Bourgain s Theorem. Computational and Metric Geometry. Instructor: Yury Makarychev. d(s 1, s 2 ).
|
|
- Alvin Morris
- 6 years ago
- Views:
Transcription
1 Bourgain s Theorem Computationa and Metric Geometry Instructor: Yury Makarychev 1 Notation Given a metric space (X, d) and S X, the distance from x X to S equas d(x, S) = inf d(x, s). s S The distance between two sets S 1, S 2 X equas d(s 1, S 2 ) = inf s 1 S 1,s 2 S 2 d(s 1, s 2 ). Exercise 1. Show that distances between sets do not necessariy satisfy the triange inequaity. That is, it is possibe that d(s 1, S 2 ) + d(s 2, S 3 ) > d(s 1, S 3 ) for some sets S 1, S 2 and S 3. Exercise 2. Prove that d(x, y) d(s, x) d(s, y) and thus d(x, y) d(s, x) d(s, y). Proof. Fix ε >. Let y S be such that d(y, y) d(s, y) + ε (if S is a finite set, there is y S s.t. d(y, y ) = d(s, y)). Then d(x, S) d(x, y ) d(x, y) + d(y, y ) d(x, y) + d(s, y) + ε. We proved that d(x, S) d(x, y) + d(s, y) + ε for every ε >. Therefore, d(x, S) d(x, y) + d(s, y). Definition 1.1. Let (X, d) be a metric space, x X and r >. The (cosed) ba of radius r around x is B r (x ) = Ba r (x ) = {x : d(x, x ) r}. 1
2 2 Warm-up Consider two normed spaces (U, U ) and (V, V ). Let f be a inear operator between U and V. What is the Lipschitz norm of f? It is equa f(x) f(y) V sup x,y U x y U x y by inearity of f f(x y) V = sup x,y U x y U x y f(z) V = sup. z U z U z f(z) The expression sup V z U z z U is caed the operator norm of f. The above computation shows that the Lipschitz norm of a inear operator equas its operator norm. At the previous ecture, we proved that q p and L p [, s] L q [, s] when p < q and a, b R. These embeddings define incusion maps i 1 : p q and i 2 : L q [, s] L p [, s] defined by i 1 (a) = a for every a p i 2 (f) = f for every f L q [, s]. Note that even though maps i 1 and i 2 do not do much they just map every eement to itsef they are not ow distortion maps! Exercise 3. Compute the Lipschitz norm and distortion of map i 1 : p q. Soution. Consider a p. Note that a j a p and a j q = a j p a j q p a j p a q p p. Therefore, a q q = a j q a j p a q p p = ( aj p ) a q p p = a p p a q p p = a q p. We get that a q a p. That is, i 1 Lip 1. On the other hand, e 1 p = e 1 q = 1, where e 1 = (1,,... ). We get, i 1 Lip = 1. Now et n 1. Consider a = ( 1,..., 1 }{{},,... ) p. We have, a p = n 1/p and n coordinates a q = n 1/q. Thus i 1 1 Lip a p / a q = n 1/p /n 1/q = n 1/p 1/q. Since n 1/p 1/q as n, the norm f 1 Lip is unbounded. Answer: i 1 Lip = 1, i 1 has infinite distortion. We wi need the foowing inequaity. Theorem 2.1 (Lyapunov s inequaity). Let 1 p < q =. For every random variabe α with finite q-th moment, we have α p α q. Proof. The statement is obvious for q = since α < α amost surey. Let us assume that q <. Let f(x) = x q/p for x. Note that f(x) is a convex function. Let β = α p (β is a random variabe). We have α q q = E [ α q ] = E [ β q/p] = E [f( β )] We concude that α q α p as required. by Jensen s Inequaity f(e [ β ]) = (E [ α p ]) q/p. 2
3 Exercise 4. Compute the Lipschitz norm and distortion of map i 2 : L q [, s] L p [, s]. Proof. First, consider f(x) = 1, a constant function defined on [, s]. We have f Lp = s 1/p and f Lq = s 1/q. Therefore, i 2 Lip i 2(f) p f q = s 1/p 1/q. Now consider f L q [, s]. Let ξ be a random variabe uniformy distributed on [, s]. Note that for every function h on [, s], we have s h(x)dx = s 1 h(ys)dy = se [h(ξ)]. Therefore, f p L p = se [ f(ξ) p ] = s f(ξ) p p, and f Lp = s 1/p f(ξ) p (here, f(ξ) is a random variabe). Simiary, f Lq = s 1/q f(ξ) q. By Lyapunov s inequaity for α = f(ξ), f Lp = s 1/p f(ξ) p s 1/p f(ξ) q = s 1/p 1/q ( s 1/q f(ξ) q ) = s 1/p 1/q f Lq. We get that f Lip s 1/p 1/q and therefore f Lip = s 1/p 1/q Let ε (, 1). Consider f ε (x) = x 1 ε q. We compute its p and q norms and get that f ε p (qs q p q q p ) 1/p < as ε, f ε q as ε. Therefore, i 2 has infinite distortion. Answer: i 2 Lip = s 1/p 1/q, i 2 has infinite distortion. 3 Bourgain s Theorem Definition 3.1. Let X be a finite metric space and p 1. Suppose that Z is a random subset of X (chosen according to some probabiity distribution). For every u X, define random variabe ξ u = d(u, Z) = min z Z d(u, z). Consider the map f from X to the space of random variabes L p (Ω, µ) that sends u to ξ u (where Ω is the probabiity space and µ is the probabiity measure on Ω). We say that f is a Fréchet embedding. Lemma 3.2. Every Fréchet embedding f is non-expanding. That is, f Lip 1. Proof. Consider a Fréchet embedding that sends u to ξ u = d(u, Z). For every u, v X, we have ξ u ξ v p = (E [ d(u, Z) d(v, Z) p by Exercise 2 1/p ]) (E [ d(u, v) p ]) 1/p = d(u, v). 3
