SciPost Phys. 10, 019 (2021) ·
published 28 January 2021
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Within the tensor network framework, the (positive) thermal density operator
can be approximated by a double layer of infinite Projected Entangled Pair
Operator (iPEPO) coupled via ancilla degrees of freedom. To investigate the
thermal properties of the spin-1/2 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 $\beta \gtrsim 2$, 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
$\beta\rightarrow\infty$ 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.
SciPost Phys. 7, 041 (2019) ·
published 2 October 2019
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We consider a family of SU(2)-symmetric Projected Entangled Paired States
(PEPS) on the square lattice, defining colored-Resonating Valence Bond (RVB)
states, to describe the quantum disordered phase of the $J_1-J_2$ frustrated
Heisenberg model.For $J_2/J_1\sim 0.55$ we show the emergence of critical
(algebraic) dimer-dimer correlations -- typical of Rokhsar-Kivelson (RK) points
of quantum dimer models on bipartite lattices -- while, simultaneously, the
spin-spin correlation length remains short. Our findings are consistent with a
spin liquid or a weak Valence Bond Crystal in the neighborhood of an RK point.
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