User contributions for Rosso
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26 January 2026
- 10:5510:55, 26 January 2026 diff hist −2 L1 ICTS →Back to REM current
25 January 2026
- 16:5816:58, 25 January 2026 diff hist −270 L2 ICFP →Solution in Fourier space current
- 16:3616:36, 25 January 2026 diff hist +492 L2 ICFP →Solution in Fourier space
- 16:2316:23, 25 January 2026 diff hist +117 L2 ICFP →Thermal interfaces: Langevin dynamics
23 January 2026
- 21:2421:24, 23 January 2026 diff hist −3 L2 ICFP →Width of the interface
- 21:2421:24, 23 January 2026 diff hist −5 L2 ICFP →Symmetries and scaling invariance
- 21:2421:24, 23 January 2026 diff hist −130 L2 ICFP →Short-time behavior
- 21:2421:24, 23 January 2026 diff hist −5 L2 ICFP →Long-time behavior
- 21:2321:23, 23 January 2026 diff hist +4 Main Page →Lectures and tutorials
- 20:1120:11, 23 January 2026 diff hist +1,163 L2 ICFP →Growth and saturation of the width
- 19:5819:58, 23 January 2026 diff hist −606 L2 ICFP →Width of the interface
- 19:5719:57, 23 January 2026 diff hist −33 L2 ICFP →Solution in Fourier space
- 19:1119:11, 23 January 2026 diff hist +1,898 L2 ICFP →Solution in Fourier space
- 16:3216:32, 23 January 2026 diff hist +2 L2 ICFP →Symmetries and scaling invariance
- 16:2716:27, 23 January 2026 diff hist −5 L2 ICFP →Elastic energy and Edwards–Wilkinson equation
- 16:2716:27, 23 January 2026 diff hist −61 L2 ICFP →Edwards–Wilkinson model: thermal interfaces
- 16:2616:26, 23 January 2026 diff hist +5,196 N L2 ICFP Created page with "= Edwards–Wilkinson model: thermal interfaces = == Interfaces and manifolds == Many physical systems are governed by elastic manifolds embedded in a higher-dimensional medium. Typical examples include domain walls in ferromagnets, dislocations in crystals, vortex lines in superconductors, and propagating fronts. We introduce the following notation: * <math>d</math>: internal dimension of the manifold * <math>N</math>: dimension of the displacement (or height) fie..."
- 08:5008:50, 23 January 2026 diff hist 0 L1 ICTS →Extreme value statistics for Gaussian variables
- 08:4908:49, 23 January 2026 diff hist 0 L1 ICTS →Universality
- 08:4808:48, 23 January 2026 diff hist −57 L1 ICTS →Universality
- 08:4708:47, 23 January 2026 diff hist +2 L1 ICTS →Gumbel scaling of the minimum
- 08:4608:46, 23 January 2026 diff hist +1,917 L1 ICTS →Gaussian Case
- 08:0908:09, 23 January 2026 diff hist +8 L1 ICTS →Determination of the freezing temperature
- 08:0808:08, 23 January 2026 diff hist +858 L1 ICTS →Freezing transition
- 08:0808:08, 23 January 2026 diff hist +25 L1 ICTS →Gaussian Case
- 07:5707:57, 23 January 2026 diff hist −3 L1 ICTS →Determination of the freezing temperature
- 07:5707:57, 23 January 2026 diff hist +46 L1 ICTS →Freezing transition
- 07:5607:56, 23 January 2026 diff hist 0 L1 ICTS →Determination of the freezing temperature
- 07:5207:52, 23 January 2026 diff hist +138 L1 ICTS →Back to REM
- 07:5007:50, 23 January 2026 diff hist +8 L1 ICTS →Phase Transition in the Random Energy Model
- 07:4907:49, 23 January 2026 diff hist −8 L1 ICTS →Back to REM
- 07:4707:47, 23 January 2026 diff hist +36 L1 ICTS →Simpler models
- 07:4607:46, 23 January 2026 diff hist +4 L1 ICTS →Simpler models
- 07:4007:40, 23 January 2026 diff hist −4 L1 ICTS →Back to REM
- 07:4007:40, 23 January 2026 diff hist +2,013 L1 ICTS →Back to REM
18 January 2026
- 20:3620:36, 18 January 2026 diff hist +3 L1 ICTS →Deterministic observables
- 19:2419:24, 18 January 2026 diff hist −4 L1 ICTS →Back to REM
- 19:2319:23, 18 January 2026 diff hist −5 L1 ICTS →Back to REM
- 19:2319:23, 18 January 2026 diff hist +3 L1 ICTS →Random energy landascape
- 19:1819:18, 18 January 2026 diff hist −2 L1 ICTS →Random energy landascape
- 14:5714:57, 18 January 2026 diff hist −1 Main Page →Lectures and tutorials
- 14:2314:23, 18 January 2026 diff hist +1 Main Page →Lectures and tutorials
- 14:2314:23, 18 January 2026 diff hist +1 Main Page →Lectures and tutorials
- 14:2014:20, 18 January 2026 diff hist +46 Main Page →Lectures and tutorials
- 14:1114:11, 18 January 2026 diff hist +2,640 H 1 →Exercise 2: Weakest-link statistics and the Weibull law current
- 14:0314:03, 18 January 2026 diff hist +2 H 1 →Exercise 2: Weakest-link statistics and the Weibull law
- 13:5213:52, 18 January 2026 diff hist −7 H 1 →Exercise 2: Weakest-link statistics and the Weibull law
- 13:4913:49, 18 January 2026 diff hist +4 H 1 →Exercise 2: Weakest-link statistics and the Weibull law
- 13:3913:39, 18 January 2026 diff hist −3 H 1 →Exercise 2: Weakest-link statistics and the Weibull law
- 13:3913:39, 18 January 2026 diff hist 0 H 1 →Exercise 2: Weakest-link statistics and the Weibull law