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arxiv: 1701.03872 · v2 · pith:CIXJLHGYnew · submitted 2017-01-14 · ❄️ cond-mat.str-el · cond-mat.stat-mech· quant-ph

Symmetric minimally entangled typical thermal states for canonical and grand-canonical ensembles

classification ❄️ cond-mat.str-el cond-mat.stat-mechquant-ph
keywords symmetricmettsbasesensemblesstatesautocorrelationscanonicalcollapse
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Based on the density matrix renormalization group (DMRG), strongly correlated quantum many-body systems at finite temperatures can be simulated by sampling over a certain class of pure matrix product states (MPS) called minimally entangled typical thermal states (METTS). When a system features symmetries, these can be utilized to substantially reduce MPS computation costs. It is conceptually straightforward to simulate canonical ensembles using symmetric METTS. In practice, it is important to alternate between different symmetric collapse bases to decrease autocorrelations in the Markov chain of METTS. To this purpose, we introduce symmetric Fourier and Haar-random block bases that are efficiently mixing. We also show how grand-canonical ensembles can be simulated efficiently with symmetric METTS. We demonstrate these approaches for spin-1/2 XXZ chains and discuss how the choice of the collapse bases influences autocorrelations as well as the distribution of measurement values and, hence, convergence speeds.

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  1. Gauge-invariant QMETTS with mutually unbiased physical bases for $Z_2$ lattice gauge theories at finite temperature and density

    quant-ph 2026-03 conditional novelty 7.0

    Introduces gauge-invariant QMETTS using mutually unbiased physical bases derived from stabilizer formalism for Z2 LGT at finite T and density, with single-shot sampling shown near-optimal and numerical validation in 1+1D.