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13:5613:56, 8 September 2025 diff hist 0‎ LBan-IV ‎ →‎Second moment
13:5613:56, 8 September 2025 diff hist +21‎ LBan-IV ‎ →‎Second moment
13:5513:55, 8 September 2025 diff hist +149‎ LBan-IV ‎ →‎Second moment
13:4113:41, 8 September 2025 diff hist +727‎ LBan-IV ‎ →‎Velocity-Force Caracteristics
13:3813:38, 8 September 2025 diff hist 0‎ LBan-IV ‎ →‎Velocity-Force Caracteristics
11:5411:54, 8 September 2025 diff hist +1,097‎ LBan-IV ‎ →‎Velocity-Force Caracteristics
11:0811:08, 8 September 2025 diff hist +630‎ LBan-IV ‎No edit summary
08:3008:30, 8 September 2025 diff hist +211‎ LBan-IV ‎ →‎Velocity-Force Caracteristics

10:4610:46, 7 September 2025 diff hist +550‎ LBan-IV ‎ →‎Step 2: Discretization along the h-direction
10:4510:45, 7 September 2025 diff hist −79‎ LBan-IV ‎ →‎Extensions of the 1D model
10:1810:18, 7 September 2025 diff hist −3‎ LBan-IV ‎ →‎Step 1: Discretization along the x-direction
10:1710:17, 7 September 2025 diff hist +2,117‎ LBan-IV ‎ →‎Extensions of the 1D model
08:5508:55, 7 September 2025 diff hist +720‎ LBan-IV ‎ →‎Depinning tranition: the equation of motion

19:0019:00, 6 September 2025 diff hist −52‎ LBan-IV ‎ →‎Cellular Automata
18:5518:55, 6 September 2025 diff hist +621‎ LBan-IV ‎ →‎Depinning tranition: the equation of motion

15:2615:26, 4 September 2025 diff hist 0‎ LBan-1 ‎ →‎The partition function
15:2615:26, 4 September 2025 diff hist +75‎ LBan-1 ‎ →‎The partition function
15:2415:24, 4 September 2025 diff hist +12‎ LBan-1 ‎ →‎The partition function
15:2215:22, 4 September 2025 diff hist +11‎ LBan-1 ‎ →‎Overview
12:0912:09, 4 September 2025 diff hist −6‎ LBan-1 ‎ →‎Overview
12:0912:09, 4 September 2025 diff hist +9‎ LBan-1 ‎ →‎Overview
12:0812:08, 4 September 2025 diff hist +11‎ LBan-1 ‎ →‎Overview

20:2620:26, 31 August 2025 diff hist −58‎ LBan-IV ‎ →‎Step 3: Mean-Field (Fully Connected) Limit
20:2420:24, 31 August 2025 diff hist +75‎ LBan-IV ‎ →‎Step 3: Mean-Field (Fully Connected) Limit
20:2320:23, 31 August 2025 diff hist +88‎ LBan-IV ‎ →‎Step 3: Mean-Field (Fully Connected) Limit
20:2320:23, 31 August 2025 diff hist +198‎ LBan-IV ‎ →‎Step 3: Mean-Field (Fully Connected) Limit
20:2220:22, 31 August 2025 diff hist +170‎ LBan-IV ‎ →‎Step 2: Discretization along the h-direction
20:1920:19, 31 August 2025 diff hist +681‎ LBan-IV ‎ →‎Step 2: Discretization along the h-direction
20:0620:06, 31 August 2025 diff hist +136‎ LBan-IV ‎ →‎Step 2: Discretization along the h-direction
19:5819:58, 31 August 2025 diff hist +411‎ LBan-IV ‎ →‎Step 2: Discretization along the h-direction
19:5719:57, 31 August 2025 diff hist +1,769‎ LBan-IV ‎ →‎Depinning tranition: the equation of motion
18:3118:31, 31 August 2025 diff hist +1,885‎ N LBan-IV ‎ Created page with "= Pinning and Depinning of a Disordered Material = In earlier lectures, we discussed how disordered systems can become trapped in deep energy states, forming a glass. Today, we will examine how such systems can also be ''pinned'' and resist external deformation. This behavior arises because disorder creates a complex energy landscape with numerous features, including minima (of varying depth), maxima, and saddle points. When an external force is applied, it tilts t..."
18:0218:02, 31 August 2025 diff hist +178‎ ICTS ‎No edit summary
17:0317:03, 31 August 2025 diff hist +8‎ TBan-III ‎ →‎Exercise 2: Edwards-Wilkinson Interface with Stationary Initial Condition current
16:3316:33, 31 August 2025 diff hist +2,785‎ TBan-III ‎ →‎Exercise 1: Back to REM
16:2916:29, 31 August 2025 diff hist +2,088‎ TBan-III ‎No edit summary
15:5215:52, 31 August 2025 diff hist +78‎ TBan-III ‎ →‎Exercise 2: Edwards-Wilkinson Interface with Stationary Initial Condition (7.5 points)
15:5015:50, 31 August 2025 diff hist +3,923‎ N TBan-III ‎ Created page with "= Exercise 2: Edwards-Wilkinson Interface with Stationary Initial Condition (7.5 points) = Consider an Edwards-Wilkinson interface in 1+1 dimensions, at temperature <math>T</math>, and of length <math>L</math> with periodic boundary conditions: <center><math> \frac{\partial h(x,t)}{\partial t} = \nu \nabla^2 h(x,t) + \eta(x,t) </math></center> where <math>\eta(x,t)</math> is a Gaussian white noise with zero mean and variance: <center><math> \langle \eta(x,t) \eta(x',..."
15:1715:17, 31 August 2025 diff hist +4‎ TBan-I ‎ →‎Exercise 3: number of states above the minimum
15:1515:15, 31 August 2025 diff hist +123‎ TBan-I ‎ →‎Exercise 2: The Weakest Link and the Weibull Distribution
15:1315:13, 31 August 2025 diff hist +175‎ TBan-I ‎ →‎Exercise 2: The Weakest Link and the Weibull Distribution
15:1215:12, 31 August 2025 diff hist +118‎ TBan-I ‎ →‎Exercise 2: The Weakest Link and the Weibull Distribution
15:1115:11, 31 August 2025 diff hist +109‎ TBan-I ‎ →‎Exercise 2: The Weakest Link and the Weibull Distribution
15:1015:10, 31 August 2025 diff hist +397‎ TBan-I ‎ →‎Exercise 3: The Weakest Link and the Weibull Distribution
15:0915:09, 31 August 2025 diff hist +410‎ TBan-I ‎ →‎esercizio 2: The weakest link
14:5314:53, 31 August 2025 diff hist −25‎ TBan-I ‎ →‎Exercise 1: The Gumbel Distribution

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