2001
DOI: 10.1016/s0304-8853(00)00749-6
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Hysteresis and avalanches: phase transitions and critical phenomena in driven disordered systems

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Cited by 24 publications
(15 citation statements)
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“…While the AE and elastic three-point-bending experiments 20 have been instrumental in defining jerky interfacial behavior, both methods fail to generate a full picture of the front propagation, namely the coexistence of smooth fronts and jerks, and thermally activated movement and athermal avalanches. In magnetic systems, Barkhausen noise shows a similar characteristic 21 .…”
Section: Introductionmentioning
confidence: 91%
“…While the AE and elastic three-point-bending experiments 20 have been instrumental in defining jerky interfacial behavior, both methods fail to generate a full picture of the front propagation, namely the coexistence of smooth fronts and jerks, and thermally activated movement and athermal avalanches. In magnetic systems, Barkhausen noise shows a similar characteristic 21 .…”
Section: Introductionmentioning
confidence: 91%
“…Two scaling parameters can be predicted from this model, firstly the size of the avalanches D(S) $ S À and the correlation between the avalanche and the avalanche duration T $ S Àz . The value for these exponents for the three most important classes of solutions [90,91] is as follow: ¼ 1.6 (short range), 1.28 (front propagation) and 1.5 (mean field); z ¼ 0.58 (short range), 0.58 (front propagation) and 0.5 (mean field).…”
Section: Phase Transitions 663mentioning
confidence: 99%
“…In order to model and explain the Barkhausen noise that emerges when the ferromagnetic sample is driven by varying external magnetic field, a number of theoretical models were developed [24][25][26][27][28][29][30][31][32][33][34]. One of the most prominent appears to be the random field Ising model (RFIM), that has been extensively studied in the past few decades [35][36][37][38][39][40][41].…”
Section: Introductionmentioning
confidence: 99%