Entanglement and Charge-Sharpening Transitions in U(1) Symmetric Monitored Quantum Circuits
Entanglement and Charge-Sharpening Transitions in U(1) Symmetric Monitored Quantum Circuits
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DOI:
10.1103/physrevx.12.041002
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发表时间:
2021-07
影响因子:
12.5
通讯作者:
Utkarsh Agrawal;A. Zabalo;Kun Chen;Justin H. Wilson;A. Potter;J. Pixley;S. Gopalakrishnan;R. Vasseur
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文献类型:
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作者:
Utkarsh Agrawal;A. Zabalo;Kun Chen;Justin H. Wilson;A. Potter;J. Pixley;S. Gopalakrishnan;R. Vasseur
Monitored quantum circuits can exhibit an entanglement transition as a function of the rate of measurements, stemming from the competition between scrambling unitary dynamics and disen-tangling projective measurements. We study how entanglement dynamics in non-unitary quantum circuits can be enriched in the presence of charge conservation, using a combination of exact numerics and a mapping onto a statistical mechanics model of constrained hard-core random walkers. We uncover a charge-sharpening transition that separates different scrambling phases with volume-law scaling of entanglement, distinguished by whether measurements can efficiently reveal the total charge of the system. We find that while R´enyi entropies grow sub-ballistically as √ t in the absence of measurement, for even an infinitesimal rate of measurements, all average R´enyi entropies grow ballistically with time ∼ t . We study numerically the critical behavior of the charge-sharpening and entanglement transitions in U(1) circuits, and show that they exhibit emergent Lorentz invariance and can also be diagnosed using scalable local ancilla probes. Our statistical mechanical mapping technique readily generalizes to arbitrary Abelian groups, and offers a general framework for studying dissipatively-stabilized symmetry-breaking and topological orders. monitored quantum circuits. Our numerical results indicate that there are two distinct phases in the entangling (volume-law) regime p 1 ] ∼ √ t to ballistic ∼ t scaling over a time scale ∼ p − 3 / 2 , then (2) charge sharpens after the crossover time scale t # ∼ L , and finally (3) the system purifies over a much long time scale t π ∼ e L .