Bridging quantum criticality via many-body scarring
ORAL
Abstract
Quantum dynamics in certain kinetically-constrained systems can display a strong sensitivity to the initial condition, wherein some initial states give rise to persistent quantum revivals—a type of weak ergodicity breaking known as “quantum many-body scarring” (QMBS) due to mid spectrum "scarred" eigenstates. Another well-known phenomena is quantum criticality which, in contrast, concerns the properties of ground states. While initially appearing as independent properties, we show that this picture can be much richer in systems that display QMBS dynamics from a continuous family of initial conditions: As the system is tuned across the critical point while at the same time deforming the initial state, the dynamical signatures of QMBS at intermediate times can undergo an apparently smooth evolution across the equilibrium phase transition point. Remarkably the dynamics exactly at the critical point also displays profound ergodicity breaking. We demonstrate this using the PXP model—a paradigmatic model of QMBS. Using exact diagonalization and matrix product state methods, we map out the dynamical phase diagram of the PXP model with the quenched chemical potential. We demonstrate the existence of a continuous family of initial states that give rise to QMBS and formulate a ramping protocol that we use to prepare such states on QuEra's quantum simulator where we find great agreement. Our results show the ubiquity of scarring in the PXP model and highlight its intriguing interplay with quantum criticality.
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Publication: https://journals.aps.org/prb/abstract/10.1103/PhysRevB.107.235108<br>Unreleased arXiv e-print with A. Hudomal, A. Daniel, QuEra, et al arXiv:XXXX.XXXXX
Presenters
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Aiden L Daniel
University of Leeds
Authors
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Aiden L Daniel
University of Leeds
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Ana Hudomal
Institute of Physics Belgrade
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Zlatko Papic
University of Leeds
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Jean-Yves Desaules
Institute of Science and Technology Austria
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Guo-Xian Su
Heidelberg University
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Andrew Hallam
University of Leeds
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Jad C Halimeh
INO-CNR BEC Center and Department of Physics, Uni Trento, Ludwig Maximilian University of Munich