2015
DOI: 10.1016/j.physb.2015.04.032
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Dynamic phase transition properties for the mixed spin-(1/2, 1) Ising model in an oscillating magnetic field

Abstract: a b s t r a c tHerein we study the dynamic phase transition properties for the mixed spin-(1/2, 1) Ising model on a square lattice under a time-dependent magnetic field by means of the effective-field theory (EFT) with correlations based on Glauber dynamics. We present the dynamic phase diagrams in the reduced magnetic field amplitude and reduced temperature plane and find that the phase diagrams exhibit dynamic tricitical behavior, multicritical and zero-temperature critical points as well as reentrant behavi… Show more

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Cited by 36 publications
(5 citation statements)
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References 90 publications
(125 reference statements)
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“…For bigger negative values of J BB , namely J BB = 3.65 , the DPD is similar to Figure 4d except the i 3 phase emerges instead of the i 1 phase and the compensation temperature line disappeared, illustrated in Figure 4e, J AA = 1.25 , d = 0.3 . Similar DPDs with Figure 4a were reported in the mixed spin (1/2, 1), [ 73 ] (1, 3/2), [ 74 ] and (1, 2) [ 72 ] IFS, and the similar DPD with Figure 4b were observed in the mixed spin (1/2, 1), [ 69,73,75–77 ] (1, 3/2), [ 78 ] (1, 2), [ 72 ] and (2, 5/2) [ 38,40,48 ] IFS. Moreover, qualitatively similar DPDs with Figure 4c–e were found in the mixed‐spin (1, 2) IFS, [ 72 ] and a similar DPD with Figure 4c were reported in the mixed‐spin (1, 3/2) IFS [ 79 ] ther hand, some of the first‐order phase transition lines, which might be artifact of the DMFA, were observed in the mixed spin (2, 5/2) bilayer system by the DMFA, [ 43 ] but are not observed by the PPM, compare Figure 4 and 5 in ref.…”
Section: Numerical Results and Discussionsupporting
confidence: 87%
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“…For bigger negative values of J BB , namely J BB = 3.65 , the DPD is similar to Figure 4d except the i 3 phase emerges instead of the i 1 phase and the compensation temperature line disappeared, illustrated in Figure 4e, J AA = 1.25 , d = 0.3 . Similar DPDs with Figure 4a were reported in the mixed spin (1/2, 1), [ 73 ] (1, 3/2), [ 74 ] and (1, 2) [ 72 ] IFS, and the similar DPD with Figure 4b were observed in the mixed spin (1/2, 1), [ 69,73,75–77 ] (1, 3/2), [ 78 ] (1, 2), [ 72 ] and (2, 5/2) [ 38,40,48 ] IFS. Moreover, qualitatively similar DPDs with Figure 4c–e were found in the mixed‐spin (1, 2) IFS, [ 72 ] and a similar DPD with Figure 4c were reported in the mixed‐spin (1, 3/2) IFS [ 79 ] ther hand, some of the first‐order phase transition lines, which might be artifact of the DMFA, were observed in the mixed spin (2, 5/2) bilayer system by the DMFA, [ 43 ] but are not observed by the PPM, compare Figure 4 and 5 in ref.…”
Section: Numerical Results and Discussionsupporting
confidence: 87%
“…In numerical calculations, we took the intersublattice interaction is antiferromagnetic, i.e., J AB = 1.0 , because it gives more riches and interesting dynamic critical behaviors. [ 38,41,43,49,69–73 ] We fixed k 1 = 1.0 and k 2 = 2.0 in all numerical calculation because most systems have greater relaxation durations for the translation and shorter relaxation times for rotation and ω was taken as ω = 2 π .…”
Section: Numerical Results and Discussionmentioning
confidence: 99%
“…The effective field theory has been used to study the critical phenomena in a mixed spin-1 and spin-2 Ising model on honeycomb [17] and the dynamic phase transition properties for the mixed spin-(1/2, 1) Ising model on a square lattice [28] as well as two nanoscaled thin films with dilution at the surfaces [29]. This work was motivated by the research done by Girovsky, Jan et al [30].…”
Section: Introductionmentioning
confidence: 99%
“…The phase transition and dynamic critical temperature of the system were discussed in detail [28]. Moreover, unique dynamic magnetic properties were discovered in other mixed-spin systems in the time-dependent magnetic field [29][30][31][32].…”
Section: Introductionmentioning
confidence: 99%