{ "id": "2107.06365", "version": "v1", "published": "2021-07-13T20:02:13.000Z", "updated": "2021-07-13T20:02:13.000Z", "title": "The yielding of amorphous solids at finite temperatures", "authors": [ "Ezequiel E. Ferrero", "Alejandro B. Kolton", "Eduardo A. Jagla" ], "comment": "16 pages, 11 figures", "categories": [ "cond-mat.dis-nn", "cond-mat.mtrl-sci", "cond-mat.soft" ], "abstract": "We analyze the effect of temperature on the yielding transition of amorphous solids using different coarse-grained model approaches. On one hand we use an elasto-plastic model, with temperature introduced in the form of an Arrhenius activation law over energy barriers. On the other hand, we implement a Hamiltonian model with a relaxational dynamics, where temperature is introduced in the form of a Langevin stochastic force. In both cases, temperature transforms the sharp transition of the athermal case in a smooth crossover. We show that this thermally smoothed transition follows a simple scaling form that can be fully explained using a one-particle system driven in a potential under the combined action of a mechanical and a thermal noise, the stochastically-driven Prandtl-Tomlinson model. Our work harmonizes the results of simple models for amorphous solids with the phenomenological $\\sim T^{2/3}$ law proposed by Johnson and Samwer [Phys. Rev. Lett. 95, 195501 (2005)] in the framework of experimental metallic glasses yield observations, and extend it to a generic case. Conclusively, our results strengthen the interpretation of the yielding transition as an effective mean-field phenomenon.", "revisions": [ { "version": "v1", "updated": "2021-07-13T20:02:13.000Z" } ], "analyses": { "keywords": [ "amorphous solids", "finite temperatures", "experimental metallic glasses yield observations", "langevin stochastic force", "arrhenius activation law" ], "note": { "typesetting": "TeX", "pages": 16, "language": "en", "license": "arXiv", "status": "editable" } } }