Specific heat and non-linear susceptibility in spin glasses with random fields
arXiv:1901.01799 · doi:10.1103/PhysRevB.99.014203
Abstract
We study magnetic properties of spin glass SG systems under a random field (RF), beased on the suggestion that RFs can be induced by a weak transverse field in the compound LiHoYF. We consider a cluster spin model that allows long-range disordered interactions among clusters and short-range interactions inside the clusters, besides a local RF for each spin following a Gaussian distribution with standard deviation . We adopt the one-step replica symmetry breaking (RSB) approach to get an exactly solvable single-cluster problem. We discuss the behavior of order parameters, specific heat , nonlinear susceptibility and phase diagrams for different disorder configurations. In the absence of RF, the exhibits a divergence at , while the shows a broad maximum at a temperature around 30 above , as expected for conventional SG systems. The presence of RF changes this scenario. The still shows the maximum at that is weakly dependent on . However, the is displaced to lower temperatures, enhancing considerable the ration . Furthermore, the divergence in is replaced by a rounded maximum at a temperature , which becomes increasingly higher than as enhances. As a consequence, the paramagnetic phase is unfolded in three regions: (i) a conventional paramagnetism (; (ii) a region with formation of short-range order with frozen spins (); (iii) a region with slow growth of free-energy barriers slowing down the spin dynamics before the SG transition () suggesting an intermediate Griffiths phase before the SG state. Our results reproduce qualitatively some findings of LiHoYF as the rounded maximum of behavior triggered by RF.
arXiv comment9 pages, 6 figures
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