4 Remark 3.3. If X is infinite, then the random variabe ξ u = d(u, Z) does not necessariy beong to L p (Ω, µ) (its p-norm might be infinite). However, we can define ξ u as ξ u = d(u, Z) d(x, Z), where x is some point in X. Then the proof of Lemma 3.2 shows that ξ u p d(u, x ) < and the map f : u ξ u is non-expanding. Theorem 3.4 (Bourgain s Theorem). Every metric space X on n points embeds into L p (X, µ) with distortion O(og n) (for every p 1). That is, c p (X) = O(og n). Proof. Let = og 2 n + 1. Construct a random set Z as foows. Choose s uniformy at random from {1,..., }. Initiay, et Z =. Add every point of X to Z with probabiity 1/2 s, independenty. Now et f be the Fréchet embedding that maps u X to random variabe ξ u = d(z, u). By Lemma 3.2, f is non-expanding. We are going to prove that for every u and v, f(u) f(v) p c d(u, v), for some absoute constant c. Note that it is sufficient to prove this statement for p = 1, since by Lyapunov s inequaity f(u) f(v) p f(u) f(v) 1. Consider two points u and v. Let = d(u, v)/2. Write, [ ] f(u) f(v) 1 = E [ d(u, Z) d(v, Z) ] = E dt [d(u,z),d(v,z)) [d(v,z),d(u,z)) (by Fubini s theorem) = Pr (d(u, Z) t < d(v, Z) or d(v, Z) t < d(u, Z)) dt Pr (d(u, Z) t < d(v, Z) or d(v, Z) t < d(u, Z)) dt. We now prove that Pr (d(u, Z) t < d(v, Z) or d(v, Z) t < d(u, Z)) Ω(1) if t (, ). That wi impy that f(u) f(v) 1 Ω(1) = Ω(1) d(u, v). We fix t (, ). Consider bas B t (u) and B t (v). Note that they are disjoint since 2t < 2 = d(u, v). Assume without oss of generaity that B t (u) B t (v). Denote m = B t (u). Let s = og 2 m + 1. Then m < 2 s 2m. Let E u be the event that d(u, Z) > t and E v be the event that d(v, Z) t. We have, Pr (d(u, Z) < t < d(v, Z) or d(v, Z) < t < d(u, Z)) Pr (E u and E v ). Note that the event E v occurs if and ony if there is a point in Z at distance at most t from v; that is, when B t (v) Z. The event E u occurs if and ony if B t (u) Z =. 4
5 Consider the event s = s. It happens with probabiity 1/. Conditioned on this event, events E u and E v are independent (since B t (u) and B t (v) are disjoint) and Pr(E u s = s ) = Pr (w / Z s = s ) = ( 1 1 ) ( = 1 1 ) m 1 2 s 2 s e. w B t(u) w B t(u) Pr(E v s = s ) = 1 Pr (w / Z s = s ) = 1 ( 1 1 ) ( ) m 2 s 2 s We get w B t(v) 1 1 e 1/2. w B t(v) Pr (d(u, Z) < t < d(v, Z) or d(v, Z) < t < d(u, Z)) Pr (E u and E v ) 1 Pr (E u s = s ) Pr (E v s = s ) Ω ( ) 1. Exercise 5. The set Z might be equa to in our proof, then random variabes ξ u = d(u, Z) are not we defined. Show how to fix this probem. Proof. There are many ways to fix this probem. For instance, we can add an extra point x to the metric space X, and define d(u, x ) = 2 diam(x), where diam(x) = max u,v X d(u, v). Then construct the set Z as before, except that aways add x to Z. Thus we ensure that Z. In other words, we can define ξ u as before if Z, and ξ u = 2 diam(x) if Z =. The rest of the proof goes through without any other changes. The proof of Bourgain s theorem provides an efficient randomized procedure for generating set Z. As presented here, this procedure gives an embedding ony in L p (Ω, µ) and not in N p. We aready know that if a set of n points embeds in L p (Ω, µ) with distortion D then it embeds in (n 2) p with distortion D. However, in fact, we need ony N = O((og n) 2 ) dimensions: for every vaue of s {1,..., } we make Θ(og n) sampes of the set Z. Then the tota number of sampes equas Θ((og n) 2 ). Using the Chernoff bound, it is easy to show that the distortion of the obtained embedding is O(og n) w.h.p. Fact 3.5 (Matoušek). Let D n,p be the smaest number D such that every metric space on n points embeds in p with distortion at most D n,p. Then ( ) og n D n,p = Θ. p 5
Basic Properties of Metric and Normed Spaces
Basic Properties of Metric and Normed Spaces Computational and Metric Geometry Instructor: Yury Makarychev The second part of this course is about metric geometry. We will study metric spaces, low distortion
More informationBASIC NOTIONS AND RESULTS IN TOPOLOGY. 1. Metric spaces. Sets with finite diameter are called bounded sets. For x X and r > 0 the set
BASIC NOTIONS AND RESULTS IN TOPOLOGY 1. Metric spaces A metric on a set X is a map d : X X R + with the properties: d(x, y) 0 and d(x, y) = 0 x = y, d(x, y) = d(y, x), d(x, y) d(x, z) + d(z, y), for a
More informationMat 1501 lecture notes, penultimate installment
Mat 1501 ecture notes, penutimate instament 1. bounded variation: functions of a singe variabe optiona) I beieve that we wi not actuay use the materia in this section the point is mainy to motivate the
