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Efficient simulation of Grassmann Tensor Product States

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arxiv 1109.4470 v2 pith:IJORT3OC submitted 2011-09-21 cond-mat.str-el quant-ph

classification cond-mat.str-elquant-ph
keywords approachgtpssimplefermionproductstatestensorvariational
verification ladder T0 review T1 audit T2 compute T3 formal
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abstract

Recently, the Grassmann-tensor-entanglement renormalization group(GTERG) approach was proposed as a generic variational approach to study strongly correlated boson/fermion systems. However, the weakness of such a simple variational approach is that generic Grassmann tensor product states(GTPS) with large inner dimension $D$ will contain a large number of variational parameters and be hard to be determined through usual minimization procedures. In this paper, we first introduce a standard form of GTPS which significantly simplifies the representations. Then we describe a simple imaginary-time-evolution algorithm to efficiently update the GTPS based on the fermion coherent state representation and show all the algorithm developed for usual tensor product states(TPS) can be implemented for GTPS in a similar way. Finally, we study the environment effect for the GTERG approach and propose a simple method to further improve its accuracy. We demonstrate our algorithms by studying a simple 2D free fermion system on honeycomb lattice, including both off-critical and critical cases.

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Cited by 2 Pith papers

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  1. Phase diagram of the single-flavor Gross--Neveu--Wilson model from the Grassmann corner transfer matrix renormalization group

    hep-lat 2026-02 conditional novelty 6.0 of 10

    For one-flavor Gross-Neveu-Wilson fermions, the Aoki phase is bounded by c=1/2 Ising critical lines and terminates at strong coupling, while c=1 lines separate topological and trivial insulators.

  2. Toward tensor renormalization group study of lattice QCD

    hep-lat 2025-01 conditional novelty 3.0 of 10

    Tensor renormalization group methods for multi-flavor and non-Abelian gauge theories are summarized with 2D Z2 and 3D SU(2) and SU(3) proof-of-principle results.

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