Abstract

We compute the full probability distribution of the spectral form factor in the self-dual kicked Ising model by providing an exact lower bound for each moment and verifying numerically that the latter is saturated. We show that at large enough times the probability distribution agrees exactly with the prediction of Random Matrix Theory if one identifies the appropriate ensemble of random matrices. We find that this ensemble is not the circular orthogonal one - composed of symmetric random unitary matrices and associated with time-reversal-invariant evolution operators - but is an ensemble of random matrices on a more restricted symmetric space (depending on the parity of the number of sites this space is either ${Sp(N)/U(N)}$ or ${O(2N)/{O(N)\!\times\!O(N)}}$). Even if the latter ensembles yield the same averaged spectral form factor as the circular orthogonal ensemble they show substantially enhanced fluctuations. This behaviour is due to a recently identified additional anti-unitary symmetry of the self-dual kicked Ising model.

Highlights

  • The quantum chaos conjecture [1,2,3] states that a quantum system is chaotic if the correlations of its energy levels have the same structure as those of random Hermitian matrices [4,5]

  • This conjecture originates from studies on singleparticle quantum systems where the aforementioned property can be connected to the conventional chaoticity of the system in the classical limit [6,7,8,9,10,11]

  • For quantum many-body systems with no well-defined classical limit the quantum chaos conjecture can be taken as a definition of quantum chaos

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Summary

INTRODUCTION

The quantum chaos conjecture [1,2,3] states that a quantum system is chaotic if the correlations of its energy levels have the same structure as those of random Hermitian matrices [4,5] This conjecture originates from studies on singleparticle quantum systems where the aforementioned property can be connected to the conventional chaoticity of the system (i.e., sensitivity of the system’s trajectories to initial conditions) in the classical limit [6,7,8,9,10,11]. [22] provided an exact result for the spectral form factor in the self-dual kicked Ising model: A system of spin-1/2 variables which are interacting locally with an Ising Hamiltonian and are periodically kicked by a longitudinal magnetic field. The Appendix reports some details on the spectrum of the spacetransfer matrix for short (finite) times

THE MODEL
PREDICTION OF RANDOM-MATRIX THEORY
Symmetries of the time-evolution operator
L even
Relevant random-matrix ensembles
Thermodynamic limit of the moments
Transfer matrix in space
Higher moments of the spectral form factor
MONTE CARLO SIMULATIONS
CONCLUSIONS
Full Text
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