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Titlebook: Mean Field Models for Spin Glasses; Volume II: Advanced Michel Talagrand Book 2011Latest edition Springer-Verlag GmbH Berlin Heidelberg 20

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樓主: Malevolent
11#
發(fā)表于 2025-3-23 12:23:21 | 只看該作者
12#
發(fā)表于 2025-3-23 14:53:26 | 只看該作者
isce with faint nostalgia on days long past when the artisans of plant physiology, biochemistry, analytical chemistry and other scientific disciplines ebbed and waned in prominence. No intentional reference is made here regarding Darwinism; the plant sciences always have been extremely competitive.
13#
發(fā)表于 2025-3-23 18:31:44 | 只看該作者
isce with faint nostalgia on days long past when the artisans of plant physiology, biochemistry, analytical chemistry and other scientific disciplines ebbed and waned in prominence. No intentional reference is made here regarding Darwinism; the plant sciences always have been extremely competitive.
14#
發(fā)表于 2025-3-23 23:20:12 | 只看該作者
isce with faint nostalgia on days long past when the artisans of plant physiology, biochemistry, analytical chemistry and other scientific disciplines ebbed and waned in prominence. No intentional reference is made here regarding Darwinism; the plant sciences always have been extremely competitive.
15#
發(fā)表于 2025-3-24 03:13:15 | 只看該作者
16#
發(fā)表于 2025-3-24 10:33:35 | 只看該作者
The Gardner Formula for the Discrete CubeThis is a continuation of Chapter 2 of the first volume. It culminates in the proof of the Gardner formula for the cube, which in some sense computes in large dimension . the proportion of the vertices of the unit cube which are contained in the intersection of . random half-spaces for small ..
17#
發(fā)表于 2025-3-24 10:47:50 | 只看該作者
The Hopfield ModelThis is a continuation of Chapter 4 of the first volume. We reach a considerably more detailed understanding of the Hopfield model.
18#
發(fā)表于 2025-3-24 18:11:21 | 只看該作者
19#
發(fā)表于 2025-3-24 22:49:41 | 只看該作者
20#
發(fā)表于 2025-3-25 00:01:50 | 只看該作者
The Parisi SolutionIn the chapter we prove as much as is currently rigorously known about the structure of the Sherrington-Kirkpatrick model at low temperature, and we explain the physicist’s picture. We describe the fundamental problems that remain for a satisfactory understanding: ultrametricity and chaos.
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