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Entanglement entropy of theQ<mml:mspace width="0.16em"/>≥<mml:mspace width="0.16em"/>4quantum Potts chain

2016/08/17 by Péter Lajkó, Ferenc Iglói
Computer Science · Physics and Astronomy · #Algorithm #Computer science #Entropy (arrow of time) #Physics #Quantum Computing Algorithms and Architecture #Quantum Information and Cryptography #Quantum many-body systems #Thermodynamics #cond-mat.stat-mech

paper · pdf · doi:10.1103/physreve.95.012105

published as Phys. Rev. E 95, 012105 (2017)

arxiv created 2016/08/17 · openalex created_date 2016/09/16 · openalex publication_date 2017/01/04 · arxiv updated 2017/01/11 · openalex updated_date 2026/08/05

Abstract

The entanglement entropy S is an indicator of quantum correlations in the ground state of a many-body quantum system. At a second-order quantum phase-transition point in one dimension S generally has a logarithmic singularity. Here we consider quantum spin chains with a first-order quantum phase transition, the prototype being the Q-state quantum Potts chain for Q&gt;4 and calculate S across the transition point. According to numerical, density matrix renormalization group results at the first-order quantum phase transition point S shows a jump, which is expected to vanish for Q\ensuremath→4+. This jump is calculated in leading order as \mathrm\ensuremathΔS=lnQ[1\ensuremath-4/Q\ensuremath-2/(QlnQ)+O(1/Q2)].

Citations