Hysteresis in the Random Field Ising Model and Bootstrap Percolation

dc.creatorSabhapandit, Sanjib
dc.creatorDhar, Deepak
dc.creatorShukla, Prabodh
dc.date2002-04-29
dc.date.accessioned2026-07-07T09:31:21Z
dc.date.available2026-07-07T09:31:21Z
dc.descriptionWe study hysteresis in the random-field Ising model with an asymmetric distribution of quenched fields, in the limit of low disorder in two and three dimensions. We relate the spin flip process to bootstrap percolation, and show that the characteristic length for self-averaging $L^*$ increases as $exp(exp (J/Δ))$ in 2d, and as $exp(exp(exp(J/Δ)))$ in 3d, for disorder strength $Δ$ much less than the exchange coupling J. For system size $1 << L < L^*$, the coercive field $h_{coer}$ varies as $2J - Δ\ln \ln L$ for the square lattice, and as $2J - Δ\ln \ln \ln L$ on the cubic lattice. Its limiting value is 0 for L tending to infinity, both for square and cubic lattices. For lattices with coordination number 3, the limiting magnetization shows no jump, and $h_{coer}$ tends to J.
dc.description4 pages, 4 figures
dc.identifierhttps://arxiv.org/abs/cond-mat/0204618
dc.identifierhttp://arxiv.org/abs/cond-mat/0204618
dc.identifierPhys. Rev. Lett. 88, 197202 (2002)
dc.identifierdoi:10.1103/PhysRevLett.88.197202
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/158428
dc.subjectStatistical Mechanics
dc.titleHysteresis in the Random Field Ising Model and Bootstrap Percolation
dc.typetext

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