2017
DOI: 10.1016/j.jmmm.2016.08.094
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Effects of the random single-ion anisotropy and random magnetic field in the spin-3/2 Blume–Capel model

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Cited by 15 publications
(3 citation statements)
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“…Disordered magnetic systems represent a great challenge in condensed matter physics since their properties are richer and more complex than their pure, non-disordered, counterparts [2]. In particular, multicritical behavior and reentrance phenomena in disordered magnetic systems have been the subject of recent studies [3,4,5,6,7,8,9]. Due to both theoretical and experimental importance some attention has been devoted to models under the presence of random fields [2,10,11].…”
Section: Introductionmentioning
confidence: 99%
“…Disordered magnetic systems represent a great challenge in condensed matter physics since their properties are richer and more complex than their pure, non-disordered, counterparts [2]. In particular, multicritical behavior and reentrance phenomena in disordered magnetic systems have been the subject of recent studies [3,4,5,6,7,8,9]. Due to both theoretical and experimental importance some attention has been devoted to models under the presence of random fields [2,10,11].…”
Section: Introductionmentioning
confidence: 99%
“…This model is very useful for describing disordered systems as long as random single-ion anisotropy [14] is incorporated, random magnetic fields [15][16][17][18], and disorders in the couplings between the spins [19]. Other disordered systems are formed by two sublattices with different spins that are subjected to random single-ion anisotropy [20][21][22][23] and random magnetic field [24].…”
Section: Introductionmentioning
confidence: 99%
“…In some of the works, instead of H the nearest-neighbor bilinear exchange interaction parameter J is considered, for example, the random J model on a honeycomb lattice in the EFT with correlation [25], in a longitudinal random field with crystal field by using the EFT with correlations [26], in the transverse Ising model with the longitudinal random field on a honeycomb lattice within the EFT with correlations [27], on a simple cubic lattice with H and random J and random crystal field effects in the EFT [28] and the random crystal field and random H effects via the Curie-Weiss mean-field approximation [29]. It is found that the randomness included models give much more interesting and richer phase diagrams when compared with the regular models.…”
mentioning
confidence: 99%