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自旋玻璃与消息传递算法 Spin Glass and Message-Passing Algorithms 周海军 http://www.itp.ac.cn/~zhouhj/ 中国科学院理论物理研究所
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2 提纲 1 。自旋玻璃理论 基本图像与平衡自 由能分布 空腔方法 2 。消息传递算法 Vertex-Cover 问题, 3- SAT 问题 Survey Propagation 算 法
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3 部分参考文献 1.Mezard, Parisi, Virasoro, “Spin Glass Theory and Beyond” (World Scientific, 1987 ) 2.Mezard, Parisi, “The Bethe lattice spin glass revisited”, European Physics Journal B 20: 217-233 (2001) 3.Mezard, Parisi, Zecchina, “Analytic and algorithmic solution of random satisfiability problems”, Science 297: 812-815 (2002) 如果对报告中所涉及的具体模型的计算细节感兴趣,请参考 http://www.itp.ac.cn/~zhouhj/mainen.html
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自旋玻璃理论: 自由能分
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5 Statistical mechanics of a (simple) system in equilibrium is well-established. Partition function, free energy, …. Mean-field treatment. Phase transitions. Correlation length, scaling exponents, …. Renormalization flow.
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6 …, but non-equilibrium dynamics of even a simple system may be difficult to understand Formal framework. Connection with equilibrium. Glassy dynamics. Why relaxation becomes so low and non-exponential? ……
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7 Equilibrium (static) and dynamical properties of complex systems are both difficult and interesting Quenched randomness, frustration, non- self averaging, …, broken ergodicity. NP-complete combinatorial optimizations, message-passing algorithms for information science (CDMA, for example!), econo-physics, …, biological systems.
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8 自旋玻璃:无序与阻错系统的简单模型 3D regular lattice (Edwards-Anderson, 1975) Complete graph (Sherrington-Kirkpatrick 1975) Random Poisson graph (Viana-Bray, 1985)
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9 What we learned from an equilibrium statistical mechanics course?
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10 What we learned from an equilibrium statistical mechanics course? (contl.)
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11 What we learned from an equilibrium statistical mechanics course? (contl.)
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12 ergodic vs non-ergodic ?
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13 repeated heating—annealing and the equilibrium Gibbs measure Complexity (复杂度)
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14 distribution of equilibrium free-energies 1
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15 distribution of equilibrium free-energies (contl.) 2
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17 Which thermodynamic states contribute to the equilibrium properties? If Excited macrostates matter! Macrostates of minimal free energy density matter!
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18 3-spin-Interaction Ising model on a complete graph
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19 the mean free energy density
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20 Overlap Distribution
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自旋玻璃理论: 空腔方法( cavity method)
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22 Let’s define an artificial system!
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23 Some examples of the grand free energy : 2-body interactions Beta=+infinity The max-2-SAT problem Beta=1.25 The +/- J spin-glass model on a random regular graph of degree K=6
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24 How to calculate the grand free energy? The cavity approach
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26 NN+2
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27 Population Dynamics Simulation
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Message-Passing Algorithms
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30 3-SAT 问题
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31 顶点覆盖问题
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32 This graph is covered, but not optimally covered.
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33 Minimal Vertex Cover Problem A vertex cover of the global minimal size. Is a NP-hard optimization problem. Efficient algorithms for constructing near- optimal solutions for a given graph.
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34 There are many optimal solutions for a given graph
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35 Three types of vertices : (1) vertices that are always covered (frozen vertices, ) (2) vertices that are always uncovered (frozen vertices, ) (3) vertices that are covered in some solutions and uncovered in the remaining solutions (unfrozen vertices, )
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36 Mean-field analysis of the minimal vertex cover problem on a random graph
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37 自洽的空穴场方法 覆盖还是不覆盖 ? The vertex cover problem
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38 = always uncovered always covered unfrozen Weigt, Hartmann, PRL (2000), PRE (2001)
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39 New vertex un-covered New vertex partially covered New vertex always covered
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40 Mean-field theory result is lower than experimental values for c > e=2.7183 2.7183
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41 假定的相空间结构
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42 引入参数 y
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43 neighborsvertex iprobabilityVC size increase re-weighted probability all unfrozen or always covered always uncovered 0 at least one always uncovered unfrozen or always covered +1
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46 同样的消息传递的算法可以用于解决 神经网络,信息系统,满足性问题, … , 中的许多计算困难
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47 Program and School in Beijing 2008 ICTP-ITP Spring School on “Statistical Physics and Interdisciplinary Applications” March 03-14, 2008 KITPC Program “Collective Dynamics in Information Systems” March 01-April 15, 2008
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