We study a free fermion model where two sets of non-commuting non-projective measurements stabilize area-law entanglement scaling phases of distinct topological order. We show the presence of a topological phase transition that is of a different universality class than that observed in stroboscopic projective circuits. In the presence of unitary dynamics, the two topologically distinct phases are separated by a region with sub-volume scaling of the entanglement entropy. We find that this entanglement transition is well identified by a combination of the bipartite entanglement entropy and the topological entanglement entropy. We further show that the phase diagram is qualitatively captured by an analytically tractable non-Hermitian model obtained via post-selecting the measurement outcome. Finally we introduce a partial-post-selection continuous mapping, that uniquely associates topological indices of the non-Hermitian Hamiltonian to the distinct phases of the stochastic measurement-induced dynamics.
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Department of Physics and Astronomy, University College London, Gower Street, LondonDepartment of Physics and Astronomy, University College London, Gower Street, London
Szyniszewski M.
Lunt O.
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Department of Physics and Astronomy, University College London, Gower Street, London
Department of Physics, King's College London, Strand, London
School of Physics & Astronomy, University of Birmingham, BirminghamDepartment of Physics and Astronomy, University College London, Gower Street, London
Lunt O.
Pal A.
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Department of Physics and Astronomy, University College London, Gower Street, LondonDepartment of Physics and Astronomy, University College London, Gower Street, London
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Philippe Meyer Institute, Physics Department, École Normale Supérieure (ENS), Université PSL, 24 rue Lhomond, ParisPhilippe Meyer Institute, Physics Department, École Normale Supérieure (ENS), Université PSL, 24 rue Lhomond, Paris
Fava M.
Piroli L.
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Philippe Meyer Institute, Physics Department, École Normale Supérieure (ENS), Université PSL, 24 rue Lhomond, ParisPhilippe Meyer Institute, Physics Department, École Normale Supérieure (ENS), Université PSL, 24 rue Lhomond, Paris
Piroli L.
Swann T.
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Rudolf Peierls Centre for Theoretical Physics, Clarendon Laboratory, Parks Road, OxfordPhilippe Meyer Institute, Physics Department, École Normale Supérieure (ENS), Université PSL, 24 rue Lhomond, Paris
Swann T.
Bernard D.
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Laboratoire de Physique de l'École Normale Supérieure, CNRS, ENS, Université PSL, Sorbonne Université, Université Paris Cité, ParisPhilippe Meyer Institute, Physics Department, École Normale Supérieure (ENS), Université PSL, 24 rue Lhomond, Paris
Bernard D.
Nahum A.
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Laboratoire de Physique de l'École Normale Supérieure, CNRS, ENS, Université PSL, Sorbonne Université, Université Paris Cité, ParisPhilippe Meyer Institute, Physics Department, École Normale Supérieure (ENS), Université PSL, 24 rue Lhomond, Paris
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Univ Pisa, Dipartimento Fis, Largo B Pontecorvo 3, I-56127 Pisa, Italy
INFN Sez Pisa, Largo B Pontecorvo 3, I-56127 Pisa, ItalyUniv Catania, Dipartimento Matemat & Informat, Viale Andrea Doria 6, I-95125 Catania, Italy
Rossini, Davide
Russomanno, Angelo
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Univ Napoli Federico II, Dipartimento Fis & Pancini, Complesso Monte S Angelo, via Cinthia, I-80126 Naples, ItalyUniv Catania, Dipartimento Matemat & Informat, Viale Andrea Doria 6, I-95125 Catania, Italy