More informationThe arc is the only chainable continuum admitting a mean
The arc is the ony chainabe continuum admitting a mean Aejandro Ianes and Hugo Vianueva September 4, 26 Abstract Let X be a metric continuum. A mean on X is a continuous function : X X! X such that for
More informationFinite Metric Spaces & Their Embeddings: Introduction and Basic Tools
Finite Metric Spaces & Their Embeddings: Introduction and Basic Tools Manor Mendel, CMI, Caltech 1 Finite Metric Spaces Definition of (semi) metric. (M, ρ): M a (finite) set of points. ρ a distance function
More informationLemma 1. Suppose K S is a compact subset and I α is a covering of K. There is a finite subcollection {I j } such that
2 Singuar Integras We start with a very usefu covering emma. Lemma. Suppose K S is a compact subset and I α is a covering of K. There is a finite subcoection {I j } such that. {I j } are disjoint. 2. The
More informationPartitioning Metric Spaces
Partitioning Metric Spaces Computational and Metric Geometry Instructor: Yury Makarychev 1 Multiway Cut Problem 1.1 Preliminaries Definition 1.1. We are given a graph G = (V, E) and a set of terminals
More informationLecture Notes 4: Fourier Series and PDE s
Lecture Notes 4: Fourier Series and PDE s 1. Periodic Functions A function fx defined on R is caed a periodic function if there exists a number T > such that fx + T = fx, x R. 1.1 The smaest number T for
More informationHomework 5 Solutions
Stat 310B/Math 230B Theory of Probabiity Homework 5 Soutions Andrea Montanari Due on 2/19/2014 Exercise [5.3.20] 1. We caim that n 2 [ E[h F n ] = 2 n i=1 A i,n h(u)du ] I Ai,n (t). (1) Indeed, integrabiity
More informationTools from Lebesgue integration
Tools from Lebesgue integration E.P. van den Ban Fall 2005 Introduction In these notes we describe some of the basic tools from the theory of Lebesgue integration. Definitions and results will be given
More informationEcon Lecture 3. Outline. 1. Metric Spaces and Normed Spaces 2. Convergence of Sequences in Metric Spaces 3. Sequences in R and R n
Econ 204 2011 Lecture 3 Outline 1. Metric Spaces and Normed Spaces 2. Convergence of Sequences in Metric Spaces 3. Sequences in R and R n 1 Metric Spaces and Metrics Generalize distance and length notions
More informationSobolev Spaces. Chapter Hölder spaces
Chapter 2 Sobolev Spaces Sobolev spaces turn out often to be the proper setting in which to apply ideas of functional analysis to get information concerning partial differential equations. Here, we collect
More informationBy (a), B ε (x) is a closed subset (which
Solutions to Homework #3. 1. Given a metric space (X, d), a point x X and ε > 0, define B ε (x) = {y X : d(y, x) ε}, called the closed ball of radius ε centered at x. (a) Prove that B ε (x) is always a
More informationSample Problems for Third Midterm March 18, 2013
Mat 30. Treibergs Sampe Probems for Tird Midterm Name: Marc 8, 03 Questions 4 appeared in my Fa 000 and Fa 00 Mat 30 exams (.)Let f : R n R n be differentiabe at a R n. (a.) Let g : R n R be defined by
More informationPhysics 235 Chapter 8. Chapter 8 Central-Force Motion
Physics 35 Chapter 8 Chapter 8 Centra-Force Motion In this Chapter we wi use the theory we have discussed in Chapter 6 and 7 and appy it to very important probems in physics, in which we study the motion
More informationA. Distribution of the test statistic
A. Distribution of the test statistic In the sequentia test, we first compute the test statistic from a mini-batch of size m. If a decision cannot be made with this statistic, we keep increasing the mini-batch
More informationThe Construction of a Pfaff System with Arbitrary Piecewise Continuous Characteristic Power-Law Functions
Differentia Equations, Vo. 41, No. 2, 2005, pp. 184 194. Transated from Differentsia nye Uravneniya, Vo. 41, No. 2, 2005, pp. 177 185. Origina Russian Text Copyright c 2005 by Izobov, Krupchik. ORDINARY
More informationOn colorings of the Boolean lattice avoiding a rainbow copy of a poset arxiv: v1 [math.co] 21 Dec 2018
On coorings of the Booean attice avoiding a rainbow copy of a poset arxiv:1812.09058v1 [math.co] 21 Dec 2018 Baázs Patkós Afréd Rényi Institute of Mathematics, Hungarian Academy of Scinces H-1053, Budapest,
More informationAkaike Information Criterion for ANOVA Model with a Simple Order Restriction
Akaike Information Criterion for ANOVA Mode with a Simpe Order Restriction Yu Inatsu * Department of Mathematics, Graduate Schoo of Science, Hiroshima University ABSTRACT In this paper, we consider Akaike
More informationWave Equation Dirichlet Boundary Conditions
