Thermal Pure Quantum States of Many-Particle Systems

TL;DR

This paper extends the thermal pure quantum (TPQ) framework to infinite-dimensional systems, introducing the grand-canonical TPQ (gTPQ) state, which accurately reproduces statistical mechanics quantities with minimal error, enhancing both theoretical understanding and practical computations.

Contribution

It develops the gTPQ state for infinite-dimensional systems, enabling accurate, single-state representations of statistical mechanics in particle systems, and demonstrates its effectiveness on the Hubbard model.

Findings

gTPQ states match exact solutions in 1D Hubbard model

Reliable results for 2D triangular lattice without exact solutions

Finite-size effects are smaller in gTPQ than in cTPQ

Abstract

We generalize the thermal pure quantum (TPQ) formulation of statistical mechanics, in such a way that it is applicable to systems whose Hilbert space is infinite dimensional. Assuming particle systems, we construct the grand-canonical TPQ (gTPQ) state, which is the counterpart of the grand-canonical Gibbs state of the ensemble formulation. A single realization of the gTPQ state gives all quantities of statistical-mechanical interest, with exponentially small probability of error. This formulation not only sheds new light on quantum statistical mechanics but also is useful for practical computations. As an illustration, we apply it to the Hubbard model, on a one-dimensional (1d) chain and on a two-dimensional (2d) triangular lattice. For the 1d chain, our results agree well with the exact solutions over wide ranges of temperature, chemical potential and the on-site interaction. For the 2d triangular lattice, for which exact results are unknown, we obtain reliable results over a wide range of temperature. We also find that finite-size effects are much smaller in the gTPQ state than in the canonical TPQ (cTPQ) state. This also shows that in the ensemble formulation the grand-canonical Gibbs state of a finite-size system simulates an infinite system much better than the canonical Gibbs state.