Finite-Temperature de Bruijn Identities: Fisher Information as the Spectral Gap of Blahut--Arimoto Dynamics

arXiv:2606.03813v1 Announce Type: new Abstract: We uncover a finite-temperature extension of de Bruijn's identity -- the classical relation $\frac{d}{dt}h(X+\sqrt{t}Z)=\frac{1}{2}J(X)$ connecting differential entropy and Fisher information. Our framework is the spectral theory of Blahut--Arimoto (BA) dynamics, recently developed by Wang~\cite{Wang2026} for the analysis of rate-distortion optimization. The central observation is elementary yet profound: for Gaussian sources, the spectral gap $\lam$ of the BA relaxation kernel $\G$ satisfies $\lam = 1/(2\beta\sigma^2)$~\cite{Wang2026}, while the Fisher information of the source is $J = 1/\sigma^2$. Hence \[ {\lam = \frac{J}{2\beta}} \] for all inverse temperatures $\beta > 1/(2\sigma^2)$. This identifies the BA spectral gap as a \emph{finite-temperature regularization of Fisher information}. From this observation we derive an exact finite-temperature de Bruijn identity: \[ \frac{\partial F_\beta}{\partial \sigma^2} = \frac{1}{2\beta\sigma^2} = \lam, \] where $F_\beta$ is the BA free energy. This identity holds for all finite $\beta$ without any limit procedure. The classical de Bruijn identity follows as the exact consequence $\beta\,\partial F_\beta/\partial\sigma^2 = J/2$. The significance is structural: classical de Bruijn is not an isolated fact about Gaussian convolutions, but the $\beta\to\infty$ shadow of a one-parameter family of exact identities living in the spectral geometry of rate-distortion optimization. We discuss implications for the entropy power inequality, the $\chi^2$-dissipation structure of BA dynamics, and the geometric unification of information inequalities.