Abstract

Recent progress in the realm of noisy, intermediate scale quantum (NISQ) devices represents an exciting opportunity for many-body physics, by introducing new laboratory platforms with unprecedented control and measurement capabilities. We explore the implications of NISQ platforms for many-body physics in a practical sense: we ask which {\it physical phenomena}, in the domain of quantum statistical mechanics, they may realize more readily than traditional experimental platforms. As a particularly well-suited target, we identify discrete time crystals (DTCs), novel non-equilibrium states of matter that break time translation symmetry. These can only be realized in the intrinsically out-of-equilibrium setting of periodically driven quantum systems stabilized by disorder induced many-body localization. While precursors of the DTC have been observed across a variety of experimental platforms - ranging from trapped ions to nitrogen vacancy centers to NMR crystals - none have \emph{all} the necessary ingredients for realizing a fully-fledged incarnation of this phase, and for detecting its signature long-range \emph{spatiotemporal order}. We show that a new generation of quantum simulators can be programmed to realize the DTC phase and to experimentally detect its dynamical properties, a task requiring extensive capabilities for programmability, initialization and read-out. Specifically, the architecture of Google's Sycamore processor is a remarkably close match for the task at hand. We also discuss the effects of environmental decoherence, and how they can be distinguished from `internal' decoherence coming from closed-system thermalization dynamics. Already with existing technology and noise levels, we find that DTC spatiotemporal order would be observable over hundreds of periods, with parametric improvements to come as the hardware advances.

Highlights

  • The quest to build a universal quantum computer has fueled sustained progress towards the development of “designer” many-body quantum systems across a variety of platforms ranging from trapped ions to superconducting qubits [1,2]

  • The discrete time crystals (DTCs) phase develops a plateau for δω → 0 corresponding to a delta-function π peak in the Fourier response, while in the thermal and many-body localized (MBL) PM phases we find that C (π, δω) ∼ δω. (d) Spin glass order parameter χ SG evaluated at late times, nmax/2 ≤ n ≤ nmax, from dynamics simulations as in (a)

  • In this work we have considered the question: what does the dawning age of noisy intermediate-scale quantum (NISQ) devices and programmable quantum simulators have in store for quantum many-body physics? We have observed that, while these devices offer universal gate sets that can in principle simulate any quantum system, their limitation in coherence time practically favors certain simulation targets over others in the near term

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Summary

INTRODUCTION

The quest to build a universal quantum computer has fueled sustained progress towards the development of “designer” many-body quantum systems across a variety of platforms ranging from trapped ions to superconducting qubits [1,2]. (i) The natural time evolutions implemented on digital gate-based programmable simulators (such as Sycamore) are quantum circuits rather than Hamiltonians This is quite far from the typical setting in which condensed matter theory operates, which concerns the low-energy, long-wavelength emergent properties of equilibrium many-body systems. For these applications, randomness in circuit elements is tolerated, but is necessary to stabilize the system against heating, and for observing interesting phenomena For these reasons, in this work we propose precisely such a ‘physicsforward” use of the Sycamore device and its relatives: to realize a MBL Floquet DTC, a nonequilibrium manybody phase of matter that displays an entirely new form of spatiotemporal order [19,20,21].

THE DISCRETE TIME CRYSTAL
The DTC and its import
Model realizations
First generation DTC experiments
Experimental checklist
Basic definitional requirements
Requirements for stabilizing MBL
Requirements for detection
NEXT GENERATION
Floquet DTC circuit on Sycamore
Diagnostics of the MBL DTC phase
EFFECT OF NOISE
Summary
Directions for future research
Control errors and decoherence
Findings
Measurement error
Full Text
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