Dynamics of position disordered Ising spins with a soft-core potential

TL;DR

This paper investigates the relaxation dynamics of disordered Ising spins with a soft-core interaction, deriving analytical solutions and numerical results that reveal how disorder and interaction range influence magnetization decay.

Contribution

It provides a theoretical analysis of magnetization relaxation in disordered Ising systems with soft-core interactions, including analytical expressions and numerical insights into different disorder regimes.

Findings

Homogeneous case exhibits exponential and stretched-exponential relaxation with exponent d/α.

Disorder affects dynamics, with coherent behavior at high density and different stretched exponent (~0.18) in dilute regimes.

Analytical and numerical results show how disorder and interaction range influence relaxation behavior.

Abstract

We theoretically study magnetization relaxation of Ising spins distributed randomly in a $d$-dimension homogeneous and Gaussian profile under a soft-core two-body interaction potential $\propto1/[1+(r/R_c)^\alpha]$ ($\alpha\ge d$), where $r$ is the inter-spin distance and $R_c$ is the soft-core radius. The dynamics starts with all spins polarized in the transverse direction. In the homogeneous case, an analytic expression is derived at the thermodynamic limit, which starts as $\propto\exp(-t^2)$ and follows a stretched-exponential law asymptotically at long time with an exponent $\beta=d/\alpha$. In between an oscillating behaviour is observed with a damping amplitude. For Gaussian samples, the degree of disorder in the system can be controlled by the ratio $l_\rho/R_c$ with $l_\rho$ the mean inter-spin distance and the magnetization dynamics is investigated numerically. In the limit of $l_\rho/R_c\ll1$, a coherent many-body dynamics is recovered for the total magnetization despite of the position disorder of spins. In the opposite limit of $l_\rho/R_c\gg1$, a similar dynamics as that in the homogeneous case emerges at later time after a initial fast decay of the magnetization. We obtain a stretched exponent of $\beta\approx0.18$ for the asymptotic evolution with $d=3, \alpha=6$, which is different from that in the homogeneous case ($\beta=0.5$).