Information Inequalities for Joint Distributions, with Interpretations and Applications Mokshay Madiman, Member, IEEE, and Prasad Tetali, Member, IEEE
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Lecture 3: Entropy, Relative Entropy, and Mutual Information 1 Notation 2
EE376A/STATS376A Information Theory Lecture 3 - 01/16/2018 Lecture 3: Entropy, Relative Entropy, and Mutual Information Lecturer: Tsachy Weissman Scribe: Yicheng An, Melody Guan, Jacob Rebec, John Sholar In this lecture, we will introduce certain key measures of information, that play crucial roles in theoretical and operational characterizations throughout the course. These include the entropy, the mutual information, and the relative entropy. We will also exhibit some key properties exhibited by these information measures. 1 Notation A quick summary of the notation 1. Discrete Random Variable: U 2. Alphabet: U = fu1; u2; :::; uM g (An alphabet of size M) 3. Specific Value: u; u1; etc. For discrete random variables, we will write (interchangeably) P (U = u), PU (u) or most often just, p(u) Similarly, for a pair of random variables X; Y we write P (X = x j Y = y), PXjY (x j y) or p(x j y) 2 Entropy Definition 1. \Surprise" Function: 1 S(u) log (1) , p(u) A lower probability of u translates to a greater \surprise" that it occurs. Note here that we use log to mean log2 by default, rather than the natural log ln, as is typical in some other contexts. This is true throughout these notes: log is assumed to be log2 unless otherwise indicated. Definition 2. Entropy: Let U a discrete random variable taking values in alphabet U. The entropy of U is given by: 1 X H(U) [S(U)] = log = − log (p(U)) = − p(u) log p(u) (2) , E E p(U) E u Where U represents all u values possible to the variable. -
An Introduction to Information Theory
An Introduction to Information Theory Vahid Meghdadi reference : Elements of Information Theory by Cover and Thomas September 2007 Contents 1 Entropy 2 2 Joint and conditional entropy 4 3 Mutual information 5 4 Data Compression or Source Coding 6 5 Channel capacity 8 5.1 examples . 9 5.1.1 Noiseless binary channel . 9 5.1.2 Binary symmetric channel . 9 5.1.3 Binary erasure channel . 10 5.1.4 Two fold channel . 11 6 Differential entropy 12 6.1 Relation between differential and discrete entropy . 13 6.2 joint and conditional entropy . 13 6.3 Some properties . 14 7 The Gaussian channel 15 7.1 Capacity of Gaussian channel . 15 7.2 Band limited channel . 16 7.3 Parallel Gaussian channel . 18 8 Capacity of SIMO channel 19 9 Exercise (to be completed) 22 1 1 Entropy Entropy is a measure of uncertainty of a random variable. The uncertainty or the amount of information containing in a message (or in a particular realization of a random variable) is defined as the inverse of the logarithm of its probabil- ity: log(1=PX (x)). So, less likely outcome carries more information. Let X be a discrete random variable with alphabet X and probability mass function PX (x) = PrfX = xg, x 2 X . For convenience PX (x) will be denoted by p(x). The entropy of X is defined as follows: Definition 1. The entropy H(X) of a discrete random variable is defined by 1 H(X) = E log p(x) X 1 = p(x) log (1) p(x) x2X Entropy indicates the average information contained in X. -
Chapter 2: Entropy and Mutual Information
Chapter 2: Entropy and Mutual Information University of Illinois at Chicago ECE 534, Natasha Devroye Chapter 2 outline • Definitions • Entropy • Joint entropy, conditional entropy • Relative entropy, mutual information • Chain rules • Jensen’s inequality • Log-sum inequality • Data processing inequality • Fano’s inequality University of Illinois at Chicago ECE 534, Natasha Devroye Definitions A discrete random variable X takes on values x from the discrete alphabet . X The probability mass function (pmf) is described by p (x)=p(x) = Pr X = x , for x . X { } ∈ X University of Illinois at Chicago ECE 534, Natasha Devroye Copyright Cambridge University Press 2003. On-screen viewing permitted. Printing not permitted. http://www.cambridge.org/0521642981 You can buy this book for 30 pounds or $50. See http://www.inference.phy.cam.ac.uk/mackay/itila/ for links. 2 Probability, Entropy, and Inference Definitions Copyright Cambridge University Press 2003. On-screen viewing permitted. Printing not permitted. http://www.cambridge.org/0521642981 This chapter, and its sibling, Chapter 8, devote some time to notation. Just You can buy this book for 30 pounds or $50. See http://www.inference.phy.cam.ac.uk/mackay/itila/as the White Knight fordistinguished links. between the song, the name of the song, and what the name of the song was called (Carroll, 1998), we will sometimes 2.1: Probabilities and ensembles need to be careful to distinguish between a random variable, the v23alue of the i ai pi random variable, and the proposition that asserts that the random variable x has a particular value. In any particular chapter, however, I will use the most 1 a 0.0575 a Figure 2.2. -
