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Mathematical Foundations for Search and Surf Engines
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Jean-Louis Lassez
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Ryan Rossi
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Lecture 1 & 2 Introduction Ergodic Theorem Perron-Frobenius Theorem Power Method Foundations of PageRank
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Search Engines Search engine: deterministic Ranking of sites Mathematical foundations: Markov and Perron Frobenius Surf Engines Non deterministic: window shopping Ranking of links Mathematical foundations: Singular Value Decomposition
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Initial approach to ranking sites: the in-degree heuristic 1 2 67 5 3 8 4
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Google’s PageRank approach Problem: rank the sites in order of most visited
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Another Approach: Hubs and Authorities Authorities: sites that contain the most important information Hubs: sites that provide directions to the authorities A H
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Ranking Hyperlinks Local Global Update
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Local ….. ? ? ?
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Global ?? …..
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2005 A C DF E B G H J I K 2006 L Updated
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Part I: Ranking Sites The Web as a Markov Chain The Ergodic Theorem Perron-Frobenius Theorem Algorithms: PageRank, HITS, SALSA
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Markov Chains Text Analysis Speech Recognition Statistical Mechanics Decision Science: Medicine, Commerce ….more recently…..
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Bioinformatics M1M1 M2M2 M3M3 d1d1 I1I1 d2d2 I2I2 d1d1 I1I1
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Internet
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Markov’s Ergodic Theorem (1906) Any irreducible, finite, aperiodic Markov Chain has all states Ergodic (reachable at any time in the future) and has a unique stationary distribution, which is a probability vector.
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s1s1.45 1 s2s2 s3s3 s4s4.25.6.75.55.4 Probabilities after 15 steps X1 =.33 X2 =.26 X3 =.26 X4 =.13 30 steps X1 =.33 X2 =.26 X3 =.23 X4 =.16 100 steps X1 =.37 X2 =.29 X3 =.21 X4 =.13 500 steps X1 =.38 X2 =.28 X3 =.21 X4 =.13 1000 steps X1 =.38 X2 =.28 X3 =.21 X4 =.13
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s1s1.45 1 s2s2 s3s3 s4s4.25.6.75.55.4 Probabilities after 15 steps X1 =.46 X2 =.20 X3 =.26 X4 =.06 30 steps X1 =.36 X2 =.26 X3 =.23 X4 =.13 100 steps X1 =.38 X2 =.28 X3 =.21 X4 =.13 500 steps X1 =.38 X2 =.28 X3 =.21 X4 =.13 1000 steps X1 =.38 X2 =.28 X3 =.21 X4 =.13
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p 11 x 1 + p 21 x 2 + p 31 x 3 = x 1 p 12 x 1 + p 22 x 2 + p 32 x 3 = x 2 p 13 x 1 + p 23 x 2 + p 33 x 3 = x 3 ∑x i = 1 x i ≥ 0 p 11 x 1 + p 21 x 2 + p 31 x 3 = x 1 p 12 x 1 + p 22 x 2 + p 32 x 3 = x 2 p 13 x 1 + p 23 x 2 + p 33 x 3 = x 3 ∑x i = 1 x i ≥ 0 X1, X2, X3 are probabilities p 11 x 1 + p 21 x 2 + p 31 x 3 = x 1 p 12 x 1 + p 22 x 2 + p 32 x 3 = x 2 p 13 x 1 + p 23 x 2 + p 33 x 3 = x 3 ∑x i = 1 x i ≥ 0 Probability of going to S1 from S2 Steady State Constraints
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Solved by Power Iteration Method Based on Perron-Frobenius Theorem Where e is an initial vector and M is the stochastic matrix associated to the system.
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Power Method Example M = 0 1 0 0 1/2 0 1/2 0 0 1/2 1 0 0 0 1 43 2 e = 1 0.3636 0.1818 0.0909
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Power Method Example M = 0 1 0 0 1/2 0 1/2 0 0 1/2 1 0 0 0 1 43 2 e = 2 100 7 3 0.3636 0.1818 0.0909
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Difficulties Proof, Design and Implementation Notion of convergence Deal with complex numbers Unique solution ……… Furthermore, it does not always work
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The process does not converge, even though the solution is obvious. 16 34 52
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Perron-Frobenius Theorem: Is it really necessary?
