Abstract

System of Majorana zero modes with random infinite range interactions -- the Sachdev-Ye-Kitaev (SYK) model -- is thought to exhibit an intriguing relation to the horizons of extremal black holes in two-dimensional anti-de Sitter (AdS$_2$) space. This connection provides a rare example of holographic duality between a solvable quantum-mechanical model and dilaton gravity. Here we propose a physical realization of the SYK model in a solid state system. The proposed setup employs the Fu-Kane superconductor realized at the interface between a three dimensional topological insulator (TI) and an ordinary superconductor. The requisite $N$ Majorana zero modes are bound to a nanoscale hole fabricated in the superconductor that is threaded by $N$ quanta of magnetic flux. We show that when the system is tuned to the surface neutrality point (i.e. chemical potential coincident with the Dirac point of the TI surface state) and the hole has sufficiently irregular shape, the Majorana zero modes are described by the SYK Hamiltonian. We perform extensive numerical simulations to demonstrate that the system indeed exhibits physical properties expected of the SYK model, including thermodynamic quantities and two-point as well as four-point correlators, and discuss ways in which these can be observed experimentally.

Highlights

  • Models of particles with infinite-range interactions have a long history in nuclear physics dating back to the pioneering works of Wigner [1] and Dyson [2] and in condensed matter physics in studies describing spin glass and spin liquid states of matter [3,4,5]

  • We find the wave functions of the Majorana zero modes by numerically diagonalizing the corresponding Bogoliubov–de Gennes (BdG) Hamiltonian for the geometry depicted in Fig. 1 with N flux quanta threading the hole

  • The resulting many-body spectra and eigenvectors are used to calculate various physical quantities, which are compared to the results previously obtained for the SYK model with random independent couplings

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Summary

Introduction

Models of particles with infinite-range interactions have a long history in nuclear physics dating back to the pioneering works of Wigner [1] and Dyson [2] and in condensed matter physics in studies describing spin glass and spin liquid states of matter [3,4,5]. Kitaev [6] and Maldacena and Stanford [7] formulated and studied a Majorana fermion version of the model with all-to-all random interactions first proposed by Sachdev and Ye [4]. The resulting Sachdev-Ye-Kitaev (SYK) model, defined by the Hamiltonian Eq (1.1), is solvable in the limit of large number N of fermions and exhibits a host of intriguing properties.

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