Sachdev–Ye–Kitaev model

In condensed matter physics and black hole physics, the Sachdev–Ye–Kitaev (SYK) model (commonly known as SYK model) is an exactly solvable model initially proposed by Subir Sachdev and Jinwu Ye, and later modified by Alexei Kitaev to the present commonly used form. The model is believed to bring insights into the understanding of strongly correlated materials and it also has a close relation with the discrete model of AdS/CFT, and fermionic code. Many condensed matter systems, such as quantum dot coupled to topological superconducting wires, graphene flake with irregular boundary, and kagome optical lattice with impurities, are proposed to be modeled by it. Some variants of the model is amenable to digital quantum simulation, with pioneering experiments implemented in a NMR setting.

Model

Let $n$ be an integer and $m$ an even integer such that $2\leq m\leq n$, and consider a set of Majorana fermions $\psi _{1},\dotsc ,\psi _{n}$ which are fermion operators satisfying conditions:

1. Hermitian $\psi _{i}^{\dagger }=\psi _{i}$;
2. Clifford relation $\{\psi _{i},\psi _{j}\}=2\delta _{ij}$.

Let $J_{i_{1}i_{2}\cdots i_{m}}$ be random variables whose expectations satisfy:

1. $\mathbf {E} (J_{i_{1}i_{2}\cdots i_{m}})=0$;
2. $\mathbf {E} (J_{i_{1}i_{2}\cdots i_{m}}^{2})=1$.

Then the SYK model is defined as

$H_{\rm {SYK}}=i^{m/2}\sum _{1\leq i_{1}<\cdots <i_{m\leq n}}J_{i_{1}i_{2}\cdots i_{m}}\psi _{i_{1}}\psi _{i_{2}}\cdots \psi _{i_{m}}$.

Note that sometimes an extra normalization factor is included.

The most famous model is when $m=4$:

$H_{\rm {SYK}}=-{\frac {1}{4!}}\sum _{i_{1},\dotsc ,i_{4}=1}^{n}J_{i_{1}i_{2}i_{3}i_{4}}\psi _{i_{1}}\psi _{i_{2}}\psi _{i_{3}}\psi _{i_{4}}$,

where the factor $1/4!$ is included to coincide with the most popular form.

See also

• Non-Fermi liquid