Wave Equation Dirichet Boundary Conditions u tt x, t = c u xx x, t, < x 1 u, t =, u, t = ux, = fx u t x, = gx Look for simpe soutions in the form ux, t = XxT t Substituting into 13 and dividing
More informationWeek 6 Lectures, Math 6451, Tanveer
Fourier Series Week 6 Lectures, Math 645, Tanveer In the context of separation of variabe to find soutions of PDEs, we encountered or and in other cases f(x = f(x = a 0 + f(x = a 0 + b n sin nπx { a n
More informationAutomobile Prices in Market Equilibrium. Berry, Pakes and Levinsohn
Automobie Prices in Market Equiibrium Berry, Pakes and Levinsohn Empirica Anaysis of demand and suppy in a differentiated products market: equiibrium in the U.S. automobie market. Oigopoistic Differentiated
More information2 (Bonus). Let A X consist of points (x, y) such that either x or y is a rational number. Is A measurable? What is its Lebesgue measure?
MA 645-4A (Real Analysis), Dr. Chernov Homework assignment 1 (Due 9/5). Prove that every countable set A is measurable and µ(a) = 0. 2 (Bonus). Let A consist of points (x, y) such that either x or y is
More informationLecture Note 3: Stationary Iterative Methods
MATH 5330: Computationa Methods of Linear Agebra Lecture Note 3: Stationary Iterative Methods Xianyi Zeng Department of Mathematica Sciences, UTEP Stationary Iterative Methods The Gaussian eimination (or
More informationANALYSIS QUALIFYING EXAM FALL 2017: SOLUTIONS. 1 cos(nx) lim. n 2 x 2. g n (x) = 1 cos(nx) n 2 x 2. x 2.
ANALYSIS QUALIFYING EXAM FALL 27: SOLUTIONS Problem. Determine, with justification, the it cos(nx) n 2 x 2 dx. Solution. For an integer n >, define g n : (, ) R by Also define g : (, ) R by g(x) = g n
More information6 Wave Equation on an Interval: Separation of Variables
6 Wave Equation on an Interva: Separation of Variabes 6.1 Dirichet Boundary Conditions Ref: Strauss, Chapter 4 We now use the separation of variabes technique to study the wave equation on a finite interva.
More informationSobolev Spaces. Chapter 10
Chapter 1 Sobolev Spaces We now define spaces H 1,p (R n ), known as Sobolev spaces. For u to belong to H 1,p (R n ), we require that u L p (R n ) and that u have weak derivatives of first order in L p
More informationCS229 Lecture notes. Andrew Ng
CS229 Lecture notes Andrew Ng Part IX The EM agorithm In the previous set of notes, we taked about the EM agorithm as appied to fitting a mixture of Gaussians. In this set of notes, we give a broader view
More informationCourse 2BA1, Section 11: Periodic Functions and Fourier Series
Course BA, 8 9 Section : Periodic Functions and Fourier Series David R. Wikins Copyright c David R. Wikins 9 Contents Periodic Functions and Fourier Series 74. Fourier Series of Even and Odd Functions...........
More informationEmpty non-convex and convex four-gons in random point sets
Empty non-convex and convex four-gons in random point sets Ruy Fabia-Monroy 1, Cemens Huemer, and Dieter Mitsche 3 1 Departamento de Matemáticas, CINVESTAV-IPN, México Universitat Poitècnica de Cataunya,
More information8 APPENDIX. E[m M] = (n S )(1 exp( exp(s min + c M))) (19) E[m M] n exp(s min + c M) (20) 8.1 EMPIRICAL EVALUATION OF SAMPLING
8 APPENDIX 8.1 EMPIRICAL EVALUATION OF SAMPLING We wish to evauate the empirica accuracy of our samping technique on concrete exampes. We do this in two ways. First, we can sort the eements by probabiity
More informationExam 2 extra practice problems
Exam 2 extra practice problems (1) If (X, d) is connected and f : X R is a continuous function such that f(x) = 1 for all x X, show that f must be constant. Solution: Since f(x) = 1 for every x X, either
More informationLecture Notes for Math 251: ODE and PDE. Lecture 34: 10.7 Wave Equation and Vibrations of an Elastic String
ecture Notes for Math 251: ODE and PDE. ecture 3: 1.7 Wave Equation and Vibrations of an Eastic String Shawn D. Ryan Spring 212 ast Time: We studied other Heat Equation probems with various other boundary
More informationCoupling of LWR and phase transition models at boundary
Couping of LW and phase transition modes at boundary Mauro Garaveo Dipartimento di Matematica e Appicazioni, Università di Miano Bicocca, via. Cozzi 53, 20125 Miano Itay. Benedetto Piccoi Department of
More informationPROCEEDINGS OF THE YEREVAN STATE UNIVERSITY GEOMETRIC PROBABILITY CALCULATION FOR A TRIANGLE
PROCEEDINGS OF THE YEREVAN STATE UNIVERSITY Physica and Mathematica Sciences 07, 5(3, p. 6 M a t h e m a t i c s GEOMETRIC PROBABILITY CALCULATION FOR A TRIANGLE N. G. AHARONYAN, H. O. HARUTYUNYAN Chair
More informationg 2 (x) (1/3)M 1 = (1/3)(2/3)M.
