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Monomer-dimer tensor-network basis for qubit-regularized lattice gauge theories

Shailesh Chandrasekharan1,*, Rui Xian Siew1,†, and Tanmoy Bhattacharya2,‡

  • *Contact author: sch27@duke.edu
  • †Contact author: ruixian.siew@duke.edu
  • ‡Contact author: tanmoy@lanl.gov

Phys. Rev. D 111, 114502 – Published 6 June, 2025

DOI: https://doi.org/10.1103/gns9-l3gk

Abstract

Traditional SU(N) lattice gauge theories (LGTs) can be formulated using an orthonormal basis constructed from the irreducible representations (irreps) Vλ of the SU(N) gauge symmetry. On a lattice, the elements of this basis are tensor networks comprising dimer tensors on the links labeled by a set of irreps {λℓ} and monomer tensors on sites labeled by {λs}. These tensors naturally define a local site Hilbert space, Hsg, on which gauge transformations act. Gauss’s law introduces an additional index αs=1,2,…,D(Hsg) that labels an orthonormal basis of the gauge-invariant subspace of Hsg. This monomer-dimer tensor-network (MDTN) basis, |{λs},{λℓ},{αs}⟩, of the physical Hilbert space enables the construction of new qubit-regularized SU(N) gauge theories that are free of sign problems while preserving key features of traditional LGTs. Here, we investigate finite-temperature confinement-deconfinement transitions in a simple qubit-regularized SU(2) and SU(3) gauge theory in d=2 and d=3 spatial dimensions, formulated using the MDTN basis, and show that they reproduce the universal results of traditional LGTs at these transitions. Additionally, in d=1, we demonstrate using a plaquette chain that the string tension at zero temperature can be continuously tuned to zero by adjusting a model parameter that plays the role of the gauge coupling in traditional LGTs.

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