2019
DOI: 10.1016/j.spmi.2019.106224
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Magnetization and compensation behaviors in a mixed spins (7/2, 1) anti-ferrimagnetic ovalene nano-structure

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Cited by 46 publications
(8 citation statements)
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“…However, comparing the two figures, we can see that the coercivity and the hysteresis loop area are less responsive to d σ variation than to d S one. A similar result is obtained in antiferrimagnetic ovalene nano-structure 42 The temperature influence on the hysteresis behavior of the sublattices as well as the whole system are seen in Fig. 13.…”
supporting
confidence: 78%
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“…However, comparing the two figures, we can see that the coercivity and the hysteresis loop area are less responsive to d σ variation than to d S one. A similar result is obtained in antiferrimagnetic ovalene nano-structure 42 The temperature influence on the hysteresis behavior of the sublattices as well as the whole system are seen in Fig. 13.…”
supporting
confidence: 78%
“…The first two correspond to the compensation temperatures (t = 1.3 and 3.6) as in Ref. 42, while the third one (t = 6.5) is the blocking temperature (t B = T B /J σ ), at which the system undergoes a second order phase transition to the superparamagnetic phase. It is worth noting that t B is not a critical point in the sense that the system does switch from an ordered ((M ≠ 0.0)) to a disordered state (M = 0.0).…”
Section: Resultsmentioning
confidence: 98%
“…In [46], the dilution effects on compensation temperature in nanotrilayer graphene structure were studied through MC simulation and it has been found that with reduction in dilution probability, compensation temperature, increases in an ABA system and decreases in BAB systems. In [47], by the MC approach, the appearance of two compensation temperatures is reported in a mixed spin (7/2, 1) antiferromagnetic ovalene nanostructures. It was observed by MC simulation [48], in Blume Capel model of a bilayer graphene structure with Ruderman-Kittel-Kasuya-Yosida (RKKY) interactions, the transition temperature increases with decrease in the number of nonmagnetic layers.…”
Section: Introductionmentioning
confidence: 98%
“…Through MC simulation it is shown in [40], with reduction in dilution probability, compensation temperature, increases in an ABA system and decreases in BAB systems, in nanotrilayer graphene structure. In [41], by the MC simulational approach, existence of two compensation temperatures in a mixed spin (7/2, 1) antiferromagnetic ovalene nanostructures is reported. In Blume Capel model (S = 1) of a bilayer graphene structure with Ruderman-Kittel-Kasuya-Yosida (RKKY) interactions, it was observed by MC simulation, in [42], the transition temperature increases with decrease in the number of nonmagnetic layers.…”
Section: Introductionmentioning
confidence: 99%