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Secret Weapon: Fourier Gauss Tarski Robinson The Power of Elimination
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The elimination of the proof is an ideal seldom reached Elimination gives us the heart of the proof
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Symbolic Gaussian Elimination Three variables: p 11 x 1 + p 21 x 2 + p 31 x 3 = x 1 p 12 x 1 + p 22 x 2 + p 32 x 3 = x 2 p 13 x 1 + p 23 x 2 + p 33 x 3 = x 3 ∑x i = 1 with Maple we get: x 1 = (p 31 p 21 + p 31 p 23 + p 32 p 21 ) / Σ x 2 = (p 13 p 32 + p 12 p 31 + p 12 p 32 ) / Σ x 3 = (p 13 p 21 + p 12 p 23 + p 13 p 23 ) / Σ Σ = (p 31 p 21 + p 31 p 23 + p 32 p 21 + p 13 p 32 + p 12 p 31 + p 12 p 32 + p 13 p 21 + p 12 p 23 + p 13 p 23 )
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s1s1 p 12 p 21 p 11 s2s2 p 22 s3s3 p 33 p 13 p 23 p 31 p 32 x 1 = (p 31 p 21 + p 23 p 31 + p 32 p 21 ) / Σ x 2 = (p 13 p 32 + p 31 p 12 + p 12 p 32 ) / Σ x 3 = (p 21 p 13 + p 12 p 23 + p 13 p 23 ) / Σ
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s1s1 p 12 p 21 p 11 s2s2 p 22 s3s3 p 33 p 13 p 23 p 31 p 32 x 1 = (p 31 p 21 + p 23 p 31 + p 32 p 21 ) / Σ x 2 = (p 13 p 32 + p 31 p 12 + p 12 p 32 ) / Σ x 3 = (p 21 p 13 + p 12 p 23 + p 13 p 23 ) / Σ
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s1s1 p 12 p 21 p 11 s2s2 p 22 s3s3 p 33 p 13 p 23 p 31 p 32 x 1 = (p 31 p 21 + p 23 p 31 + p 32 p 21 ) / Σ x 2 = (p 13 p 32 + p 31 p 12 + p 12 p 32 ) / Σ x 3 = (p 21 p 13 + p 12 p 23 + p 13 p 23 ) / Σ
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s1s1 p 12 p 21 p 11 s2s2 p 22 s3s3 p 33 p 13 p 23 p 31 p 32 x 1 = (p 31 p 21 + p 23 p 31 + p 32 p 21 ) / Σ x 2 = (p 13 p 32 + p 31 p 12 + p 12 p 32 ) / Σ x 3 = (p 21 p 13 + p 12 p 23 + p 13 p 23 ) / Σ
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s1s1 p 12 p 21 p 11 s2s2 p 22 s3s3 p 33 p 13 p 23 p 31 p 32 x 1 = (p 31 p 21 + p 23 p 31 + p 32 p 21 ) / Σ x 2 = (p 13 p 32 + p 31 p 12 + p 12 p 32 ) / Σ x 3 = (p 21 p 13 + p 12 p 23 + p 13 p 23 ) / Σ
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s1s1 p 12 p 21 p 11 s2s2 p 22 s3s3 p 33 p 13 p 23 p 31 p 32 x 1 = (p 31 p 21 + p 23 p 31 + p 32 p 21 ) / Σ x 2 = (p 13 p 32 + p 31 p 12 + p 12 p 32 ) / Σ x 3 = (p 21 p 13 + p 12 p 23 + p 13 p 23 ) / Σ
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Symbolic Gaussian Elimination System with four variables: p 21 x 2 + p 31 x 3 + p 41 x 4 = x 1 p 12 x 1 + p 42 x 4 = x 2 p 13 x 1 = x 3 p 34 x 3 = x 4 ∑x i = 1
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s1s1 p 12 p 21 s2s2 s3s3 p 31 s4s4 p 41 p 34 p 42 p 13 x 1 = p 21 p 34 p 41 + p 34 p 42 p 21 + p 21 p 31 p 41 + p 31 p 42 p 21 / Σ x 2 = p 31 p 41 p 12 + p 31 p 42 p 12 + p 34 p 41 p 12 + p 34 p 42 p 12 + p 13 p 34 p 42 / Σ x 3 = p 41 p 21 p 13 + p 42 p 21 p 13 / Σ x 4 = p 21 p 13 p 34 / Σ Σ = p 21 p 34 p 41 + p 34 p 42 p 21 + p 21 p 31 p 41 + p 31 p 42 p 21 + p 31 p 41 p 12 + p 31 p 42 p 12 + p 34 p 41 p 12 + p 34 p 42 p 12 + p 13 p 34 p 42 + p 41 p 21 p 13 + p 42 p 21 p 13 + p 21 p 13 p 34 with Maple we get:
