2018
DOI: 10.1088/1367-2630/aaaa27
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Dynamic depinning phase transition in magnetic thin film with anisotropy

Abstract: The dynamic pinning effects induced by quenched disorder are significant in manipulating the domain-wall motion in nano-magnetic materials. Through numerical simulations of the nonstationary domain-wall dynamics with the Landau-Lifshitz-Gilbert equation, we confidently detect a dynamic depinning phase transition in a magnetic thin film with anisotropy, which is of second order. The transition field, static and dynamic exponents are accurately determined, based on the dynamic scaling behavior far from stationar… Show more

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Cited by 10 publications
(13 citation statements)
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“…2b), θ depends on σ: For small but finite σ, θ approaches the qEW value of 0.25, while in the limit of large σ it tends to a value close to 1. We note that recent simulations for a specific disorder strength based on the LLG equation of a Heisenberg-like model found θ > θ qEW [29].…”
mentioning
confidence: 56%
“…2b), θ depends on σ: For small but finite σ, θ approaches the qEW value of 0.25, while in the limit of large σ it tends to a value close to 1. We note that recent simulations for a specific disorder strength based on the LLG equation of a Heisenberg-like model found θ > θ qEW [29].…”
mentioning
confidence: 56%
“…Due to critical slowing down, it is very difficult to simulate the stationary state around the depinning phase transition. The nonstationary dynamic approach looks novel and efficient in tackling the dynamic phase transitions, since the measurements are carried out in the short-time regime of the dynamic evolution [35,[44][45][46][47]. In addition, it may avoid the errors induced by the finite time step Δt in the molecular dynamics simulations of the stationary state.…”
Section: Introductionmentioning
confidence: 99%
“…In the past years, much effort of physicists has been devoted to the understanding of the domain-wall dynamics of ferroic materials (ferroelectrics, ferromagnets, ferroelastics) in both experiments and theories [1][2][3][4][5][6][7][8], due to the possible applications in high-density magnetic memories, spin logic devices, and shift registers by means of switching and detecting the polarization orientations of the domains [9][10][11][12]. The dynamic properties of domain walls in the macroscopic, mesoscopic, and microscopic scales have been investigated with different numerical methods, such as the Edwards-Wilkinson equation with quenched disorder [4,13,14], Monte Carlo method in the Isingtype lattice models [15][16][17][18], and Landau-Lifshitz-Gilbert equation in the Heisenberg-like models [19][20][21][22].…”
Section: Introductionmentioning
confidence: 99%
“…Driven by a constant external field in the presence of the quenched disorder, a pinning-depinning dynamic transition occurs at zero temperature, separating the regimes of static pinning and friction-limited viscous sliding [22][23][24]. At low temperatures, the sharp depinning transition is softened, and a thermally activated creep motion appears [25][26][27][28].…”
Section: Introductionmentioning
confidence: 99%
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