Abstract The existence of a positive log-Sobolev constant implies a bound on the mixing time of a quantum dissipative evolution under the Markov approximation. For classical spin systems, such constant was proven to exist, under the assumption of a mixing condition in the Gibbs measure associated to their dynamics, via a quasi-factorization of the entropy in terms of the conditional entropy in some sub- σ -algebras. In this work we analyze analogous quasi-factorization results in the quantum case. For that, we define the quantum conditional relative entropy and prove several quasi-factorization results for it. As an illustration of their potential, we use one of them to obtain a positive log-Sobolev constant for the heat-bath dynamics with product fixed point.
We prove global existence and uniqueness of dynamics on the quasi-local algebra
A of a quantum lattice system for spatially growing derivations
LΦ=∑x[Φx,⋅]. Existing results assume that the local terms
Φx∈A of the generator are uniformly bounded in space with respect to appropriate weighted norms
∥Φx∥G,x. Analogous to the global existence result for first order ODEs, we show that global existence and uniqueness persist if the size of the local terms
∥Φx∥G,x grows at most linearly in space. This considerably enlarges the class of derivations known to have well-defined dynamics. Moreover, we obtain Lieb-Robinson bounds with exponential light cones for such dynamics.
For the proof, we assume Lieb-Robinson bounds with linear light cones for dynamics, whose generators have uniformly bounded local terms. Such bounds are known to hold, for example, if the local terms are of finite range or exponentially localized.