COMPACTNESS If C R n is closed and bounded, then by B-W it is sequentially compact: any sequence of points in C has a subsequence converging to a point in C Conversely, any sequentially compact C R n is
More informationLecture 10: Bourgain s Theorem
princeton u. sp 0 cos 598B: algorithms and complexity Lecture 10: Bourgain s Theorem Lecturer: Sanjeev Arora Scribe:Daniel J. Peng The goal of this week s lecture is to prove the l version of Bourgain
More informationStatistical Learning Theory: A Primer
Internationa Journa of Computer Vision 38(), 9 3, 2000 c 2000 uwer Academic Pubishers. Manufactured in The Netherands. Statistica Learning Theory: A Primer THEODOROS EVGENIOU, MASSIMILIANO PONTIL AND TOMASO
More informationA CLUSTERING LAW FOR SOME DISCRETE ORDER STATISTICS
J App Prob 40, 226 241 (2003) Printed in Israe Appied Probabiity Trust 2003 A CLUSTERING LAW FOR SOME DISCRETE ORDER STATISTICS SUNDER SETHURAMAN, Iowa State University Abstract Let X 1,X 2,,X n be a sequence
More informationSolution Sheet 3. Solution Consider. with the metric. We also define a subset. and thus for any x, y X 0
Solution Sheet Throughout this sheet denotes a domain of R n with sufficiently smooth boundary. 1. Let 1 p
More informationMATH 172: MOTIVATION FOR FOURIER SERIES: SEPARATION OF VARIABLES
MATH 172: MOTIVATION FOR FOURIER SERIES: SEPARATION OF VARIABLES Separation of variabes is a method to sove certain PDEs which have a warped product structure. First, on R n, a inear PDE of order m is
More informationExplicit overall risk minimization transductive bound
1 Expicit overa risk minimization transductive bound Sergio Decherchi, Paoo Gastado, Sandro Ridea, Rodofo Zunino Dept. of Biophysica and Eectronic Engineering (DIBE), Genoa University Via Opera Pia 11a,
More information18.409: Topics in TCS: Embeddings of Finite Metric Spaces. Lecture 6
Massachusetts Institute of Technology Lecturer: Michel X. Goemans 8.409: Topics in TCS: Embeddings of Finite Metric Spaces September 7, 006 Scribe: Benjamin Rossman Lecture 6 Today we loo at dimension
More informationMath 124B January 17, 2012
Math 124B January 17, 212 Viktor Grigoryan 3 Fu Fourier series We saw in previous ectures how the Dirichet and Neumann boundary conditions ead to respectivey sine and cosine Fourier series of the initia
More informationFréchet embeddings of negative type metrics
Fréchet embeddings of negative type metrics Sanjeev Arora James R Lee Assaf Naor Abstract We show that every n-point metric of negative type (in particular, every n-point subset of L 1 ) admits a Fréchet
More informationResearch Article On the Lower Bound for the Number of Real Roots of a Random Algebraic Equation
Appied Mathematics and Stochastic Anaysis Voume 007, Artice ID 74191, 8 pages doi:10.1155/007/74191 Research Artice On the Lower Bound for the Number of Rea Roots of a Random Agebraic Equation Takashi
More informationProblem set 6 The Perron Frobenius theorem.
