User contributions for Rosso
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30 August 2025
- 17:4017:40, 30 August 2025 diff hist +18 L-4 →First Moment
- 17:3817:38, 30 August 2025 diff hist +16 L-4 →First Moment
- 17:3717:37, 30 August 2025 diff hist +44 L-4 →First Moment
- 17:3117:31, 30 August 2025 diff hist +76 L-4 →First Moment
- 17:3117:31, 30 August 2025 diff hist +29 L-4 →First Moment
- 17:3017:30, 30 August 2025 diff hist +54 L-4 →First Moment
- 17:2917:29, 30 August 2025 diff hist +7 L-4 →First Moment
- 17:2817:28, 30 August 2025 diff hist +126 L-4 →First Moment
- 17:2717:27, 30 August 2025 diff hist +67 L-4 →First Moment
- 17:2717:27, 30 August 2025 diff hist +239 L-4 →First Moment
- 17:2617:26, 30 August 2025 diff hist +19 L-4 →Directed Polymer in finite dimension
- 17:2217:22, 30 August 2025 diff hist −37 L-4 →Let's do replica!
- 14:5414:54, 30 August 2025 diff hist +227 L-4 →Let's do replica!
- 14:5314:53, 30 August 2025 diff hist 0 L-4 →Let's do replica!
- 14:5214:52, 30 August 2025 diff hist +98 L-4 →Let's do replica!
- 14:5114:51, 30 August 2025 diff hist +275 L-4 →Let's do replica!
- 14:4514:45, 30 August 2025 diff hist +102 L-4 →Let's do replica!
- 14:3314:33, 30 August 2025 diff hist +2 L-4 →Directed Polymer in finite dimension === State of the Art =
- 14:3314:33, 30 August 2025 diff hist +59 L-4 →KPZ : from 1d to the Cayley tree
- 13:5813:58, 30 August 2025 diff hist −34 L-4 →Let's do replica!
- 13:5613:56, 30 August 2025 diff hist +538 L-4 →Let's do replica!
- 13:5313:53, 30 August 2025 diff hist +150 L-4 →Let's do replica!
- 13:3913:39, 30 August 2025 diff hist −5,859 L-4 No edit summary
27 August 2025
- 19:1519:15, 27 August 2025 diff hist −132 LBan-III →KPZ: from 1D to the Cayley tree current
- 19:1019:10, 27 August 2025 diff hist +1,071 N LBan-III Created page with "= Goal = The goal of this lecture is to present the final lecture on KPZ and directed polymers in finite dimension. We show that for <math>d>2</math>, a "glass transition" occurs. = KPZ: from 1D to the Cayley tree = Much is known about KPZ, but several aspects remain elusive: In <math>d=1</math>, we have <math>\theta=1/3</math> and a glassy regime present at all temperatures. The stationary solution of the KPZ equation describes, at long times, the fluctuations of qu..."
- 19:0619:06, 27 August 2025 diff hist +15 ICTS →Lectures and tutorials
- 19:0619:06, 27 August 2025 diff hist +61 ICTS No edit summary
- 18:1918:19, 27 August 2025 diff hist −168 LBan-II →Remarks
- 18:0818:08, 27 August 2025 diff hist −19 LBan-II →Directed polymers in random media
- 17:2217:22, 27 August 2025 diff hist +621 LBan-II →Directed polymers in random media
26 August 2025
- 18:3718:37, 26 August 2025 diff hist +2 LBan-II →Remarks
- 18:3618:36, 26 August 2025 diff hist +22 LBan-II →Remarks
- 18:3518:35, 26 August 2025 diff hist +76 LBan-II →Remarks
- 18:3518:35, 26 August 2025 diff hist +21 LBan-II →Remarks
- 18:3418:34, 26 August 2025 diff hist +35 LBan-II →Remarks
- 18:3218:32, 26 August 2025 diff hist +87 LBan-II →Remarks
- 18:3118:31, 26 August 2025 diff hist +83 LBan-II →Remarks
- 18:3018:30, 26 August 2025 diff hist +93 LBan-II →Remarks
- 18:2918:29, 26 August 2025 diff hist +190 LBan-II →Remarks
- 18:2918:29, 26 August 2025 diff hist +626 LBan-II →Feynman-Kac formula
- 18:2818:28, 26 August 2025 diff hist +446 LBan-II →Feynman-Kac formula
- 18:2718:27, 26 August 2025 diff hist +954 LBan-II →Feynman-Kac formula
- 18:2618:26, 26 August 2025 diff hist +394 LBan-II →Polymer partition function and propagator of a quantum particle
- 18:2518:25, 26 August 2025 diff hist +1,856 LBan-II →Directed polymers in random media
- 18:2418:24, 26 August 2025 diff hist +5 LBan-II →Directed polymers in random media
- 08:4808:48, 26 August 2025 diff hist +34 LBan-II →Thermal Interfaces
- 08:4508:45, 26 August 2025 diff hist +19 LBan-II →Solution in the Fourier space
25 August 2025
- 18:5418:54, 25 August 2025 diff hist −238 LBan-II →Solution in the Fourier space
- 18:4418:44, 25 August 2025 diff hist +138 LBan-II →Solution in the Fourier space
- 18:4018:40, 25 August 2025 diff hist −23 LBan-II →Width of the interface