1990
DOI: 10.1063/1.346423
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Domain-wall dynamics and Barkhausen effect in metallic ferromagnetic materials. I. Theory

Abstract: Article] Domain wall dynamics and Barkhausen effect in metallic ferromagnetic materials. I. TheoryOriginal Citation: Alessandro B.; Beatrice C.; Bertotti G.; Montorsi A. (1990). Domain wall dynamics and Barkhausen effect in metallic ferromagnetic materials. I.

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Cited by 323 publications
(235 citation statements)
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“…For example, different scaling functions are obtained for the maximum heights of periodic Gaussian interfaces: if the maximum is measured relative to the spatially averaged height, the corresponding EVS is determined by the so-called Airy distribution function [41][42][43][44], whereas measuring the maximum relative to the boundary value leads to the Rayleigh distribution [50,51]. We will discuss the extreme value distribution for an avalanche in a mean field theory of interface depinning known as the Alessandro-BeatriceBertotti-Montorsi (ABBM) model [52] and will show that this avalanche signal can be viewed as a sequence of strongly-correlated, non-identically distributed, nonGaussian variables. The probability distribution function (PDF) of the maximum velocity inside avalanches of fixed duration T follows a universal scaling form P (v m |T ) = (2v m T ) −1/2 F ( 2v m /T ), with a scaling function F (x) that can be derived exactly by a mapping to an equivalent problem of random excursions of Brownian motion in a logarithmic potential.…”
Section: Quantitiymentioning
confidence: 99%
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“…For example, different scaling functions are obtained for the maximum heights of periodic Gaussian interfaces: if the maximum is measured relative to the spatially averaged height, the corresponding EVS is determined by the so-called Airy distribution function [41][42][43][44], whereas measuring the maximum relative to the boundary value leads to the Rayleigh distribution [50,51]. We will discuss the extreme value distribution for an avalanche in a mean field theory of interface depinning known as the Alessandro-BeatriceBertotti-Montorsi (ABBM) model [52] and will show that this avalanche signal can be viewed as a sequence of strongly-correlated, non-identically distributed, nonGaussian variables. The probability distribution function (PDF) of the maximum velocity inside avalanches of fixed duration T follows a universal scaling form P (v m |T ) = (2v m T ) −1/2 F ( 2v m /T ), with a scaling function F (x) that can be derived exactly by a mapping to an equivalent problem of random excursions of Brownian motion in a logarithmic potential.…”
Section: Quantitiymentioning
confidence: 99%
“…However, Eq. (34) can also be obtained from the exact solutions to the untransformed k = 0 Fokker-Planck equation [52] …”
Section: Velocity Statistics For Avalanches Of Fixed Durationmentioning
confidence: 99%
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“…In recent years, there is an increasing interest in the study of record statistics in the context of global warming and climate change [3], occurrence of cyclones and floods [4] and stock markets. In physics, records statistics is useful in understanding the behavior of stochastic motion of a domain wall in metallic ferromagnetic materials [5] and as an alternative indicator of quantum chaos in kicked rotor model [6]. Even as the record breaking events continue to enjoy media attention, there is also an increased research interest in the statistical study of record events [7][8][9][10][11][12].…”
Section: Introductionmentioning
confidence: 99%