2007
DOI: 10.1103/physrevlett.98.267002
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Depinning and Creep Motion in Glass States of Flux Lines

Abstract: Using dynamical computer simulation, we investigate vortex matter in glass states. A genuine continuous depinning transition is observed at zero temperature, which also governs the low-temperature creep motion. With the notion of scaling, we evaluate in high accuracy critical exponents and scaling functions; we observe a non-Arrhenius creep motion for weak collective pinning where the Bragg glass is stabilized at equilibrium, while for strong pinning, the well-known Arrhenius law is recovered. In both cases, a… Show more

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Cited by 64 publications
(96 citation statements)
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References 40 publications
(64 reference statements)
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“…The naive analogy with standard phase transitions (e.g., magnetization vs temperature with an external magnetic field in the Ising model), thinking of V as the order parameter and H as the control parameter, suggests that V ∼ T ψ at H = H c , with ψ being a universal thermal rounding exponent. [30][31][32][33][34][35][36][37] Although the very existence and universality of such a power law has not been rigorously proven for the depinning transition, it is consistent with recent numerical simulations. 33,[35][36][37] Furthermore, based on this analogy with standard phase transitions one can argue that the order parameter is a homogeneous function of the external parameters.…”
Section: Introductionsupporting
confidence: 83%
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“…The naive analogy with standard phase transitions (e.g., magnetization vs temperature with an external magnetic field in the Ising model), thinking of V as the order parameter and H as the control parameter, suggests that V ∼ T ψ at H = H c , with ψ being a universal thermal rounding exponent. [30][31][32][33][34][35][36][37] Although the very existence and universality of such a power law has not been rigorously proven for the depinning transition, it is consistent with recent numerical simulations. 33,[35][36][37] Furthermore, based on this analogy with standard phase transitions one can argue that the order parameter is a homogeneous function of the external parameters.…”
Section: Introductionsupporting
confidence: 83%
“…This scaling behavior is expected to hold close to the critical point, i.e., for H − H c H c and T → 0. Although this scaling form has been successfully tested in numerical simulations, 33,35,37 it has not yet been experimentally probed.…”
Section: Introductionmentioning
confidence: 99%
“…On the other hand, at forces around the critical value, F ≈ F c , a finite temperature value smears out the transition, which is no longer abrupt. This thermal rounding of the depinning transition can be characterized, exactly at the critical force F = F c , by a power-law vanishing of the velocity with the temperature as V ∼ T ψ , with ψ the thermal rounding exponent [24][25][26][27][28][29][30].…”
Section: Introductionmentioning
confidence: 99%
“…Finalement, notons que les mesuresà température non nulle confirment notre résultat β = 0.27 ± 0.04. Notonségalement qu'un travail précédent sur les vortex dans les supraconducteurs en dimension d = 3 [14] trouvait un exposant β = 0.65 ± 0.01.…”
Section: Dépiégeageélastique : Résultatsunclassified