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18 January 2026
- 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
13 January 2026
- 15:3015:30, 13 January 2026 diff hist +4,249 L1 ICTS →Random Energy Model
- 15:2715:27, 13 January 2026 diff hist +16 LBan-1 →Back to REM current
- 15:2315:23, 13 January 2026 diff hist −6 LBan-1 →Back to REM
- 15:1915:19, 13 January 2026 diff hist +321 LBan-1 →Part III
- 14:3614:36, 13 January 2026 diff hist +64 L1 ICTS →Spin glass Transition
- 14:2614:26, 13 January 2026 diff hist +2,053 L1 ICTS →Self-averaging observables
- 14:2514:25, 13 January 2026 diff hist −2,034 L1 ICTS →Edwards Anderson order parameter
- 09:2909:29, 13 January 2026 diff hist −4 L1 ICTS →Edwards Anderson model
- 09:2909:29, 13 January 2026 diff hist +493 L1 ICTS →Edwards Anderson model
- 08:4608:46, 13 January 2026 diff hist +510 L1 ICTS →Random energy model
- 08:4408:44, 13 January 2026 diff hist −576 L1 ICTS →The SK model
- 07:1907:19, 13 January 2026 diff hist +10,081 N L1 ICTS Created page with "<strong>Goal: </strong> Spin glass transition. From the experiments with the anomaly on the magnetic susceptibility to order parameter of the transition. We will discuss the arguments linked to extreme value statistics = Spin glass Transition = Spin glass behavior was first observed in experiments with non-magnetic metals (such as Cu, Fe, Au, etc.) doped with a small percentage of magnetic impurities, typically Mn. At low doping levels, the magnetic moments of Mn..."
18 September 2025
- 20:5220:52, 18 September 2025 diff hist +10 LBan-V →Stationary solution
- 19:4919:49, 18 September 2025 diff hist 0 LBan-V →The final evolution equation
- 18:1418:14, 18 September 2025 diff hist −295 LBan-V →Avalanches at the Depinning Transition
- 12:1112:11, 18 September 2025 diff hist −48 LBan-V →Avalanche Size
17 September 2025
16 September 2025
- 21:0921:09, 16 September 2025 diff hist −139 LBan-IV →Depinning tranition: the equation of motion
- 21:0621:06, 16 September 2025 diff hist −2 LBan-IV →Extensions of the 1D model
- 20:1420:14, 16 September 2025 diff hist +12 L-4 →Back to REM: condensation of the Gibbs measure
- 15:3715:37, 16 September 2025 diff hist −20 TBan-IV →Bienaymé Galton Watson process current
- 15:3615:36, 16 September 2025 diff hist −16 TBan-IV →Bienaymé Galton Watson process
- 15:1815:18, 16 September 2025 diff hist +162 L-4 →Overlap Distribution and Replica Symmetry Breaking:
- 15:0415:04, 16 September 2025 diff hist −999 L-4 →More general REM and systems in Finite dimensions
- 14:3314:33, 16 September 2025 diff hist +3 L-4 →Overlap Distribution and Replica Symmetry Breaking:
- 14:2914:29, 16 September 2025 diff hist +1,070 L-4 →Behavior in Different Phases:
- 14:1014:10, 16 September 2025 diff hist −452 L-4 →Exercise 1: Back to REM
- 13:4213:42, 16 September 2025 diff hist +4,711 L-4 No edit summary
- 13:3813:38, 16 September 2025 diff hist +6 ICTS →Lectures and tutorials current
- 13:3613:36, 16 September 2025 diff hist −4,873 TBan-III →Exercise 1: Back to REM current
- 11:0311:03, 16 September 2025 diff hist 0 ICTS →Lectures and tutorials
- 07:5607:56, 16 September 2025 diff hist +2 LBan-II →Entropy and scaling relation current
- 04:5504:55, 16 September 2025 diff hist 0 LBan-II →Directed Polymers on a lattice
- 04:4604:46, 16 September 2025 diff hist +1 LBan-II →Directed polymers in random media
- 04:4504:45, 16 September 2025 diff hist +2,707 LBan-II →Introduction: Interfaces and Directed Polymers
- 04:4404:44, 16 September 2025 diff hist −13 ICTS →Lectures and tutorials
- 04:4404:44, 16 September 2025 diff hist +1,070 TBan-II No edit summary current
- 04:4204:42, 16 September 2025 diff hist −3,777 LBan-II →Thermal Interfaces
15 September 2025
- 17:3217:32, 15 September 2025 diff hist −38 LBan-II →Thermal Interfaces
- 11:3411:34, 15 September 2025 diff hist −23 LBan-II →Feynman-Kac formula
- 10:4210:42, 15 September 2025 diff hist 0 LBan-1 →Back to REM
- 10:4010:40, 15 September 2025 diff hist +3 LBan-1 →Back to canonical ensemble: the freezing transition
13 September 2025
- 14:1314:13, 13 September 2025 diff hist +79 TBan-I →Exercise 1: The Gumbel Distribution current
- 14:0814:08, 13 September 2025 diff hist +40 LBan-1 →Gaussian Case