Elastic interfaces on disordered substrates: From mean-field depinning to yielding
arXiv:1905.08771 · doi:10.1103/PhysRevLett.123.218002
Abstract
We consider a model of an elastic manifold driven on a disordered energy landscape, with generalized long range elasticity. Varying the form of the elastic kernel by progressively allowing for the existence of zero-modes, the model interpolates smoothly between mean field depinning and finite dimensional yielding. We find that the critical exponents of the model change smoothly in this process. Also, we show that in all cases the Herschel-Buckley exponent of the flowcurve depends on the analytical form of the microscopic pinning potential. This is a compelling indication that within the present elastoplastic description yielding in finite dimension is a mean-field transition.
6 pages, 5 figures
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- Ductile and brittle yielding of athermal amorphous solids: a mean-field paradigm beyond the random field Ising model
- Theory and Experiments for Disordered Elastic Manifolds, Depinning, Avalanches, and Sandpiles
- The Fate of Shear-Oscillated Amorphous Solids
- Emergence of a random field at the yielding transition of a mean-field Elasto-Plastic model
- Soil creep facilitated by cyclic variations of environmental conditions
- Yielding versus random organization: convex absorbing transitions in soft matter