Inverse Transitions in the Ghatak-Sherrington model with Bimodal Random Fields
arXiv:1302.1828 · doi:10.1016/j.physa.2012.12.025
Abstract
The present work studies the Ghatak-Sherrington (GS) model with the presence of a longitudinal magnetic random field (RF) following a bimodal distribution. The model considers a random bond interaction which follows a Gaussian distribution with mean and variance . This allows us to introduce the bond disorder strength parameter to probe the combined effects of disorder coming from the random bond and the discrete RF over unusual phase transitions known as inverse transitions (ITs). The results within a mean field approximation indicate that these two types of disorder have complete distinct roles for the ITs. They indicate that bond disorder creates the necessary conditions for the presence of inverse freezing or even inverse melting depending on the bond disorder strength, while the RF tends to enforce mechanisms that destroy the ITs.
References in corpus (12)
- Inverse melting of the vortex lattice
- Inverse melting and inverse freezing: a spin model
- Spin Model for Inverse Melting and Inverse Glass Transition
- Stable Solution of the Simplest Spin Model for Inverse Freezing
- Simplest model to study reentrance in physical systems
- Thermodynamic first order transition and inverse freezing in a 3D spin-glass
- The random Blume-Capel model on cubic lattice: first order inverse freezing in a 3D spin-glass system
- Role of the transverse field in inverse freezing in the fermionic Ising spin-glass model
- Inverse freezing in the Ghatak-Sherrington model with a random field
- Tricriticality and Reentrance in a Naive Spin-Glass Model
- On exact mappings between fermionic Ising spin glass and classical spin glass models
- Inverse freezing in the Hopfield Fermionic Ising Spin Glass