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The Displacement Functional for Quantum Markov Semigroups: A Cramér-Rao Bound for Cumulative Dissipation

Christian Balfagon

Published Apr 3, 2026• 0 citations
Publisher

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.

DOI
10.5281/zenodo.19396273

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•Jul 14, 2026•0 citations

Exponential Relative Entropy Decay Along Quantum Markov Semigroups

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This paper introduces the displacement functional J(ρ0):=∫0∞S(Φt(ρ0)∣∣σ)dt\mathcal{J}(\rho_{0}) := \int_{0}^{\infty} S(\Phi_{t}(\rho_{0})||\sigma) dtJ(ρ0​):=∫0∞​S(Φt​(ρ0​)∣∣σ)dt for quantum Markov semigroups (QMS) with a unique faithful fixed point σ\sigmaσ. The functional measures the cumulative relative-entropy dissipation along the trajectory from an initial state ρ0\rho_{0}ρ0​ to the equilibrium state σ\sigmaσ. Main Results: Quantum Cramér-Rao Inequality: We prove a fundamental lower bound for J\mathcal{J}J given by J(ρ0)≥S(ρ0∣∣σ)2/EPL(ρ0)\mathcal{J}(\rho_{0}) \ge S(\rho_{0}||\sigma)^{2} / EP_{\mathcal{L}}(\rho_{0})J(ρ0​)≥S(ρ0​∣∣σ)2/EPL​(ρ0​), where EPEPEP 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: S2Λ≤J≤S2α\frac{S}{2\Lambda} \le \mathcal{J} \le \frac{S}{2\alpha}2ΛS​≤J≤2αS​. 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.
States of open quantum systems often decay continuously under environmental interactions. Quantum Markov semigroups model such processes in dissipative environments. It is known that finite-dimensional quantum Markov semigroups with GNS detailed balance universally obey complete modified logarithmic Sobolev inequalities (CMLSIs), yielding exponential decay of relative entropy to a subspace of fixed point states. We analyze continuous processes that combine dissipative with Hamiltonian time-evolution, precluding this notion of detailed balance. First, we find counterexamples to CMLSI-like decay for these processes and determine conditions under which it fails. In contrast, we prove that despite its absence at early times, exponential decay re-appears for unital, finite-dimensional quantum Markov semigroups at finite timescales. Finally, we show that when dissipation is much stronger than Hamiltonian time-evolution, the rate of eventual, exponential decay toward the semigroup's decoherence-free subspace is bounded inversely in the decay rate of the dissipative part alone. Dubbed self-restricting noise, this inverse relationship arises when strong damping suppresses effects that would otherwise spread noise beyond its initial subspace.
In this work, we extend the theory of quantum Markov processes on a single quantum state to a broader theory that covers Markovian evolution of an ensemble of quantum states, which generalizes Lindblad’s formulation of quantum dynamical semigroups. Our results establish the equivalence between an exponential decrease of the matrix Φ-entropies and the Φ-Sobolev inequalities, which allows us to characterize the dynamical evolution of a quantum ensemble to its equilibrium. In particular, we study the convergence rates of two special semigroups, namely, the depolarizing channel and the phase-damping channel. In the former, since there exists a unique equilibrium state, we show that the matrix Φ-entropy of the resulting quantum ensemble decays exponentially as time goes on. Consequently, we obtain a stronger notion of monotonicity of the Holevo quantity—the Holevo quantity of the quantum ensemble decays exponentially in time and the convergence rate is determined by the modified log-Sobolev inequalities. However, in the latter, the matrix Φ-entropy of the quantum ensemble that undergoes the phase-damping Markovian evolution generally will not decay exponentially. There is no classical analogy for these different equilibrium situations. Finally, we also study a statistical mixing of Markov semigroups on matrix-valued functions. We can explicitly calculate the convergence rate of a Markovian jump process defined on Boolean hypercubes and provide upper bounds to the mixing time.
In this paper, we study finite-mode Gaussian quantum Markov semigroups with a faithful invariant Gaussian state. We present an algebraic characterization of the complete modified logarithmic Sobolev inequality relative to the fixed-point algebra, and we obtain the corresponding optimal constant under the assumption that the drift evolution etZe^{t\mathbf{Z}}etZ converges as t→∞t\to\inftyt→∞. We establish hypercontractivity for such quantum Markov semigroups with Hurwitz drift, in the sense that every fixed pair $1
We investigate quantum Markov semigroups on bosonic Fock space and identify a broad class of infinite-dimensional dissipative evolutions that exhibit instantaneous Sobolev regularization. Motivated by stability problems in quantum computation, we show that for certain Lindblad operators that are polynomials of creation and annihilation operators, the resulting dynamics immediately transform any initial state into one with finite expectation in all powers of the number operator. A key application is in the bosonic cat code, where we obtain explicit estimates in the trace norm for the speed of convergence. These estimates sharpen existing perturbative bounds at both short and long times, offering new analytic tools for assessing stability and error suppression in bosonic quantum information processing. For example, we improve the strong exponential convergence of the (shifted) 222-photon dissipation to its asymptotic channel to the uniform topology. For multi-mode systems, a generation theorem in concentrated single-sandwich norms supplies the domain properties required for the regularization argument.
Reproducibility archive for the paper “The displacement functional for quantum Markov semigroups: a mean-residual-life criterion, a sharp classification, and relaxation anisotropy.” The paper studies, for a primitive quantum Markov semigroup with faithful stationary state, the displacement functional J(ρ₀) = ∫₀^∞ D(Φ_t ρ₀ ‖ σ) dt together with the initial divergence and the entropy-production rate, and asks when the dimensionless ratio 𝓡 = J·Σ/r₀² is at least one — a mean-residual-life inequality. It gives a sharp classification for the χ² and Umegaki relative-entropy divergences, an exact increasing-mean-residual-life criterion, the strong-field relaxation-anisotropy floor, and the mixing-time bounds. This archive contains the LaTeX source and compiled PDF, the figure generators, and the verification code. The self-contained script verification/reproduce_numerics.py reproduces every exact rational identity and high-precision numerical value quoted in the paper, using exact sympy arithmetic and mpmath (finishing with “ALL CHECKS PASSED”); verification/certificates/ contains the directed-rounding interval and sum-of-squares programs supporting the global log-convexity certificate and the strictness results. README.md gives the equation-to-test map, reproduction instructions, and the exact dependency versions