Probem set 6 The Perron Frobenius theorem. Math 22a4 Oct 2 204, Due Oct.28 In a future probem set I want to discuss some criteria which aow us to concude that that the ground state of a sef-adjoint operator
More informationNOISE-INDUCED STABILIZATION OF STOCHASTIC DIFFERENTIAL EQUATIONS
NOISE-INDUCED STABILIZATION OF STOCHASTIC DIFFERENTIAL EQUATIONS TONY ALLEN, EMILY GEBHARDT, AND ADAM KLUBALL 3 ADVISOR: DR. TIFFANY KOLBA 4 Abstract. The phenomenon of noise-induced stabiization occurs
More informationMathematics for Economists
Mathematics for Economists Victor Filipe Sao Paulo School of Economics FGV Metric Spaces: Basic Definitions Victor Filipe (EESP/FGV) Mathematics for Economists Jan.-Feb. 2017 1 / 34 Definitions and Examples
More informationFRST Multivariate Statistics. Multivariate Discriminant Analysis (MDA)
1 FRST 531 -- Mutivariate Statistics Mutivariate Discriminant Anaysis (MDA) Purpose: 1. To predict which group (Y) an observation beongs to based on the characteristics of p predictor (X) variabes, using
More informationu(x) s.t. px w x 0 Denote the solution to this problem by ˆx(p, x). In order to obtain ˆx we may simply solve the standard problem max x 0
Bocconi University PhD in Economics - Microeconomics I Prof M Messner Probem Set 4 - Soution Probem : If an individua has an endowment instead of a monetary income his weath depends on price eves In particuar,
More informationSUPPLEMENTARY MATERIAL TO INNOVATED SCALABLE EFFICIENT ESTIMATION IN ULTRA-LARGE GAUSSIAN GRAPHICAL MODELS
ISEE 1 SUPPLEMENTARY MATERIAL TO INNOVATED SCALABLE EFFICIENT ESTIMATION IN ULTRA-LARGE GAUSSIAN GRAPHICAL MODELS By Yingying Fan and Jinchi Lv University of Southern Caifornia This Suppementary Materia
More informationFrom now on, we will represent a metric space with (X, d). Here are some examples: i=1 (x i y i ) p ) 1 p, p 1.
Chapter 1 Metric spaces 1.1 Metric and convergence We will begin with some basic concepts. Definition 1.1. (Metric space) Metric space is a set X, with a metric satisfying: 1. d(x, y) 0, d(x, y) = 0 x
More informationSobolev embeddings and interpolations
embed2.tex, January, 2007 Sobolev embeddings and interpolations Pavel Krejčí This is a second iteration of a text, which is intended to be an introduction into Sobolev embeddings and interpolations. The
More informationEmbeddings of finite metric spaces in Euclidean space: a probabilistic view
Embeddings of finite metric spaces in Euclidean space: a probabilistic view Yuval Peres May 11, 2006 Talk based on work joint with: Assaf Naor, Oded Schramm and Scott Sheffield Definition: An invertible
More information1D Heat Propagation Problems
Chapter 1 1D Heat Propagation Probems If the ambient space of the heat conduction has ony one dimension, the Fourier equation reduces to the foowing for an homogeneous body cρ T t = T λ 2 + Q, 1.1) x2
More informationCS229T/STATS231: Statistical Learning Theory. Lecturer: Tengyu Ma Lecture 11 Scribe: Jongho Kim, Jamie Kang October 29th, 2018
CS229T/STATS231: Statistical Learning Theory Lecturer: Tengyu Ma Lecture 11 Scribe: Jongho Kim, Jamie Kang October 29th, 2018 1 Overview This lecture mainly covers Recall the statistical theory of GANs
More information6.434J/16.391J Statistics for Engineers and Scientists May 4 MIT, Spring 2006 Handout #17. Solution 7
6.434J/16.391J Statistics for Engineers and Scientists May 4 MIT, Spring 2006 Handout #17 Soution 7 Probem 1: Generating Random Variabes Each part of this probem requires impementation in MATLAB. For the
More informationSeparation of Variables and a Spherical Shell with Surface Charge
Separation of Variabes and a Spherica She with Surface Charge In cass we worked out the eectrostatic potentia due to a spherica she of radius R with a surface charge density σθ = σ cos θ. This cacuation
More informationBounded uniformly continuous functions
Bounded uniformly continuous functions Objectives. To study the basic properties of the C -algebra of the bounded uniformly continuous functions on some metric space. Requirements. Basic concepts of analysis:
More informationAlgorithms, Geometry and Learning. Reading group Paris Syminelakis
Algorithms, Geometry and Learning Reading group Paris Syminelakis October 11, 2016 2 Contents 1 Local Dimensionality Reduction 5 1 Introduction.................................... 5 2 Definitions and Results..............................
More informationXSAT of linear CNF formulas
XSAT of inear CN formuas Bernd R. Schuh Dr. Bernd Schuh, D-50968 Kön, Germany; bernd.schuh@netcoogne.de eywords: compexity, XSAT, exact inear formua, -reguarity, -uniformity, NPcompeteness Abstract. Open
More informationA Glimpse into Topology
A Glimpse into Topology by Vishal Malik A project submitted to the Department of Mathematical Sciences in conformity with the requirements for Math 430 (203-4) Lakehead University Thunder Bay, Ontario,
More informationLecture 11. Fourier transform
Lecture. Fourier transform Definition and main resuts Let f L 2 (R). The Fourier transform of a function f is a function f(α) = f(x)t iαx dx () The normaized Fourier transform of f is a function R ˆf =
More informationA Unique Common Coupled Fixed Point Theorem for Four Maps in Partial b-metric- Like Spaces
SQU Journa for Science 05 9() 55-6 04 Sutan Qaboos University A Unique Common Couped Fixed Point Theorem for Four Maps in Partia b-metric- Like Spaces Mohammad S. Khan * Konduru P.R. Rao and Kandipai V.S.
More informationNumerical methods for elliptic partial differential equations Arnold Reusken
Numerica methods for eiptic partia differentia equations Arnod Reusken Preface This is a book on the numerica approximation of partia differentia equations. On the next page we give an overview of the
More informationare left and right inverses of b, respectively, then: (b b 1 and b 1 = b 1 b 1 id T = b 1 b) b 1 so they are the same! r ) = (b 1 r = id S b 1 r = b 1
Lecture 1. The Category of Sets PCMI Summer 2015 Undergraduate Lectures on Fag Varieties Lecture 1. Some basic set theory, a moment of categorica zen, and some facts about the permutation groups on n etters.
