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Effects of monitoring on entanglement dynamics for (1+1)DZ2 lattice gauge theory

Nilachal Chakrabarti1,*, Nisa Ara2,3,4,†, Neha Nirbhan1,‡, Arpan Bhattacharyya1,§, and Indrakshi Raychowdhury3,4,∥

  • *Contact author: nilachalchakrabarti@iitgn.ac.in
  • †Contact author: nisa.ara@theory.tifr.res.in
  • ‡Contact author: neha.nirbhan1207@gmail.com
  • §Contact author: abhattacharyya@iitgn.ac.in
  • ∥Contact author: indrakshir@goa.bits-pilani.ac.in

APS Open Sci. 1, 000118 – Published 1 September, 2026

DOI: https://doi.org/10.1103/1tmj-fftr

Abstract

The (1+1)-dimensional Z2 gauge theory is the simplest model that allows for quantum simulation to probe the fundamental aspects of a gauge theory coupled with dynamical fermions. To reliably benchmark such a system, it is crucial to understand the nonunitary quantum dynamics arising from effective non-Hermitian evolution and postselected monitoring protocols. This work focuses on the postselected non-Hermitian filtering dynamics of a Z2 gauge theory, where the non-Hermitian terms are associated with local and nonlocal gauge-invariant operators naturally present in the theory. We interpret the resulting dynamics as postselected filtering, where different operator sectors are coupled to loss channels with different rates. This gives a unified framework for both the local electric flux and particle-number terms and the nonlocal mesonic hopping term. Tensor network calculations are performed to probe the effect of the filtering for larger lattice sizes (up to 256-site systems). Using matrix product state calculations, the dynamics of entanglement entropy are studied as a function of the filtering rate and the coupling constant. We find that, under both local and nonlocal filtering, the late-time saturation value of the bipartite entanglement entropy remains independent of system size, providing no evidence of a measurement-induced phase transitionlike phenomenon in the postselected dynamics across the range of filtering strengths, evolution times, and system sizes considered here.

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