Far-from-equilibrium criticality in the Random Field Ising Model with Eshelby Interactions
arXiv:2309.14919 · doi:10.1103/PhysRevB.108.L220202
Abstract
We study a quasi-statically driven random field Ising model (RFIM) at zero temperature with interactions mediated by the long-range anisotropic Eshelby kernel. Analogously to amorphous solids at their yielding transition, and differently from ferromagnetic and dipolar RFIMs, the model shows a discontinuous magnetization jump associated with the appearance of a band-like structure for weak disorder and a continuous magnetization growth, yet punctuated by avalanches, for strong disorder. Through a finite-size scaling analysis in 2 and 3 dimensions we find that the two regimes are separated by a finite-disorder critical point which we characterize. We discuss similarities and differences between the present model and models of sheared amorphous solids.
References in corpus (8)
- Statistical Models of Fracture
- Scaling description of the yielding transition in soft amorphous solids at zero temperature
- Marginal Stability in Structural, Spin and Electron Glasses
- The effects of cooling rate on particle rearrangement statistics: Rapidly cooled glasses are more ductile and less reversible
- Rigidity-Controlled Crossover: From Spinodal to Critical Failure
- Yielding, shear banding and brittle failure of amorphous materials
- Finite-disorder critical point in the yielding transition of elasto-plastic models
- Hysteresis in Anti-Ferromagnetic Random-Field Ising Model at Zero Temperature
Cited by in corpus (4)
- Yielding and plasticity in amorphous solids
- Ductile and brittle yielding of athermal amorphous solids: a mean-field paradigm beyond the random field Ising model
- Yielding in dense active matter
- Discontinuity in the distribution of field increments between avalanches in non-abelian random field Blume-Emery-Griffiths model with no passing violation