More informationCONGRUENCES. 1. History
CONGRUENCES HAO BILLY LEE Abstract. These are notes I created for a seminar tak, foowing the papers of On the -adic Representations and Congruences for Coefficients of Moduar Forms by Swinnerton-Dyer and
More information4 Expectation & the Lebesgue Theorems
STA 205: Probability & Measure Theory Robert L. Wolpert 4 Expectation & the Lebesgue Theorems Let X and {X n : n N} be random variables on a probability space (Ω,F,P). If X n (ω) X(ω) for each ω Ω, does
More informationMath 220B - Summer 2003 Homework 1 Solutions
Math 0B - Summer 003 Homework Soutions Consider the eigenvaue probem { X = λx 0 < x < X satisfies symmetric BCs x = 0, Suppose f(x)f (x) x=b x=a 0 for a rea-vaued functions f(x) which satisfy the boundary
More informationStatistical Inference, Econometric Analysis and Matrix Algebra
Statistica Inference, Econometric Anaysis and Matrix Agebra Bernhard Schipp Water Krämer Editors Statistica Inference, Econometric Anaysis and Matrix Agebra Festschrift in Honour of Götz Trenker Physica-Verag
More informationTHE REACHABILITY CONES OF ESSENTIALLY NONNEGATIVE MATRICES
THE REACHABILITY CONES OF ESSENTIALLY NONNEGATIVE MATRICES by Michae Neumann Department of Mathematics, University of Connecticut, Storrs, CT 06269 3009 and Ronad J. Stern Department of Mathematics, Concordia
More informationIntegrality ratio for Group Steiner Trees and Directed Steiner Trees
Integraity ratio for Group Steiner Trees and Directed Steiner Trees Eran Haperin Guy Kortsarz Robert Krauthgamer Aravind Srinivasan Nan Wang Abstract The natura reaxation for the Group Steiner Tree probem,
More informationStrauss PDEs 2e: Section Exercise 1 Page 1 of 7
Strauss PDEs 2e: Section 4.3 - Exercise 1 Page 1 of 7 Exercise 1 Find the eigenvaues graphicay for the boundary conditions X(0) = 0, X () + ax() = 0. Assume that a 0. Soution The aim here is to determine
More informationLecture 5 - Hausdorff and Gromov-Hausdorff Distance
Lecture 5 - Hausdorff and Gromov-Hausdorff Distance August 1, 2011 1 Definition and Basic Properties Given a metric space X, the set of closed sets of X supports a metric, the Hausdorff metric. If A is
More informationAssignment 7 Due Tuessday, March 29, 2016
Math 45 / AMCS 55 Dr. DeTurck Assignment 7 Due Tuessday, March 9, 6 Topics for this week Convergence of Fourier series; Lapace s equation and harmonic functions: basic properties, compuations on rectanges
More informationAALBORG UNIVERSITY. The distribution of communication cost for a mobile service scenario. Jesper Møller and Man Lung Yiu. R June 2009
AALBORG UNIVERSITY The distribution of communication cost for a mobie service scenario by Jesper Møer and Man Lung Yiu R-29-11 June 29 Department of Mathematica Sciences Aaborg University Fredrik Bajers
More informationB. Appendix B. Topological vector spaces
B.1 B. Appendix B. Topological vector spaces B.1. Fréchet spaces. In this appendix we go through the definition of Fréchet spaces and their inductive limits, such as they are used for definitions of function
More informationA Brief Introduction to Markov Chains and Hidden Markov Models
A Brief Introduction to Markov Chains and Hidden Markov Modes Aen B MacKenzie Notes for December 1, 3, &8, 2015 Discrete-Time Markov Chains You may reca that when we first introduced random processes,
More informationMATH 6337: Homework 8 Solutions
6.1. MATH 6337: Homework 8 Solutions (a) Let be a measurable subset of 2 such that for almost every x, {y : (x, y) } has -measure zero. Show that has measure zero and that for almost every y, {x : (x,
More informationMARKOV CHAINS AND MARKOV DECISION THEORY. Contents
MARKOV CHAINS AND MARKOV DECISION THEORY ARINDRIMA DATTA Abstract. In this paper, we begin with a forma introduction to probabiity and expain the concept of random variabes and stochastic processes. After
More informationReal Analysis Problems
Real Analysis Problems Cristian E. Gutiérrez September 14, 29 1 1 CONTINUITY 1 Continuity Problem 1.1 Let r n be the sequence of rational numbers and Prove that f(x) = 1. f is continuous on the irrationals.
