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• 17:56, 20 March 2026 Rosso talk contribs uploaded a new version of File:Exercises 13 15.pdf
• 21:29, 16 March 2026 Ros talk contribs uploaded a new version of File:2025 P8 solutions.pdf
• 21:28, 16 March 2026 Ros talk contribs uploaded a new version of File:2025 P9 solutions.pdf
• 17:40, 15 March 2026 Ros talk contribs uploaded a new version of File:2025 P7 solutions .pdf
• 17:39, 15 March 2026 Ros talk contribs uploaded a new version of File:2025 P666 solutions .pdf
• 17:06, 15 March 2026 Ros talk contribs created page File:Exercise 16-17.pdf
• 17:06, 15 March 2026 Ros talk contribs uploaded File:Exercise 16-17.pdf
• 17:00, 15 March 2026 Ros talk contribs created page Sample questions (Created page with "XZXZXZ")
• 10:52, 12 March 2026 Rosso talk contribs created page File:DISSYTS.pdf
• 10:52, 12 March 2026 Rosso talk contribs uploaded File:DISSYTS.pdf
• 11:30, 11 March 2026 Ros talk contribs uploaded a new version of File:2025 P5 solutions.pdf
• 16:46, 9 March 2026 Rosso talk contribs created page File:DISSYST.pdf
• 16:46, 9 March 2026 Rosso talk contribs uploaded File:DISSYST.pdf
• 14:16, 9 March 2026 Ros talk contribs created page File:Exercises 13 15.pdf
• 14:16, 9 March 2026 Ros talk contribs uploaded File:Exercises 13 15.pdf
• 17:34, 26 February 2026 Rosso talk contribs created page File:11-12 Exercises.pdf
• 17:34, 26 February 2026 Rosso talk contribs uploaded File:11-12 Exercises.pdf
• 16:24, 25 February 2026 Rosso talk contribs created page File:WellsFigure.png
• 16:24, 25 February 2026 Rosso talk contribs uploaded File:WellsFigure.png
• 09:26, 16 February 2026 Ros talk contribs uploaded a new version of File:Exercises 7&8.pdf
• 17:42, 12 February 2026 Ros talk contribs created page File:Exercises 9-10.pdf
• 17:42, 12 February 2026 Ros talk contribs uploaded File:Exercises 9-10.pdf
• 17:39, 12 February 2026 Ros talk contribs uploaded a new version of File:2025 P3 solutions.pdf
• 19:01, 8 February 2026 Ros talk contribs uploaded a new version of File:2025 Parisi scheme.pdf
• 18:43, 8 February 2026 Ros talk contribs uploaded a new version of File:2025 P4 solutions.pdf
• 18:41, 8 February 2026 Ros talk contribs uploaded a new version of File:2025 P3 solutions.pdf
• 16:04, 7 February 2026 Ros talk contribs uploaded a new version of File:2025 P2 solutions.pdf
• 16:03, 7 February 2026 Ros talk contribs uploaded a new version of File:2025 P1 solutions.pdf
• 09:28, 7 February 2026 Rosso talk contribs created page File:Exercises 7&8.pdf
• 09:28, 7 February 2026 Rosso talk contribs uploaded File:Exercises 7&8.pdf
• 19:36, 28 January 2026 Ros talk contribs created page File:Exercises 5-6.pdf
• 19:36, 28 January 2026 Ros talk contribs uploaded File:Exercises 5-6.pdf
• 19:30, 28 January 2026 Ros talk contribs uploaded a new version of File:2025 P2 solutions.pdf
• 19:29, 28 January 2026 Ros talk contribs uploaded a new version of File:2025 P1 solutions.pdf
• 10:36, 25 January 2026 Ros talk contribs created page File:Exercises 1-3.pdf
• 10:36, 25 January 2026 Ros talk contribs uploaded File:Exercises 1-3.pdf
• 16:26, 23 January 2026 Rosso talk contribs created page 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...")
• 22:25, 21 January 2026 Ros talk contribs created page File:Tutorial and Exercise 4.pdf
• 22:25, 21 January 2026 Ros talk contribs uploaded File:Tutorial and Exercise 4.pdf
• 21:21, 18 January 2026 Ros talk contribs uploaded a new version of File:2025 P1 solutions.pdf
• 13:27, 18 January 2026 Rosso talk contribs created page 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...")
