User contributions for Rosso

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A user with 1,359 edits. Account created on 25 September 2023.

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22:2422:24, 23 January 2026 diff hist −5 L2 ICFP →Long-time behavior
22:2322:23, 23 January 2026 diff hist +4 Main Page →Lectures and tutorials
21:1121:11, 23 January 2026 diff hist +1,163 L2 ICFP →Growth and saturation of the width
20:5820:58, 23 January 2026 diff hist −606 L2 ICFP →Width of the interface
20:5720:57, 23 January 2026 diff hist −33 L2 ICFP →Solution in Fourier space
20:1120:11, 23 January 2026 diff hist +1,898 L2 ICFP →Solution in Fourier space
17:3217:32, 23 January 2026 diff hist +2 L2 ICFP →Symmetries and scaling invariance
17:2717:27, 23 January 2026 diff hist −5 L2 ICFP →Elastic energy and Edwards–Wilkinson equation
17:2717:27, 23 January 2026 diff hist −61 L2 ICFP →Edwards–Wilkinson model: thermal interfaces
17:2617:26, 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..."
09:5009:50, 23 January 2026 diff hist 0 L1 ICTS →Extreme value statistics for Gaussian variables
09:4909:49, 23 January 2026 diff hist 0 L1 ICTS →Universality
09:4809:48, 23 January 2026 diff hist −57 L1 ICTS →Universality
09:4709:47, 23 January 2026 diff hist +2 L1 ICTS →Gumbel scaling of the minimum
09:4609:46, 23 January 2026 diff hist +1,917 L1 ICTS →Gaussian Case
09:0909:09, 23 January 2026 diff hist +8 L1 ICTS →Determination of the freezing temperature
09:0809:08, 23 January 2026 diff hist +858 L1 ICTS →Freezing transition
09:0809:08, 23 January 2026 diff hist +25 L1 ICTS →Gaussian Case
08:5708:57, 23 January 2026 diff hist −3 L1 ICTS →Determination of the freezing temperature
08:5708:57, 23 January 2026 diff hist +46 L1 ICTS →Freezing transition
08:5608:56, 23 January 2026 diff hist 0 L1 ICTS →Determination of the freezing temperature
08:5208:52, 23 January 2026 diff hist +138 L1 ICTS →Back to REM
08:5008:50, 23 January 2026 diff hist +8 L1 ICTS →Phase Transition in the Random Energy Model
08:4908:49, 23 January 2026 diff hist −8 L1 ICTS →Back to REM
08:4708:47, 23 January 2026 diff hist +36 L1 ICTS →Simpler models
08:4608:46, 23 January 2026 diff hist +4 L1 ICTS →Simpler models
08:4008:40, 23 January 2026 diff hist −4 L1 ICTS →Back to REM
08:4008:40, 23 January 2026 diff hist +2,013 L1 ICTS →Back to REM

21:3621:36, 18 January 2026 diff hist +3 L1 ICTS →Deterministic observables
20:2420:24, 18 January 2026 diff hist −4 L1 ICTS →Back to REM
20:2320:23, 18 January 2026 diff hist −5 L1 ICTS →Back to REM
20:2320:23, 18 January 2026 diff hist +3 L1 ICTS →Random energy landascape
20:1820:18, 18 January 2026 diff hist −2 L1 ICTS →Random energy landascape
15:5715:57, 18 January 2026 diff hist −1 Main Page →Lectures and tutorials
15:2315:23, 18 January 2026 diff hist +1 Main Page →Lectures and tutorials
15:2315:23, 18 January 2026 diff hist +1 Main Page →Lectures and tutorials
15:2015:20, 18 January 2026 diff hist +46 Main Page →Lectures and tutorials
15:1115:11, 18 January 2026 diff hist +2,640 H 1 →Exercise 2: Weakest-link statistics and the Weibull law current
15:0315:03, 18 January 2026 diff hist +2 H 1 →Exercise 2: Weakest-link statistics and the Weibull law
14:5214:52, 18 January 2026 diff hist −7 H 1 →Exercise 2: Weakest-link statistics and the Weibull law
14:4914:49, 18 January 2026 diff hist +4 H 1 →Exercise 2: Weakest-link statistics and the Weibull law
14:3914:39, 18 January 2026 diff hist −3 H 1 →Exercise 2: Weakest-link statistics and the Weibull law
14:3914:39, 18 January 2026 diff hist 0 H 1 →Exercise 2: Weakest-link statistics and the Weibull law
14:3814:38, 18 January 2026 diff hist −17 H 1 →Exercise 2: Weakest-link statistics and the Weibull law
14:3714:37, 18 January 2026 diff hist +2,736 H 1 No edit summary
14:2714:27, 18 January 2026 diff hist +1,261 N H 1 Created page with "We are interested in the asymptotic behavior of the cumulative distribution <math>P(E)</math> in the left tail <math>E\to -\infty</math>, since the minimum is controlled by the regime where <math>M P(E)=O(1)</math>. Starting from the Gaussian distribution with zero mean and variance <math>\sigma^2</math>, we write the cumulative as <center><math> P(E) = \int_{-\infty}^E \frac{dx}{\sqrt{2\pi\sigma^2}} \, e^{-x^2/2\sigma^2}. </math></center> Using integration by parts (o..."
13:2513:25, 18 January 2026 diff hist +7 L1 ICTS →Detour: Extreme Value Statistics
12:5612:56, 18 January 2026 diff hist −10 L1 ICTS →Glass Transition: the Edwards Anderson order parameter
12:5012:50, 18 January 2026 diff hist +4 Main Page →Lectures and tutorials

15:3015:30, 13 January 2026 diff hist +4,249 L1 ICTS →Random Energy Model

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