2021
DOI: 10.1140/epjb/s10051-021-00081-3
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Kinetic Ising model under sinusoidal oscillating external magnetic field: hysteresis and dynamic phase transition

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Cited by 1 publication
(2 citation statements)
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“…For type-3 curves, hysteresis loops are always symmetric, so coercivity survives for entire frequency spectrum, indicating that the system resides in a dynamic paramagnetic phase. Similar arguments have also been underlined in a recent work by [75]. Besides, using an EFT formulation, influence of quenched bond dilution on the frequency evolutions of hysteresis loop area and hysteresis tools such as remanence and coercivity of a kinetic ferromagnetic Ising model has been reported by Vatansever et al [73] where it has been reported that increasing randomness drives the system from dynamically ordered state to dynamically disordered phase.…”
Section: Dynamic Hysteresis and Scaling Of The Dynamic Loop Areasupporting
confidence: 75%
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“…For type-3 curves, hysteresis loops are always symmetric, so coercivity survives for entire frequency spectrum, indicating that the system resides in a dynamic paramagnetic phase. Similar arguments have also been underlined in a recent work by [75]. Besides, using an EFT formulation, influence of quenched bond dilution on the frequency evolutions of hysteresis loop area and hysteresis tools such as remanence and coercivity of a kinetic ferromagnetic Ising model has been reported by Vatansever et al [73] where it has been reported that increasing randomness drives the system from dynamically ordered state to dynamically disordered phase.…”
Section: Dynamic Hysteresis and Scaling Of The Dynamic Loop Areasupporting
confidence: 75%
“…To be more clear, γ exponents were found as approximately 1.2, 0.5 and 0.5 for the time-dependent Ginzburg-Landau, Glauber and Arrhenius techniques, respectively. (b) The second group is the group that consists of the studies where the effects of thermal fluctuations on the system driven by a time dependent magnetic field are partially or completely taken into account [48,[63][64][65][66][67][68][69][70][71][72][73][74][75][76][77]. It should be underlined that extensive numerical simulations have been undertaken by Acharyya and Chakrabarti for ferromagnetic Ising systems in two to four dimensions to clarify the variations of A with respect to frequency and amplitude of the external field and temperature of the system [78,79].…”
Section: Dynamic Hysteresis and Scaling Of The Dynamic Loop Areamentioning
confidence: 99%