Noisy Channel Coding
Noisy Channel Coding: Correlated Random Variables & Communication over a Noisy Channel Toni Hirvonen Helsinki University of Technology Laboratory of Acoustics and Audio Signal Processing [email protected] T-61.182 Special Course in Information Science II / Spring 2004 1 Contents • More entropy definitions { joint & conditional entropy { mutual information • Communication over a noisy channel { overview { information conveyed by a channel { noisy channel coding theorem 2 Joint Entropy Joint entropy of X; Y is: 1 H(X; Y ) = P (x; y) log P (x; y) xy X Y 2AXA Entropy is additive for independent random variables: H(X; Y ) = H(X) + H(Y ) iff P (x; y) = P (x)P (y) 3 Conditional Entropy Conditional entropy of X given Y is: 1 1 H(XjY ) = P (y) P (xjy) log = P (x; y) log P (xjy) P (xjy) y2A "x2A # y2A A XY XX XX Y It measures the average uncertainty (i.e. information content) that remains about x when y is known. 4 Mutual Information Mutual information between X and Y is: I(Y ; X) = I(X; Y ) = H(X) − H(XjY ) ≥ 0 It measures the average reduction in uncertainty about x that results from learning the value of y, or vice versa. Conditional mutual information between X and Y given Z is: I(Y ; XjZ) = H(XjZ) − H(XjY; Z) 5 Breakdown of Entropy Entropy relations: Chain rule of entropy: H(X; Y ) = H(X) + H(Y jX) = H(Y ) + H(XjY ) 6 Noisy Channel: Overview • Real-life communication channels are hopelessly noisy i.e. introduce transmission errors • However, a solution can be achieved { the aim of source coding is to remove redundancy from the source data -
Networked Distributed Source Coding
Networked distributed source coding Shizheng Li and Aditya Ramamoorthy Abstract The data sensed by differentsensors in a sensor network is typically corre- lated. A natural question is whether the data correlation can be exploited in innova- tive ways along with network information transfer techniques to design efficient and distributed schemes for the operation of such networks. This necessarily involves a coupling between the issues of compression and networked data transmission, that have usually been considered separately. In this work we review the basics of classi- cal distributed source coding and discuss some practical code design techniques for it. We argue that the network introduces several new dimensions to the problem of distributed source coding. The compression rates and the network information flow constrain each other in intricate ways. In particular, we show that network coding is often required for optimally combining distributed source coding and network information transfer and discuss the associated issues in detail. We also examine the problem of resource allocation in the context of distributed source coding over networks. 1 Introduction There are various instances of problems where correlated sources need to be trans- mitted over networks, e.g., a large scale sensor network deployed for temperature or humidity monitoring over a large field or for habitat monitoring in a jungle. This is an example of a network information transfer problem with correlated sources. A natural question is whether the data correlation can be exploited in innovative ways along with network information transfer techniques to design efficient and distributed schemes for the operation of such networks. This necessarily involves a Shizheng Li · Aditya Ramamoorthy Iowa State University, Ames, IA, U.S.A. -
On Measures of Entropy and Information
On Measures of Entropy and Information Tech. Note 009 v0.7 http://threeplusone.com/info Gavin E. Crooks 2018-09-22 Contents 5 Csiszar´ f-divergences 12 Csiszar´ f-divergence ................ 12 0 Notes on notation and nomenclature 2 Dual f-divergence .................. 12 Symmetric f-divergences .............. 12 1 Entropy 3 K-divergence ..................... 12 Entropy ........................ 3 Fidelity ........................ 12 Joint entropy ..................... 3 Marginal entropy .................. 3 Hellinger discrimination .............. 12 Conditional entropy ................. 3 Pearson divergence ................. 14 Neyman divergence ................. 14 2 Mutual information 3 LeCam discrimination ............... 14 Mutual information ................. 3 Skewed K-divergence ................ 14 Multivariate mutual information ......... 4 Alpha-Jensen-Shannon-entropy .......... 14 Interaction information ............... 5 Conditional mutual information ......... 5 6 Chernoff divergence 14 Binding information ................ 6 Chernoff divergence ................. 14 Residual entropy .................. 6 Chernoff coefficient ................. 14 Total correlation ................... 6 Renyi´ divergence .................. 15 Lautum information ................ 6 Alpha-divergence .................. 15 Uncertainty coefficient ............... 7 Cressie-Read divergence .............. 15 Tsallis divergence .................. 15 3 Relative entropy 7 Sharma-Mittal divergence ............. 15 Relative entropy ................... 7 Cross entropy -
