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In disordered elastic systems, driven by displacing a parabolic confining potential adiabatically slowly, all advance of the system is in bursts, termed avalanches.
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H. Barkhausen, · 1919
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Interface fluctuations in disordered systems: 5 − ε 5-\varepsilon expansion
D.S. Fisher, · 1964
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Asymptotic uniqueness of the sliding state for charge-density waves
AA. Middleton, · 1992
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Dynamics of interface depinning in a disordered medium
T. Nattermann, S. Stepanow, L.-H. Tang and H. Leschhorn, · 1992
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Critical behavior of sliding charge-density waves in 4-epsilon dimensions
O. Narayan and D.S. Fisher, · 1992
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D.S. Fisher, · 1998
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Scaling exponents for Barkhausen avalanches in polycrystalline and amorphous ferromagnets
G. Durin and S. Zapperi, · 2000
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P. Chauve, P. Le Doussal and K.J. Wiese, · 2001
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2-loop functional renormalization group analysis of the depinning transition
P. Le Doussal, K.J. Wiese and P. Chauve, · 2002
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Evolution of the average avalanche shape with the universality class
L. Laurson, X. Illa, S. Santucci, K.T. Tallakstad, K.J. Måløy and M.J. Alava, · 2013
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P. Le Doussal and K.J. Wiese, · 2013
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Universality in the mean spatial shape of avalanches
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Distribution of joint local and total size and of extension for avalanches in the Brownian force model
M. Delorme, P. Le Doussal and K.J. Wiese, · 2016
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Spatiotemporal patterns in ultraslow domain wall creep dynamics
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