Abstract

It has been recently proposed by Maldacena and Qi that an eternal traversable wormhole in a two-dimensional anti--de Sitter space is the gravity dual of the low temperature limit of two Sachdev-Ye-Kitaev (SYK) models coupled by a relevant interaction (which we will refer to as spin operator). We study spectral and eigenstate properties of this coupled SYK model. We find that level statistics in the tail of the spectrum, and for a sufficiently weak coupling, show substantial deviations from random matrix theory, which suggests that traversable wormholes are not quantum chaotic. By contrast, for sufficiently strong coupling, corresponding to the black hole phase, level statistics are well described by random matrix theory. This transition in level statistics coincides approximately with a previously reported Hawking-Page transition for weak coupling. We show explicitly that this thermodynamic transition turns into a sharp crossover as the coupling increases. Likewise, this critical coupling also corresponds to the one at which the overlap between the ground state and the thermofield double state (TFD) is smallest. In the range of sizes we can reach by exact diagonalization, the ground state is well approximated by the TFD only in the strong coupling limit. This is due to the fact that the ground state is close to the eigenstate of the spin operator corresponding to the lowest eigenvalue which is an exact TFD at infinite temperature. In this region, the spectral density is separated into blobs centered around the eigenvalues of the spin operator. For weaker couplings, the exponential decay of coefficients in a tensor product basis, typical of the TFD, becomes power law. Finally, we also find that the total Hamiltonian has an additional discrete symmetry which has not been reported previously.

Highlights

  • The dynamics of quantum many-body systems is very rich and, in general, highly dependent of the details of both initial conditions and the Hamiltonian that governs its time evolution

  • We have studied a coupled two-site SYK model whose gravity dual is conjectured to be [39] a traversable wormhole geometry in the low temperature, small coupling, limit and dual to a black hole geometry for sufficiently strong coupling or high temperature

  • In this paper we have found that except in the limit of strong coupling between the two SYK models, a thermofield double state (TFD) is never a good approximation of the ground state for the number of Majoranas (N ≤ 34) that we can investigate by exact diagonalization

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Summary

INTRODUCTION

The dynamics of quantum many-body systems is very rich and, in general, highly dependent of the details of both initial conditions and the Hamiltonian that governs its time evolution. Universal bound which is saturated for field theories with a gravity dual Later this feature was observed [9,10] in the strong coupling limit of the Sachdev-Ye-Kitaev (SYK) model [9,11,12,13,14,15,16,17,18,19,20], a zero-dimensional fermionic model with infinite-range random interactions. We aim to investigate the longtime dynamics of this two-site coupled SYK model by level statistics in order to clarify whether quantum chaos and random matrix theory are generic in quantum gravity backgrounds or are restricted to black holes. VI, devoted to outlook and conclusions, we speculate that the termination of the observed transition at strong coupling is reminiscent of a GrossWitten transition [51], induced by the gradual reduction of the effect of interactions by increasing the coupling between the two SYK models

THE MODEL AND ITS SYMMETRIES
S mod 4 symmetry Let us define the spin operator S as
COMPARISON OF THE TFD WITH THE GROUND STATE
THERMODYNAMIC PROPERTIES
Numerical study
Solution of Schwinger-Dyson equations
LEVEL STATISTICS
Small k
Critical k
OUTLOOK AND CONCLUSIONS
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