• 17:44, 14 January 2026 Lptmswikids talk contribs deleted page L-1-new (content was: "<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 * Random energy model * Detour: Extreme Value Statistics * A Concrete Example: The Gaussian Case * The Scaling Form in the Large ''M'...", and the only contributor was "Lptmswikids" (talk))
• 17:36, 14 January 2026 Lptmswikids talk contribs deleted page The Scaling Form in the Large ''M'' Limit (content was: "In the spirit of the central limit theorem, we look for a scaling form: <center> <math>E_{\min} = a_M + b_M z</math> </center> The constants <math>a_M</math> and <math>b_M</math> absorb the dependence on <math>M</math>, while the random variable <math>z</math> is distributed according to a probability distribution <math>P(z)</math> that does not depend on <math>M</...", and the only contributor was "Lptmswikids" (talk))
• 17:35, 14 January 2026 Lptmswikids talk contribs deleted page The SK model (content was: "== The SK model == Sherrington and Kirkpatrik considered the fully connected version of the model with Gaussian couplings: <center> <math> E= - \sum_{i,j} \frac{J_{ij}}{ \sqrt{N}} \sigma_i \sigma_j </math></center> At the inverse temperature <math> \beta </math>, the partion function of the model is <center> <math> Z= \sum_{\alpha=1}^{2^N} z_{\alpha}, \quad \te...", and the only contributor was "Lptmswikids" (talk))
• 17:35, 14 January 2026 Lptmswikids talk contribs deleted page Test-qin (content was: "=Detour: Extreme Value Statistics= Consider the REM spectrum of <math>M</math> energies <math>E_1, \dots, E_M</math> drawn from a distribution <math>p(E)</math>. It is useful to introduce the cumulative probability of finding an energy smaller than ''E'' <center> <math>P(E) = \int_{-\infty}^E dx \, p(x)</math> </center> We also define: <center> <math>E_{\min} = \...", and the only contributor was "Lptmswikids" (talk))
• 17:35, 14 January 2026 Lptmswikids talk contribs deleted page More general REM and systems in Finite dimensions (content was: "In random energy models with i.i.d. random variables, the distribution <math>p(E)</math> determines the dependence of <math>a_M</math> and <math>b_M</math> on ''M'', and consequently their scaling with ''N'', the number of degrees of freedom. It is insightful to consider a more general case where an exponent <math>\omega</math> describes the fluctuations of the gro...", and the only contributor was "Lptmswikids" (talk))
• 17:35, 14 January 2026 Lptmswikids talk contribs deleted page Phase Transition in the Random Energy Model (content was: "The Random Energy Model (REM) exhibits two distinct phases: * '''High-Temperature Phase:''' : At high temperatures, the system is in a paramagnetic phase where the entropy is extensive, and the occupation probability of a configuration is approximately <math>\sim 1/M</math>. * '''Low-Temperature Phase:''' : Below a critical freezing temperature <math>T_f</m...", and the only contributor was "Lptmswikids" (talk))
• 17:34, 14 January 2026 Lptmswikids talk contribs deleted page Random energy model (content was: "The solution of the Sherrington-Kirkpatrick (SK) model is challenging. To make progress, we first study the Random Energy Model (REM), introduced by B. Derrida. This model simplifies the problem by neglecting correlations between the <math>M=2^N</math> configurations and assuming that the energies <math>E_{\alpha}</math> are independent and identically distributed...", and the only contributor was "Lptmswikids" (talk))
• 17:34, 14 January 2026 Lptmswikids talk contribs deleted page Spin glass Transition (content was: "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 atoms interact via the Ruderman–Kittel–Kasuya–Yosida (RKKY) interaction. This interaction has a random sign due to the random spatial dist...", and the only contributor was "Lptmswikids" (talk))
• 17:33, 14 January 2026 Lptmswikids talk contribs deleted page Edwards Anderson order parameter (content was: "Since <math>\overline{J} = 0</math>, the model does not exhibit spatial magnetic order, such as ferromagnetic or antiferromagnetic order. Instead, the idea is to distinguish between two phases: * Paramagnetic phase: Configurations are explored with all possible spin orientations. * Spin glass phase: Spin orientations are random but frozen (i.e., immobile). The gla...", and the only contributor was "Lptmswikids" (talk))