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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 current
- 14:0514:05, 13 September 2025 diff hist −4 LBan-1 →Gaussian Case
- 13:5913:59, 13 September 2025 diff hist −40 LBan-1 →Il Caso Gaussiano
- 13:5713:57, 13 September 2025 diff hist +113 LBan-1 →Back to REM
- 13:0513:05, 13 September 2025 diff hist −773 LBan-1 →Back to REM
- 12:5112:51, 13 September 2025 diff hist +25 LBan-1 →Back to canonical ensemble: the freezing transition
- 12:4912:49, 13 September 2025 diff hist +20 LBan-1 →Microcanonical calculation
- 12:4712:47, 13 September 2025 diff hist +35 LBan-1 →Microcanonical calculation
11 September 2025
- 16:5316:53, 11 September 2025 diff hist +5 LBan-V →Mapping to the Brownian motion current
- 16:5016:50, 11 September 2025 diff hist +8 LBan-V →Stationary solution
- 16:4716:47, 11 September 2025 diff hist −1 LBan-V →The final evolution equation
- 16:4516:45, 11 September 2025 diff hist +62 LBan-V →Derivation of the Evolution Equation
- 16:3416:34, 11 September 2025 diff hist −45 LBan-V →Avalanches
- 16:2116:21, 11 September 2025 diff hist +51 LBan-V →Stationary solution
- 15:3915:39, 11 September 2025 diff hist −1,797 LBan-V →Dynamics
- 15:1415:14, 11 September 2025 diff hist −5 LBan-V →Derivation of the Evolution Equation
- 14:5214:52, 11 September 2025 diff hist −11 LBan-V →Derivation of the Evolution Equation
- 14:1014:10, 11 September 2025 diff hist +66 LBan-V →Derivation of the Evolution Equation
- 09:3509:35, 11 September 2025 diff hist +16 LBan-V →Derivation of the Evolution Equation
- 09:2709:27, 11 September 2025 diff hist +626 LBan-V →Derivation of the Evolution Equation
- 08:5608:56, 11 September 2025 diff hist +189 LBan-V →Derivation of the Evolution Equation
- 07:5607:56, 11 September 2025 diff hist −230 LBan-V →Derivation of the Evolution Equation
10 September 2025
- 15:1015:10, 10 September 2025 diff hist +94 LBan-V →Derivation of the Evolution Equation
- 15:0415:04, 10 September 2025 diff hist +34 LBan-V →Derivation of the Evolution Equation
- 15:0215:02, 10 September 2025 diff hist −4 LBan-V →Dynamics
- 15:0115:01, 10 September 2025 diff hist +88 LBan-V →Derivation of the Evolution Equation
- 12:2412:24, 10 September 2025 diff hist +39 LBan-V →Derivation of the Evolution Equation
- 12:0312:03, 10 September 2025 diff hist +11 LBan-V →Derivation of the Evolution Equation
- 11:4311:43, 10 September 2025 diff hist +3 LBan-V →Derivation of the Evolution Equation
- 11:2811:28, 10 September 2025 diff hist −35 LBan-V →Derivation of the Evolution Equation
- 11:2711:27, 10 September 2025 diff hist −6 LBan-V →Derivation of the Evolution Equation
- 11:2611:26, 10 September 2025 diff hist +2,631 LBan-V →Avalanche Size
9 September 2025
- 12:4112:41, 9 September 2025 diff hist −42 LBan-V →Quasi-Static Protocol and Avalanche Definition
- 12:3912:39, 9 September 2025 diff hist +606 LBan-V →Fully connected model with parabolic potential
- 12:3812:38, 9 September 2025 diff hist +2,202 LBan-V →Fully connected model with parabolic potential
- 09:5409:54, 9 September 2025 diff hist −2 L-6 →Bienaymé Galton Watson process current
- 09:1109:11, 9 September 2025 diff hist +2,500 N TBan-IV Created page with "== Bienaymé Galton Watson process== A time <math> t=0 </math> appears as infected individual which dies with a rate <math> a </math> and branches with a rate <math> b </math>. On average, each infection generates in average <math> R_0 = b/a </math> new ones. Real epidemics corresponds to <math> R_0>1 </math>. At time <math> t </math>, the infected population is <math> n(t) </math>, while the total infected population is <center> <math> N(t) = \int_0^t n(t') d t'..." current
- 09:0809:08, 9 September 2025 diff hist +1 ICTS →Lectures and tutorials current
- 09:0809:08, 9 September 2025 diff hist −2 ICTS →Lectures and tutorials
- 09:0709:07, 9 September 2025 diff hist −8 ICTS →Lectures and tutorials
- 09:0709:07, 9 September 2025 diff hist −24 ICTS →Lectures and tutorials
8 September 2025
- 22:0822:08, 8 September 2025 diff hist +386 LBan-V →Fully connected model with parabolic potential
- 22:0022:00, 8 September 2025 diff hist −236 LBan-V No edit summary
- 21:5921:59, 8 September 2025 diff hist +7,818 N LBan-V Created page with "<Strong> Goal: </Strong> We solve the mean field version of the cellular automaton, derive its avalanche statistics and make a connection with the Bienaymé-Galton-Watson process used to describe an epidemic outbreak. = Fully connected (mean field) model for the cellular automaton= Let's study the mean field version of the cellular automata introduced in the previous lecture. We introduce two approximations: * Replace the Laplacian, which is short range, with a mea..."
- 19:0719:07, 8 September 2025 diff hist +211 LBan-IV →Second moment current
- 19:0319:03, 8 September 2025 diff hist +31 LBan-IV →Second moment
- 16:1916:19, 8 September 2025 diff hist −30 LBan-IV →Second moment
- 16:1716:17, 8 September 2025 diff hist −7 LBan-IV →Second moment
- 16:1616:16, 8 September 2025 diff hist +533 LBan-IV →Second moment