2012
DOI: 10.1088/1751-8113/45/11/115001
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Universality class of the depinning transition in the two-dimensional Ising model with quenched disorder

Abstract: With Monte Carlo methods, we investigate the universality class of the depinning transition in the two-dimensional Ising model with quenched random fields. Based on the short-time dynamic approach, we accurately determine the depinning transition field and both static and dynamic critical exponents. The critical exponents vary significantly with the form and strength of the random fields, but exhibit independence on the updating schemes of the Monte Carlo algorithm. From the roughness exponents ζ, ζ loc and ζ … Show more

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Cited by 14 publications
(30 citation statements)
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“…states of quiescence alternated with avalanches, before reaching the phase state of moving or pinning. Until today, theoretical approaches to explain the depinning transition of the MDW into disordered medium pushed by an external magnetic field, are based on: (a) the continuous equation of Edwards-Wilkinson with quenched noise (QEW) [29][30][31][32] and (b) discrete models based on microscopic structures and interactions, such as random-field Ising field model with driving (DRFIM) [33][34][35][36][37].…”
Section: Introductionmentioning
confidence: 99%
“…states of quiescence alternated with avalanches, before reaching the phase state of moving or pinning. Until today, theoretical approaches to explain the depinning transition of the MDW into disordered medium pushed by an external magnetic field, are based on: (a) the continuous equation of Edwards-Wilkinson with quenched noise (QEW) [29][30][31][32] and (b) discrete models based on microscopic structures and interactions, such as random-field Ising field model with driving (DRFIM) [33][34][35][36][37].…”
Section: Introductionmentioning
confidence: 99%
“…If the latter is correct and general, this would mean that critically pinned interfaces in 2-d isotropic media are always in the universality class of OP. This had been conjectured before [19], but the opposite was claimed in many, even very recent, papers [12][13][14][15][16][20][21][22][23][24][25][26][27] In most of these papers [12-16, 20, 26-28] it is claimed that the percolation scenario breaks down when the disorder is weak. But in others [23][24][25], even in the percolation like phase the critical exponents were found to be different.…”
mentioning
confidence: 99%
“…S(k, t, ǫ = 0, L) is plotted against q for the pure case. Different curves correspond to exponentially increasing times (t = 2,3,5,7,11,18, 29, 46, 73, 118, 189, 304, 490, 789, 1269, 2044, 3291, 5299, 8532, 13739, 22123, 35623, 57362, 92368, 148736, 239503, 385663, 621017, 10 6 from bottom to top)…”
mentioning
confidence: 99%