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s1s1 p 12 p 21 s2s2 s3s3 p 31 s4s4 p 41 p 34 p 42 p 13 x 1 = p 21 p 34 p 41 + p 34 p 42 p 21 + p 21 p 31 p 41 + p 31 p 42 p 21 / Σ x 2 = p 31 p 41 p 12 + p 31 p 42 p 12 + p 34 p 41 p 12 + p 34 p 42 p 12 + p 13 p 34 p 42 / Σ x 3 = p 41 p 21 p 13 + p 42 p 21 p 13 / Σ x 4 = p 21 p 13 p 34 / Σ Σ = p 21 p 34 p 41 + p 34 p 42 p 21 + p 21 p 31 p 41 + p 31 p 42 p 21 + p 31 p 41 p 12 + p 31 p 42 p 12 + p 34 p 41 p 12 + p 34 p 42 p 12 + p 13 p 34 p 42 + p 41 p 21 p 13 + p 42 p 21 p 13 + p 21 p 13 p 34
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s1s1 p 12 p 21 s2s2 s3s3 p 31 s4s4 p 41 p 34 p 42 p 13 x 1 = p 21 p 34 p 41 + p 34 p 42 p 21 + p 21 p 31 p 41 + p 31 p 42 p 21 / Σ x 2 = p 31 p 41 p 12 + p 31 p 42 p 12 + p 34 p 41 p 12 + p 34 p 42 p 12 + p 13 p 34 p 42 / Σ x 3 = p 41 p 21 p 13 + p 42 p 21 p 13 / Σ x 4 = p 21 p 13 p 34 / Σ Σ = p 21 p 34 p 41 + p 34 p 42 p 21 + p 21 p 31 p 41 + p 31 p 42 p 21 + p 31 p 41 p 12 + p 31 p 42 p 12 + p 34 p 41 p 12 + p 34 p 42 p 12 + p 13 p 34 p 42 + p 41 p 21 p 13 + p 42 p 21 p 13 + p 21 p 13 p 34
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s1s1 p 12 p 21 s2s2 s3s3 p 31 s4s4 p 41 p 34 p 42 p 13 x 1 = p 21 p 34 p 41 + p 34 p 42 p 21 + p 21 p 31 p 41 + p 31 p 42 p 21 / Σ x 2 = p 31 p 41 p 12 + p 31 p 42 p 12 + p 34 p 41 p 12 + p 34 p 42 p 12 + p 13 p 34 p 42 / Σ x 3 = p 41 p 21 p 13 + p 42 p 21 p 13 / Σ x 4 = p 21 p 13 p 34 / Σ Σ = p 21 p 34 p 41 + p 34 p 42 p 21 + p 21 p 31 p 41 + p 31 p 42 p 21 + p 31 p 41 p 12 + p 31 p 42 p 12 + p 34 p 41 p 12 + p 34 p 42 p 12 + p 13 p 34 p 42 + p 41 p 21 p 13 + p 42 p 21 p 13 + p 21 p 13 p 34
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s1s1 p 12 p 21 s2s2 s3s3 p 31 s4s4 p 41 p 34 p 42 p 13 x 1 = p 21 p 34 p 41 + p 34 p 42 p 21 + p 21 p 31 p 41 + p 31 p 42 p 21 / Σ x 2 = p 31 p 41 p 12 + p 31 p 42 p 12 + p 34 p 41 p 12 + p 34 p 42 p 12 + p 13 p 34 p 42 / Σ x 3 = p 41 p 21 p 13 + p 42 p 21 p 13 / Σ x 4 = p 21 p 13 p 34 / Σ Σ = p 21 p 34 p 41 + p 34 p 42 p 21 + p 21 p 31 p 41 + p 31 p 42 p 21 + p 31 p 41 p 12 + p 31 p 42 p 12 + p 34 p 41 p 12 + p 34 p 42 p 12 + p 13 p 34 p 42 + p 41 p 21 p 13 + p 42 p 21 p 13 + p 21 p 13 p 34
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Do you see the LIGHT? James Brown (The Blues Brothers)
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s1s1 p 12 p 21 s2s2 s3s3 p 31 s4s4 p 41 p 34 p 42 p 13 x 1 = p 21 p 34 p 41 + p 34 p 42 p 21 + p 21 p 31 p 41 + p 31 p 42 p 21 / Σ x 2 = p 31 p 41 p 12 + p 31 p 42 p 12 + p 34 p 41 p 12 + p 34 p 42 p 12 + p 13 p 34 p 42 / Σ x 3 = p 41 p 21 p 13 + p 42 p 21 p 13 / Σ x 4 = p 21 p 13 p 34 / Σ Σ = p 21 p 34 p 41 + p 34 p 42 p 21 + p 21 p 31 p 41 + p 31 p 42 p 21 + p 31 p 41 p 12 + p 31 p 42 p 12 + p 34 p 41 p 12 + p 34 p 42 p 12 + p 13 p 34 p 42 + p 41 p 21 p 13 + p 42 p 21 p 13 + p 21 p 13 p 34
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Ergodic Theorem Revisited If there exists a reverse spanning tree in a graph of the Markov chain associated to a stochastic system, then: (a)the stochastic system admits the following probability vector as a solution: (b) the solution is unique. (c) the conditions {x i ≥ 0} i=1,n are redundant and the solution can be computed by Gaussian elimination.
