The effect of disorder geometry on the critical force in disordered elastic systems

被引:10
|
作者
Demery, Vincent [1 ,2 ]
Lecomte, Vivien [3 ,4 ]
Rosso, Alberto [5 ]
机构
[1] Univ Paris 06, CNRS, Inst Jean Le Rond Dalembert, UMR 7190, F-75005 Paris, France
[2] Univ Massachusetts, Dept Phys, Amherst, MA 01003 USA
[3] Univ Paris 06, CNRS, Lab Probabil & Modeles Aleatoires, UMR 7599, F-75013 Paris, France
[4] Univ Paris Diderot, F-75013 Paris, France
[5] Univ Paris 11, CNRS, Lab Phys Theor & Modeles Stat, UMR 8626, F-91405 Orsay, France
来源
JOURNAL OF STATISTICAL MECHANICS-THEORY AND EXPERIMENT | 2014年
关键词
classical phase transitions (theory); interfaces in random media (theory); disordered systems (theory); heterogeneous materials (theory); RANDOM-MEDIA; INTERFACES; DYNAMICS; MOTION; CREEP; WAVES; STATE;
D O I
10.1088/1742-5468/2014/03/P03009
中图分类号
O3 [力学];
学科分类号
08 ; 0801 ;
摘要
We address the effect of disorder geometry on the critical force in disordered elastic systems. We focus on the model system of a long-range elastic line driven in a random landscape. In the collective pinning regime. we compute the critical force perturbatively. Not only does our expression for the critical force confirm previous results on its scaling with respect to the microscopic disorder parameters, but it also provides its precise dependence on the disorder geometry (represented by the disorder two-point correlation function). Our results are successfully compared with the results of numerical simulations for random field and random bond disorders.
引用
收藏
页数:20
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