4.5 Article

Finite-temperature symmetric tensor network for spin-1/2 Heisenberg antiferromagnets on the square lattice

Journal

SCIPOST PHYSICS
Volume 10, Issue 1, Pages -

Publisher

SCIPOST FOUNDATION
DOI: 10.21468/SciPostPhys.10.1.019

Keywords

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Funding

  1. French Research Council [TNSTRONG ANR-16-CE30-0025, TNTOP ANR-18CE30-0026-01]

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The (positive) thermal density operator in the tensor network framework can be approximated by a double layer of infinite iPEPO coupled via ancilla degrees of freedom. A variational optimization is performed on plaquettes to investigate the thermal properties of the spin1/2 Heisenberg model, showing accurate behavior of various observables and validating the imaginary-time evolution procedure. The method is extended to frustrated models, with preliminary results shown.
Within the tensor network framework, the (positive) thermal density operator can be approximated by a double layer of infinite Projected Entangled Pair Operators (iPEPO) coupled via ancilla degrees of freedom. To investigate the thermal properties of the spin1/2 Heisenberg model on the square lattice, we introduce a family of fully spin-SU (2) and lattice-C-4v symmetric on-site tensors (of bond dimensions D = 4 or D = 7) and a plaquette-based Trotter-Suzuki decomposition of the imaginary-time evolution operator. A variational optimization is performed on the plaquettes, using a full (for D = 4) or simple (for D = 7) environment obtained from the single-site Corner Transfer Matrix Renormalization Group fixed point. The method is benchmarked by a comparison to quantum Monte Carlo in the thermodynamic limit. Although the iPEPO spin correlation length starts to deviate from the exact exponential growth for inverse-temperature beta greater than or similar to 2, the behavior of various observables turns out to be quite accurate once plotted w.r.t the inverse correlation length. We also find that a direct T = 0 variational energy optimization provides results in full agreement with the beta ->infinity limit of finite-temperature data, hence validating the imaginary-time evolution procedure. Extension of the method to frustrated models is described and preliminary results are shown.

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