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Quantum critical behavior at the many-body localization transition

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TLDR
Quantum critical behaviour at the many-body localization transition in a disordered Bose–Hubbard system of bosonic rubidium atoms in an optical lattice is observed, connecting the macroscopic phenomenology of the transition to the system’s microscopic quantum correlations.
Abstract
Phase transitions are driven by collective fluctuations of a system’s constituents that emerge at a critical point1. This mechanism has been extensively explored for classical and quantum systems in equilibrium, whose critical behaviour is described by the general theory of phase transitions. Recently, however, fundamentally distinct phase transitions have been discovered for out-of-equilibrium quantum systems, which can exhibit critical behaviour that defies this description and is not well understood1. A paradigmatic example is the many-body localization (MBL) transition, which marks the breakdown of thermalization in an isolated quantum many-body system as its disorder increases beyond a critical value2–11. Characterizing quantum critical behaviour in an MBL system requires probing its entanglement over space and time4,5,7, which has proved experimentally challenging owing to stringent requirements on quantum state preparation and system isolation. Here we observe quantum critical behaviour at the MBL transition in a disordered Bose–Hubbard system and characterize its entanglement via its multi-point quantum correlations. We observe the emergence of strong correlations, accompanied by the onset of anomalous diffusive transport throughout the system, and verify their critical nature by measuring their dependence on the system size. The correlations extend to high orders in the quantum critical regime and appear to form via a sparse network of many-body resonances that spans the entire system12,13. Our results connect the macroscopic phenomenology of the transition to the system’s microscopic structure of quantum correlations, and they provide an essential step towards understanding criticality and universality in non-equilibrium systems1,7,13.Quantum critical behaviour at the many-body localization transition in a disordered Bose–Hubbard system of bosonic rubidium atoms in an optical lattice is observed, connecting the macroscopic phenomenology of the transition to the system’s microscopic quantum correlations.

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Ergodicity breaking transition in finite disordered spin chains

TL;DR: In this paper, the authors studied the disorder-induced ergodicity breaking transition in high-energy eigenstates of interacting spin-1/2 chains using exact diagonalization.
Journal ArticleDOI

Observation of energy-resolved many-body localization

TL;DR: In this article, an energy-resolved many-body localization with a 19-qubit programmable superconducting processor is studied, where the onset of localization occurs at different disorder strengths, with distinguishable energy scales, by measuring time-evolved observables and quantities related to manybody wave functions.
Journal ArticleDOI

Flat-band many-body localization and ergodicity breaking in the Creutz ladder

TL;DR: In this paper, disorder-free many-body localization in the flat-band Creutz ladder was studied in cold-atoms in an optical lattice with and without interactions, and the level spacing analysis exhibits Poisson-like distribution indicating the existence of disorder free localization.
Journal ArticleDOI

Many-body physics in the NISQ era: quantum programming a discrete time crystal

TL;DR: In this paper, the authors explore the implications of noisy, intermediate scale quantum (NISQ) devices for many-body physics in a practical sense: they ask which physical phenomena, in the domain of quantum statistical mechanics, they may realize more readily than traditional experimental platforms.
References
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Metal–insulator transition in a weakly interacting many-electron system with localized single-particle states

TL;DR: In this paper, it was shown that in the absence of coupling of the electrons to any external bath dc electrical conductivity exactly vanishes as long as the temperature T does not exceed some finite value Tc.
Journal ArticleDOI

From quantum chaos and eigenstate thermalization to statistical mechanics and thermodynamics

TL;DR: The eigenstate thermalization hypothesis (ETH) as discussed by the authors is a natural extension of quantum chaos and random matrix theory (RMT) that allows one to describe thermalization in isolated chaotic systems without invoking the notion of an external bath.
Journal ArticleDOI

Observation of many-body localization of interacting fermions in a quasirandom optical lattice

TL;DR: This experiment experimentally observed this nonergodic evolution for interacting fermions in a one-dimensional quasirandom optical lattice and identified the MBL transition through the relaxation dynamics of an initially prepared charge density wave.
Journal ArticleDOI

Many-body localization phase transition

TL;DR: In this paper, exact diagonalization is used to explore the many-body localization transition in a random-field spin-1/2 chain, showing that this quantum phase transition at nonzero temperature might be showing infinite-randomness scaling with a dynamic critical exponent.
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