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• 15:47, 2 March 2025 Ros talk contribs created page File:2025 Parisi scheme.pdf
• 15:47, 2 March 2025 Ros talk contribs uploaded File:2025 Parisi scheme.pdf
• 15:46, 2 March 2025 Ros talk contribs deleted page File:2025 Parisi scheme.pdf
• 15:42, 2 March 2025 Ros talk contribs created page File:2025 Parisi scheme.pdf
• 15:42, 2 March 2025 Ros talk contribs uploaded File:2025 Parisi scheme.pdf
• 15:41, 2 March 2025 Ros talk contribs deleted page File:2025 parisi scheme.pdf
• 16:42, 26 February 2025 Ros talk contribs created page File:2025 parisi scheme.pdf
• 16:42, 26 February 2025 Ros talk contribs uploaded File:2025 parisi scheme.pdf
• 16:41, 26 February 2025 Ros talk contribs deleted page File:The Parisi Scheme.pdf
• 16:06, 26 February 2025 Ros talk contribs created page File:2025 HW2.pdf
• 16:06, 26 February 2025 Ros talk contribs uploaded File:2025 HW2.pdf
• 16:04, 26 February 2025 Ros talk contribs created page File:2025 P5 solutions.pdf
• 16:04, 26 February 2025 Ros talk contribs uploaded File:2025 P5 solutions.pdf
• 16:03, 26 February 2025 Ros talk contribs deleted page File:2024 TD5 solutions.pdf
• 16:02, 26 February 2025 Ros talk contribs created page File:2025 P6 solutions .pdf
• 16:02, 26 February 2025 Ros talk contribs uploaded File:2025 P6 solutions .pdf
• 16:01, 26 February 2025 Ros talk contribs deleted page File:2024 TD6 solutions .pdf
• 19:58, 9 February 2025 Ros talk contribs created page File:2025 P4 solutions.pdf
• 19:58, 9 February 2025 Ros talk contribs uploaded File:2025 P4 solutions.pdf
• 19:58, 9 February 2025 Ros talk contribs created page File:2025 P2 solutions.pdf
• 19:58, 9 February 2025 Ros talk contribs uploaded File:2025 P2 solutions.pdf
• 19:57, 9 February 2025 Ros talk contribs deleted page File:2025 P2 solutions.pdf
• 19:57, 9 February 2025 Ros talk contribs deleted page File:2025 P4 solutions.pdf
• 19:34, 9 February 2025 Ros talk contribs uploaded File:2025 P4 solutions.pdf
• 19:34, 9 February 2025 Ros talk contribs created page File:2025 P4 solutions.pdf
• 19:01, 9 February 2025 Ros talk contribs created page File:2025 P3 solutions.pdf
• 19:01, 9 February 2025 Ros talk contribs uploaded File:2025 P3 solutions.pdf
• 23:44, 4 February 2025 Rosso talk contribs created page File:RMT introduction.pdf (new file without misprints)
• 23:44, 4 February 2025 Rosso talk contribs uploaded File:RMT introduction.pdf (new file without misprints)
• 20:52, 26 January 2025 Ros talk contribs created page File:2025 P2 solutions.pdf
• 20:52, 26 January 2025 Ros talk contribs uploaded File:2025 P2 solutions.pdf
• 20:51, 26 January 2025 Ros talk contribs deleted page File:2024 TD2 solutions.pdf
• 20:50, 26 January 2025 Ros talk contribs created page File:2025 P1 solutions.pdf
• 20:50, 26 January 2025 Ros talk contribs uploaded File:2025 P1 solutions.pdf
• 20:49, 26 January 2025 Ros talk contribs deleted page File:2024 TD1 solutions.pdf
• 13:32, 20 January 2025 Ros talk contribs created page File:HW2025 RMT.pdf
• 13:32, 20 January 2025 Ros talk contribs uploaded File:HW2025 RMT.pdf
• 10:54, 15 September 2024 Ros talk contribs created page File:2024 TD2 solutions.pdf
• 10:54, 15 September 2024 Ros talk contribs uploaded File:2024 TD2 solutions.pdf
• 10:52, 15 September 2024 Ros talk contribs deleted page File:2024 TD2 solutions.pdf
• 10:40, 15 September 2024 Ros talk contribs created page File:2024 TD2 solutions.pdf
• 10:40, 15 September 2024 Ros talk contribs uploaded File:2024 TD2 solutions.pdf
• 10:38, 15 September 2024 Ros talk contribs deleted page File:2024 TD2 solutions.pdf
• 16:25, 24 March 2024 Rosso talk contribs created page L-9 (Created page with "=Multifractality= In the last lecture we discussed that the eigenstates of the Anderson model can be localized, delocalized or multifractal. The idea is to look at the (generalized) IPR <center><math> IPR(q)=\sum_n |\psi_n|^{2 q} \sim L^{-\tau_q} </math></center> The exponent <math>\tau_q</math> is called <Strong> multifractal exponent </Strong>. Normalization imposes <math>\tau_1 =0 </math> and the fact that the wave fuction is defined everywhere that <math>\tau_0 =-d...")
• 16:04, 24 March 2024 Ros talk contribs created page File:2024 TD9 solutions.pdf
• 16:04, 24 March 2024 Ros talk contribs uploaded File:2024 TD9 solutions.pdf
• 18:35, 22 March 2024 Ros talk contribs created page File:Bethe I(beta).png
• 18:35, 22 March 2024 Ros talk contribs uploaded File:Bethe I(beta).png
• 14:50, 20 March 2024 Ros talk contribs uploaded a new version of File:2024 TD8 solutions.pdf
• 11:52, 16 March 2024 Rosso talk contribs created page L-8 (Created page with "<Strong>Goal:</Strong> we will introduce the Anderson model, discuss the behaviour as a function of the dimension. In 1d localization can be connected to the product of random matrices. = Anderson model (tight bindind model)= We consider a lattice with non-interacting particles hopping between nearest neighbors and feeling on-site disorder. The hamiltonian reads: <center> <math> H= - t \sum_{ <i, j> } (c_i c_j +c_j c_i) \sum_i \epsilon_i c_i c_i </math></center>")