Abstract
We show that spin chains in thermal equilibrium have a correlation structure in which individual regions are strongly correlated at most with their near vicinity. We quantify this with alternative notions of the conditional mutual information, defined through the so-called Belavkin–Staszewski relative entropy. We prove that these measures decay superexponentially at every positive temperature, under the assumption that the spin chain Hamiltonian is translation-invariant. Using a recovery map associated with these measures, we sequentially construct tensor network approximations in terms of marginals of small (sublogarithmic) size. As a main application, we show that classical representations of the states can be learned efficiently from local measurements with a polynomial sample complexity. We also prove an approximate factorization condition for the purity of the entire Gibbs state, which implies that it can be efficiently estimated to a small multiplicative error from a small number of local measurements. The results extend from strictly local to exponentially-decaying interactions above a threshold temperature, albeit only with exponential decay rates. As a technical step of independent interest, we show an upper bound to the decay of the Belavkin–Staszewski relative entropy upon the application of a conditional expectation.
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CITATION STYLE
Alhambra, A. M., Capel, Á., Gondolf, P., Ruiz-de-Alarcón, A., & Scalet, S. O. (2026). Conditional Independence of 1D Gibbs States with Applications to Efficient Learning. Annales Henri Poincare. https://doi.org/10.1007/s00023-026-01655-6
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