The Displacement Functional for Quantum Markov Semigroups: A Cramér-Rao Bound for Cumulative Dissipation
Christian Balfagon
Abstract
This paper introduces the displacement functional $\mathcal{J}(\rho_{0}) := \int_{0}^{\infty} S(\Phi_{t}(\rho_{0})||\sigma) dt$ for quantum Markov semigroups (QMS) with a unique faithful fixed point $\sigma$. The functional measures the cumulative relative-entropy dissipation along the trajectory from an initial state $\rho_{0}$ to the equilibrium state $\sigma$. Main Results: Quantum Cramér-Rao Inequality: We prove a fundamental lower bound for $\mathcal{J}$ given by $\mathcal{J}(\rho_{0}) \ge S(\rho_{0}||\sigma)^{2} / EP_{\mathcal{L}}(\rho_{0})$, where $EP$ is the entropy production rate. The "Sandwich" Bound: Combined with the Modified Logarithmic Sobolev Inequality (MLSI), we establish that the total dissipation is bounded both above and below: $\frac{S}{2\Lambda} \le \mathcal{J} \le \frac{S}{2\alpha}$. Rigidity Theorem: We demonstrate that the lower bound is sharp and is saturated if and only if the system's entropy decay follows a single exponential trajectory. Structural Stability: We prove that these properties are stable under perturbations of the generator. This work provides a missing piece in the study of quantum entropic convergence, offering a non-perturbative lower bound that complements existing upper bounds in open quantum systems.