Abstract

The extension of many-body quantum dynamics to the non-unitary domain has led to a series of exciting developments, including new out-of-equilibrium entanglement phases and phase transitions. We show how a duality transformation between space and time on one hand, and unitarity and non-unitarity on the other, can be used to realize steady state phases of non-unitary dynamics that exhibit a rich variety of behavior in their entanglement scaling with subsystem size -- from logarithmic to extensive to \emph{fractal}. We show how these outcomes in non-unitary circuits (that are "spacetime-dual" to unitary circuits) relate to the growth of entanglement in time in the corresponding unitary circuits, and how they differ, through an exact mapping to a problem of unitary evolution with boundary decoherence, in which information gets "radiated away" from one edge of the system. In spacetime-duals of chaotic unitary circuits, this mapping allows us to uncover a non-thermal volume-law entangled phase with a logarithmic correction to the entropy distinct from other known examples. Most notably, we also find novel steady state phases with \emph{fractal} entanglement scaling, $S(\ell) \sim \ell^{\alpha}$ with tunable $0 < \alpha < 1$ for subsystems of size $\ell$ in one dimension. These fractally entangled states add a qualitatively new entry to the families of many-body quantum states that have been studied as energy eigenstates or dynamical steady states, whose entropy almost always displays either area-law, volume-law or logarithmic scaling. We also present an experimental protocol for preparing these novel steady states with only a very limited amount of postselection via a type of "teleportation" between spacelike and timelike slices of quantum circuits.

Highlights

  • Breakthrough experimental advances in building quantum simulators have opened up new regimes in the study of many-body physics, by providing direct access to the dynamics of quantum systems

  • We have explored entanglement in nonunitary circuits that are spacetime duals of local unitary circuits [30]

  • Focusing on this class of nonunitary circuits has allowed us to translate the rich variety in entanglement growth displayed by unitary circuits into an rich variety of steady-state phases produced by nonunitary dynamics

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Summary

INTRODUCTION

Breakthrough experimental advances in building quantum simulators have opened up new regimes in the study of many-body physics, by providing direct access to the dynamics of quantum systems. Quantum simulators [15], which naturally include nonunitary ingredients in two ways: on the one hand, by the presence of (uncontrolled) environmental noise and decoherence; on the other, by allowing controlled quantum measurements during the dynamics (a key capability for error correction in future “fault-tolerant” quantum computers) In both unitary and nonunitary cases, both the growth of entanglement in time, as well as its spatial scaling, may show interesting structure, including sharp phase transitions between distinct behaviors. As a fractional, tunable power law of subsystem size (in one dimension) and is statistically self-similar over all length scales These fractally entangled steady states are generically not obtained as either eigenstates or dynamical steady states in any unitary setting and represent a striking example of new, robust nonequilibrium phenomena made possible by adding nonunitarity to the toolkit of many-body quantum dynamics.

Nonunitary dynamics from spacetime duality
Mapping to boundary decoherence
Models of unitary dynamics
LOGARITHMICALLY ENTANGLED STEADY STATES
NONTHERMAL VOLUME-LAW ENTANGLED STEADY STATES
Griffiths circuit model
Fractal entanglement
Robustness to breaking of unitarity
SUMMARY AND OUTLOOK
Uniqueness of the steady state under edge decoherence
Normalization of the wave function
Entanglement calculation
Impossibility of area-law steady states

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