More informationFunctional Analysis Winter 2018/2019
Functional Analysis Winter 2018/2019 Peer Christian Kunstmann Karlsruher Institut für Technologie (KIT) Institut für Analysis Englerstr. 2, 76131 Karlsruhe e-mail: peer.kunstmann@kit.edu These lecture
More information221B Lecture Notes Notes on Spherical Bessel Functions
Definitions B Lecture Notes Notes on Spherica Besse Functions We woud ike to sove the free Schrödinger equation [ h d r R(r) = h k R(r). () m r dr r m R(r) is the radia wave function ψ( x) = R(r)Y m (θ,
More informationMAT 570 REAL ANALYSIS LECTURE NOTES. Contents. 1. Sets Functions Countability Axiom of choice Equivalence relations 9
MAT 570 REAL ANALYSIS LECTURE NOTES PROFESSOR: JOHN QUIGG SEMESTER: FALL 204 Contents. Sets 2 2. Functions 5 3. Countability 7 4. Axiom of choice 8 5. Equivalence relations 9 6. Real numbers 9 7. Extended
More information3 (Due ). Let A X consist of points (x, y) such that either x or y is a rational number. Is A measurable? What is its Lebesgue measure?
MA 645-4A (Real Analysis), Dr. Chernov Homework assignment 1 (Due ). Show that the open disk x 2 + y 2 < 1 is a countable union of planar elementary sets. Show that the closed disk x 2 + y 2 1 is a countable
More informationA Primer on Lipschitz Functions by Robert Dr. Bob Gardner Revised and Corrected, Fall 2013
A Primer on Lipschitz Functions by Robert Dr. Bob Gardner Revised and Corrected, Fall 2013 Note. The purpose of these notes is to contrast the behavior of functions of a real variable and functions of
More informationContinuity of convex functions in normed spaces
Continuity of convex functions in normed spaces In this chapter, we consider continuity properties of real-valued convex functions defined on open convex sets in normed spaces. Recall that every infinitedimensional
More informationOn metric characterizations of some classes of Banach spaces
On metric characterizations of some classes of Banach spaces Mikhail I. Ostrovskii January 12, 2011 Abstract. The first part of the paper is devoted to metric characterizations of Banach spaces with no
More information4 Separation of Variables
4 Separation of Variabes In this chapter we describe a cassica technique for constructing forma soutions to inear boundary vaue probems. The soution of three cassica (paraboic, hyperboic and eiptic) PDE
More informationLecture 4 Lebesgue spaces and inequalities
Lecture 4: Lebesgue spaces and inequalities 1 of 10 Course: Theory of Probability I Term: Fall 2013 Instructor: Gordan Zitkovic Lecture 4 Lebesgue spaces and inequalities Lebesgue spaces We have seen how
More informationEfficiently Generating Random Bits from Finite State Markov Chains
1 Efficienty Generating Random Bits from Finite State Markov Chains Hongchao Zhou and Jehoshua Bruck, Feow, IEEE Abstract The probem of random number generation from an uncorreated random source (of unknown
More informationCHAPTER 1. Metric Spaces. 1. Definition and examples
CHAPTER Metric Spaces. Definition and examples Metric spaces generalize and clarify the notion of distance in the real line. The definitions will provide us with a useful tool for more general applications
More informationMinimum Enclosing Circle of a Set of Fixed Points and a Mobile Point
Minimum Encosing Circe of a Set of Fixed Points and a Mobie Point Aritra Banik 1, Bhaswar B. Bhattacharya 2, and Sandip Das 1 1 Advanced Computing and Microeectronics Unit, Indian Statistica Institute,
More informationMath 5210, Definitions and Theorems on Metric Spaces
Math 5210, Definitions and Theorems on Metric Spaces Let (X, d) be a metric space. We will use the following definitions (see Rudin, chap 2, particularly 2.18) 1. Let p X and r R, r > 0, The ball of radius
More informationERRATA: Probabilistic Techniques in Analysis
ERRATA: Probabilistic Techniques in Analysis ERRATA 1 Updated April 25, 26 Page 3, line 13. A 1,..., A n are independent if P(A i1 A ij ) = P(A 1 ) P(A ij ) for every subset {i 1,..., i j } of {1,...,
More informationA Union of Euclidean Spaces is Euclidean. Konstantin Makarychev, Northwestern Yury Makarychev, TTIC
Union of Euclidean Spaces is Euclidean Konstantin Makarychev, Northwestern Yury Makarychev, TTIC MS Meeting, New York, May 7, 2017 Problem by ssaf Naor Suppose that metric space (X, d) is a union of two
More informationREAL VARIABLES: PROBLEM SET 1. = x limsup E k
REAL VARIABLES: PROBLEM SET 1 BEN ELDER 1. Problem 1.1a First let s prove that limsup E k consists of those points which belong to infinitely many E k. From equation 1.1: limsup E k = E k For limsup E
More informationOn the Goal Value of a Boolean Function
On the Goa Vaue of a Booean Function Eric Bach Dept. of CS University of Wisconsin 1210 W. Dayton St. Madison, WI 53706 Lisa Heerstein Dept of CSE NYU Schoo of Engineering 2 Metrotech Center, 10th Foor
More informationLecture Notes for Math 251: ODE and PDE. Lecture 32: 10.2 Fourier Series
Lecture Notes for Math 251: ODE and PDE. Lecture 32: 1.2 Fourier Series Shawn D. Ryan Spring 212 Last Time: We studied the heat equation and the method of Separation of Variabes. We then used Separation
More information