Adiabatic dynamics of an inhomogeneous quantum phase transition: the case of z > 1 dynamical exponent

TL;DR

This paper studies the adiabatic dynamics of inhomogeneous quantum phase transitions with a dynamical exponent z > 1, revealing a nonzero threshold velocity for excitation suppression and implications for efficient quantum state preparation.

Contribution

It extends the understanding of inhomogeneous quantum phase transitions to the case z > 1, showing a nonzero adiabatic threshold velocity and its effects on excitation suppression and quantum state preparation.

Findings

Excitations are exponentially suppressed below a threshold velocity v'

The adiabatic transition time scales linearly with system size N

Post-transition excitations are swept to the chain end by the critical front

Abstract

We consider an inhomogeneous quantum phase transition across a multicritical point of the XY quantum spin chain. This is an example of a Lifshitz transition with a dynamical exponent z = 2. Just like in the case z = 1 considered in New J. Phys. 12, 055007 (2010) when a critical front propagates much faster than the maximal group velocity of quasiparticles vq, then the transition is effectively homogeneous: density of excitations obeys a generalized Kibble-Zurek mechanism and scales with the sixth root of the transition rate. However, unlike for z = 1, the inhomogeneous transition becomes adiabatic not below vq but a lower threshold velocity v', proportional to inhomogeneity of the transition, where the excitations are suppressed exponentially. Interestingly, the adiabatic threshold v' is nonzero despite vanishing minimal group velocity of low energy quasiparticles. In the adiabatic regime below v' the inhomogeneous transition can be used for efficient adiabatic quantum state preparation in a quantum simulator: the time required for the critical front to sweep across a chain of N spins adiabatically is merely linear in N, while the corresponding time for a homogeneous transition across the multicritical point scales with the sixth power of N. What is more, excitations after the adiabatic inhomogeneous transition, if any, are brushed away by the critical front to the end of the spin chain.