2017
DOI: 10.1016/j.spmi.2017.04.004
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Monte Carlo study of a ferrimagnetic mixed-spin (2, 5/2) system with the nearest and next-nearest neighbors exchange couplings

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Cited by 40 publications
(3 citation statements)
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“…We can observe that the compensation temperature appears only when J B =jJ AB j > 0:5 and takes a constant value T comp =jJ AB j ¼ 10:31 for great values of J B =jJ AB j, whereas the critical temperature grows linearly with the increase of J B =jJ AB j. Similar phase diagrams have been obtained in some mixed-spin systems such as in the case of nanowires (Aharrouch et al, 2020;Dakir et al, 2015), nanotube (Mi et al, 2018) and ferrimagnetic systems on honeycomb and square lattices (Deviren et al, 2011;Bi et al, 2017;Nakamura, 2000;Li et al, 2005).…”
Section: Effect Of the Exchange Interaction J Bsupporting
confidence: 68%
“…We can observe that the compensation temperature appears only when J B =jJ AB j > 0:5 and takes a constant value T comp =jJ AB j ¼ 10:31 for great values of J B =jJ AB j, whereas the critical temperature grows linearly with the increase of J B =jJ AB j. Similar phase diagrams have been obtained in some mixed-spin systems such as in the case of nanowires (Aharrouch et al, 2020;Dakir et al, 2015), nanotube (Mi et al, 2018) and ferrimagnetic systems on honeycomb and square lattices (Deviren et al, 2011;Bi et al, 2017;Nakamura, 2000;Li et al, 2005).…”
Section: Effect Of the Exchange Interaction J Bsupporting
confidence: 68%
“…This is due to the fact that the decrease of DB/|JAB| imposes the spins of sublattice (B) to be in a weak spin state, producing the coexistence of several frustrated spin states at low temperature. Moreover, when the temperature increases, the thermal agitation becomes more dominant than the couplings between the spins and the anisotropies, and thus the frustrated spins are released, which shows that the effect of temperature on the curves of the magnetization begins to become more important [36,37]. The results found here are similar to those obtained for mixed spin-1 and spin-2 Heisenberg ferrimagnetic system using the Green's function technique [29], and for mixed-spin (1/2, 5/2) Ising system by MFA and MCS [38].…”
Section: Case Of Ja=jb=0mentioning
confidence: 99%
“…The studies of these systems are related to the experimental researches of molecular-based magnetic materials and nano-graphene films. In particular, a kind of molecular-based ferrimagnets, namely AFe II Fe III (C 2 O 4 ) 3 (A = N( n − C n H 2 n +1 ) 4 , n = 3–5), have been the subject under extensive theoretical discussions of mixed-spin Ising (or transverse Ising) systems, where spins of Fe II and Fe III atoms are respectively taken as 2 and 5/2 and they are coupled by a negative exchange interaction in each layer and two positive interactions between layers (see the references in the recent theoretical works [1,2,3,4]). For nano-graphene films, on the other hand, the magnetic properties of the ferromagnetic and antiferromagnetic two (or three) layers of honeycomb lattices described by the spin-1/2 Ising (or transverse Ising) models have been recently investigated by the use of the EFT [5,6,7].…”
Section: Introductionmentioning
confidence: 99%