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Cycle This system is now covered by the proof 1 6 3 4 5 2
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Markov Chain as a Conservation System s1s1 p 12 p 21 p 11 s2s2 p 22 s3s3 p 33 p 13 p 23 p 31 p 32 p 11 x 1 + p 21 x 2 + p 31 x 3 = x 1 (p 11 + p 12 + p 13 ) p 12 x 1 + p 22 x 2 + p 32 x 3 = x 2 (p 21 + p 22 + p 23 ) p 13 x 1 + p 23 x 2 + p 33 x 3 = x 3 (p 31 + p 32 + p 33 )
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Kirchoff’s Current Law (1847) The sum of currents flowing towards a node is equal to the sum of currents flowing away from the node. i 31 + i 21 = i 12 + i 13 i 32 + i 12 = i 21 i 13 = i 31 + i 32 12 3 i 13 i 31 i 32 i 12 i 21 i 3 + i 2 = i 1 + i 4
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Kirchhoff’s Matrix Tree Theorem (1847) The theorem allows us to calculate the number of spanning trees of a connected graph
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Two theorems for the price of one!! Differences Ergodic Theorem: The symbolic proof is simpler and more appropriate than using Perron-Frobenius Kirchhoff Theorem: Our version calculates the spanning trees and not their total sum.
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Internet Sites Kleinberg Google SALSA Indegree Heuristic
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Google PageRank Patent “The rank of a page can be interpreted as the probability that a surfer will be at the page after following a large number of forward links.” The Ergodic Theorem
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Google PageRank Patent “The iteration circulates the probability through the linked nodes like energy flows through a circuit and accumulates in important places.” Kirchoff (1847)
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Rank Sinks 5 6 7 1 2 3 4 No Spanning Tree
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References Kirchhoff, G. "Über die Auflösung der Gleichungen, auf welche man bei der untersuchung der linearen verteilung galvanischer Ströme geführt wird." Ann. Phys. Chem. 72, 497-508, 1847. А. А. Марков. "Распространение закона больших чисел на величины, зависящие друг от друга". "Известия Физико-математического общества при Казанском университете", 2-я серия, том 15, ст. 135-156, 1906. H. Minkowski, Geometrie der Zahlen (Leipzig, 1896). J. Farkas, "Theorie der einfachen Ungleichungen," J. F. Reine u. Ang. Mat., 124, 1-27, 1902. H. Weyl, "Elementare Theorie der konvexen Polyeder," Comm. Helvet., 7, 290-306, 1935. A. Charnes, W. W. Cooper, “The Strong Minkowski Farkas-Weyl Theorem for Vector Spaces Over Ordered Fields,” Proceedings of the National Academy of Sciences, pp. 914-916, 1958.
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References E. Steinitz. Bedingt Konvergente Reihen und Konvexe Systeme. J. reine angew. Math., 146:1-52, 1916. K. Jeev, J-L. Lassez: Symbolic Stochastic Systems. MSV/AMCS 2004: 321- 328 V. Chandru, J-L. Lassez: Qualitative Theorem Proving in Linear Constraints. Verification: Theory and Practice 2003: 395-406 Jean-Louis Lassez: From LP to LP: Programming with Constraints. DBPL 1991 : 257-283
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