Gauging a superposition of fermionic Gaussian projected entangled pair states to get lattice gauge theory eigenstates

A bstract Gauged fermionic projected entangled pair states (GFPEPS) and their Gaussian counterpart (GGFPEPS) are a novel type of lattice gauge theory Ansatz state that combine ideas from the Monte Carlo and tensor network communities. In particular, computation of observables for such states boils down to a Monte Carlo integration over possible gauge field configurations that have probabilities dictated by a fermionic tensor network contraction that accounts for the matter in that background configuration. Crucially, this probability distribution is positive definite and real so that there is no sign problem. When the underlying PEPS is Gaussian, tensor network contraction can be done efficiently, and in this scenario the Ansatz has been tested well numerically. In this work we propose to gauge superpositions of Gaussian PEPS and demonstrate that one can still efficiently compute observables when few Gaussians are in the superposition. As we will argue, the latter is exactly the case for bound states on top of the strongly interacting LGT vacuum, which makes this Ansatz particularly suitable for that scenario. As a corollary, we will provide an exact representation of the LGT ground state as a gauged PEPS.

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Publication Details

Journal
Journal of High Energy Physics
Published
2025-11-11
DOI
https://doi.org/10.1007/jhep11(2025)052
Primary Topic
Quantum many-body systems
Type
article
Field-Weighted Citation Impact
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article

Gauging a superposition of fermionic Gaussian projected entangled pair states to get lattice gauge theory eigenstates

Erez Zohar, Gertian Roose
Journal of High Energy Physics
Quantum many-body systems
article

Gauging a superposition of fermionic Gaussian projected entangled pair states to get lattice gauge theory eigenstates

Erez Zohar, Gertian Roose
article en

Abstract

A bstract Gauged fermionic projected entangled pair states (GFPEPS) and their Gaussian counterpart (GGFPEPS) are a novel type of lattice gauge theory Ansatz state that combine ideas from the Monte Carlo and tensor network communities. In particular, computation of observables for such states boils down to a Monte Carlo integration over possible gauge field configurations that have probabilities dictated by a fermionic tensor network contraction that accounts for the matter in that background configuration. Crucially, this probability distribution is positive definite and real so that there is no sign problem. When the underlying PEPS is Gaussian, tensor network contraction can be done efficiently, and in this scenario the Ansatz has been tested well numerically. In this work we propose to gauge superpositions of Gaussian PEPS and demonstrate that one can still efficiently compute observables when few Gaussians are in the superposition. As we will argue, the latter is exactly the case for bound states on top of the strongly interacting LGT vacuum, which makes this Ansatz particularly suitable for that scenario. As a corollary, we will provide an exact representation of the LGT ground state as a gauged PEPS.

Journal of High Energy PhysicsVol. 2025(11)
Tel Aviv University (IL), Hebrew University of Jerusalem (IL)
Openalex Percentile: Top 73%
Quantum many-body systems
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