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      Dynamics of a ferromagnetic domain wall: avalanches, depinning transition and the Barkhausen effect

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          Abstract

          We study the dynamics of a ferromagnetic domain wall driven by an external magnetic field through a disordered medium. The avalanche-like motion of the domain walls between pinned configurations produces a noise known as the Barkhausen effect. We discuss experimental results on soft ferromagnetic materials, with reference to the domain structure and the sample geometry, and report Barkhausen noise measurements on Fe\(_{21}\)Co\(_{64}\)B\(_{15}\) amorphous alloy. We construct an equation of motion for a flexible domain wall, which displays a depinning transition as the field is increased. The long-range dipolar interactions are shown to set the upper critical dimension to \(d_c=3\), which implies that mean-field exponents (with possible logarithmic correction) are expected to describe the Barkhausen effect. We introduce a mean-field infinite-range model and show that it is equivalent to a previously introduced single-degree-of-freedom model, known to reproduce several experimental results. We numerically simulate the equation in \(d=3\), confirming the theoretical predictions. We compute the avalanche distributions as a function of the field driving rate and the intensity of the demagnetizing field. The scaling exponents change linearly with the driving rate, while the cutoff of the distribution is determined by the demagnetizing field, in remarkable agreement with experiments.

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          Phase organization

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            Sliding charge-density waves as a dynamic critical phenomenon

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              Hysteresis and hierarchies: dynamics of disorder-driven first-order phase transformations

              We use the zero-temperature random-field Ising model to study hysteretic behavior at first-order phase transitions. Sweeping the external field through zero, the model exhibits hysteresis, the return-point memory effect, and avalanche fluctuations. There is a critical value of disorder at which a jump in the magnetization (corresponding to an infinite avalanche) first occurs. We study the universal behavior at this critical point using mean-field theory, and also present preliminary results of numerical simulations in three dimensions.
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                Author and article information

                Journal
                20 March 1998
                Article
                10.1103/PhysRevB.58.6353
                cond-mat/9803253
                de71ad7a-7166-4858-afd5-31e0c33a8538
                History
                Custom metadata
                17 RevTeX pages, 19 embedded ps figures + 1 extra figure, submitted to Phys. Rev. B
                cond-mat.stat-mech cond-mat.mtrl-sci

                Condensed matter
                Condensed matter

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