black Hole Spatial Slices

Author: Lark Laflamme

Date: April 2026

Status: Version 3.2 Final - Submission-ready

Abstract

We study the Fisher information component F of Perelman's F-functional on black hole spatial slices, using the heat kernel to determine the Boltzmann measure from first principles.

Mathematical results (no physical assumptions): On constant-curvature slices, the curvature component FR is a constant independent of the black hole, and F is the unique carrier of state-dependent gravitational information (Theorem 1). On the BTZ spatial slice, exact computation gives F = r+/ℓ2.

Near-horizon structural result: F = 1/(2τ), where τ is the heat kernel diffusion parameter. The horizon area cancels; the result is dimension-independent.

Conditional geometric interpretation: If τ = 1/(2κ), then F = κ (surface gravity), and the Hawking temperature T = κ/(2π) follows without thermodynamic input.

1. Introduction

Perelman's Ricci flow functionals (2002) have a natural statistical mechanics structure: the F-functional decomposes into a curvature component FR and a gradient component F, where the latter is a Fisher information in the sense of Amari (1985). Despite significant interest in connecting Perelman's mathematics to gravitational physics, no explicit computation of these functionals on a black hole geometry has appeared in the literature.

This paper fills that gap. We compute Perelman's F and W on the BTZ spatial slice and discover a structural result: on constant-curvature backgrounds, the curvature component carries no state-dependent information, and the Fisher information component carries all of it.

2. Summary of Results

Tier 1: Mathematical Results (No Physical Assumptions)

Theorem 1 (Fisher Information Theorem): On a constant-curvature surface, FR = R0 (constant, independent of the Boltzmann measure and black hole parameters). All state dependence resides in F.
The BTZ Computation: With the exact heat kernel: F = r+/ℓ2 and W = ½ln(r+) + const.

Tier 2: Conditional on the Diffusion-Parameter Identification

Theorem 2 (Near-Horizon Formula): For the heat kernel centered at the horizon: F = 1/(2τ). This is dimension-independent; the horizon area cancels between numerator and normalization.
Proposition 1 (Surface Gravity): If τ = 1/(2κ) (motivated by Euclidean regularity, not derived from Perelman's framework), then F = κ. Temperature follows: T = κ/(2π).
Proposition 2 (Structural Cancellation): In the W-functional, τ · F = 1/2 (constant). This is a non-trivial structural constraint.

Tier 3: Interpretive Proposals

3. Physical Significance

The central discovery is a division of labor within Perelman's functional: curvature sets the stage, but the measure gradient carries the state-dependent physics. On constant-curvature backgrounds — which include the BTZ black hole and the near-horizon region of any black hole — the curvature component FR is a fixed constant. All information about which black hole we are looking at resides in the Fisher information F.

The near-horizon formula F = 1/(2τ) is striking in its simplicity: the horizon area cancels, the result is dimension-independent, and F measures a local quantity (diffusion sharpness of the thermal measure) rather than a global one like entropy.

Significance: This paper provides the first explicit computation of Perelman's Ricci flow functionals on black hole geometry. The information-geometric content resides in the gradient sector of the Boltzmann measure, suggesting a deep connection between Fisher information geometry and black hole thermodynamics that operates through the measure, not through the curvature.