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Phys. Rev. E 60, 1428–1440 (1999)

Functional integration approach to hysteresis

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G. Bertotti1, I. D. Mayergoyz2, V. Basso1, and A. Magni1
1Istituto Elettrotecnico Nazionale Galileo Ferraris, Corso Massimo d’Azeglio 42, I-10125 Torino, Italy
2Electrical and Computer Engineering Department, University of Maryland, College Park, Maryland 20742

Received 22 February 1999; published in the issue dated August 1999

A general formulation of scalar hysteresis is proposed. This formulation is based on two steps. First, a generating function g(x) is associated with an individual system, and a hysteresis evolution operator is defined by an appropriate envelope construction applied to g(x), inspired by the overdamped dynamics of systems evolving in multistable free-energy landscapes. Second, the average hysteresis response of an ensemble of such systems is expressed as a functional integral over the space G of all admissible generating functions, under the assumption that an appropriate measure μ has been introduced in G. The consequences of the formulation are analyzed in detail in the case where the measure μ is generated by a continuous, Markovian stochastic process. The calculation of the hysteresis properties of the ensemble is reduced to the solution of the level-crossing problem for the stochastic process. In particular, it is shown that, when the process is translationally invariant (homogeneous), the ensuing hysteresis properties can be exactly described by the Preisach model of hysteresis, and the associated Preisach distribution is expressed in closed analytic form in terms of the drift and diffusion parameters of the Markovian process. Possible applications of the formulation are suggested, concerning the interpretation of magnetic hysteresis due to domain wall motion in quenched-in disorder and the interpretation of critical state models of superconducting hysteresis.

© 1999 The American Physical Society

URL:
http://link.aps.org/doi/10.1103/PhysRevE.60.1428
DOI:
10.1103/PhysRevE.60.1428
PACS:
02.50.Ga, 75.60.Ej, 05.40.-a