Information Theory and Maximum Entropy 8.1 Fundamentals of Information Theory
NEU 560: Statistical Modeling and Analysis of Neural Data Spring 2018 Lecture 8: Information Theory and Maximum Entropy Lecturer: Mike Morais Scribes: 8.1 Fundamentals of Information theory Information theory started with Claude Shannon's A mathematical theory of communication. The first building block was entropy, which he sought as a functional H(·) of probability densities with two desired properties: 1. Decreasing in P (X), such that if P (X1) < P (X2), then h(P (X1)) > h(P (X2)). 2. Independent variables add, such that if X and Y are independent, then H(P (X; Y )) = H(P (X)) + H(P (Y )). These are only satisfied for − log(·). Think of it as a \surprise" function. Definition 8.1 (Entropy) The entropy of a random variable is the amount of information needed to fully describe it; alternate interpretations: average number of yes/no questions needed to identify X, how uncertain you are about X? X H(X) = − P (X) log P (X) = −EX [log P (X)] (8.1) X Average information, surprise, or uncertainty are all somewhat parsimonious plain English analogies for entropy. There are a few ways to measure entropy for multiple variables; we'll use two, X and Y . Definition 8.2 (Conditional entropy) The conditional entropy of a random variable is the entropy of one random variable conditioned on knowledge of another random variable, on average. Alternative interpretations: the average number of yes/no questions needed to identify X given knowledge of Y , on average; or How uncertain you are about X if you know Y , on average? X X h X i H(X j Y ) = P (Y )[H(P (X j Y ))] = P (Y ) − P (X j Y ) log P (X j Y ) Y Y X X = = − P (X; Y ) log P (X j Y ) X;Y = −EX;Y [log P (X j Y )] (8.2) Definition 8.3 (Joint entropy) X H(X; Y ) = − P (X; Y ) log P (X; Y ) = −EX;Y [log P (X; Y )] (8.3) X;Y 8-1 8-2 Lecture 8: Information Theory and Maximum Entropy • Bayes' rule for entropy H(X1 j X2) = H(X2 j X1) + H(X1) − H(X2) (8.4) • Chain rule of entropies n X H(Xn;Xn−1; :::X1) = H(Xn j Xn−1; :::X1) (8.5) i=1 It can be useful to think about these interrelated concepts with a so-called information diagram. -
On the Entropy of Sums
On the Entropy of Sums Mokshay Madiman Department of Statistics Yale University Email: [email protected] Abstract— It is shown that the entropy of a sum of independent II. PRELIMINARIES random vectors is a submodular set function, and upper bounds on the entropy of sums are obtained as a result in both discrete Let X1,X2,...,Xn be a collection of random variables and continuous settings. These inequalities complement the lower taking values in some linear space, so that addition is a bounds provided by the entropy power inequalities of Madiman well-defined operation. We assume that the joint distribu- and Barron (2007). As applications, new inequalities for the tion has a density f with respect to some reference mea- determinants of sums of positive-definite matrices are presented. sure. This allows the definition of the entropy of various random variables depending on X1,...,Xn. For instance, I. INTRODUCTION H(X1,X2,...,Xn) = −E[log f(X1,X2,...,Xn)]. There are the familiar two canonical cases: (a) the random variables Entropies of sums are not as well understood as joint are real-valued and possess a probability density function, or entropies. Indeed, for the joint entropy, there is an elaborate (b) they are discrete. In the former case, H represents the history of entropy inequalities starting with the chain rule of differential entropy, and in the latter case, H represents the Shannon, whose major developments include works of Han, discrete entropy. We simply call H the entropy in all cases, ˇ Shearer, Fujishige, Yeung, Matu´s, and others. The earlier part and where the distinction matters, the relevant assumption will of this work, involving so-called Shannon-type inequalities be made explicit. -
Entropy, Relative Entropy, Cross Entropy Entropy
Entropy, Relative Entropy, Cross Entropy Entropy Entropy, H(x) is a measure of the uncertainty of a discrete random variable. Properties: ● H(x) >= 0 ● Entropy Entropy ● Lesser the probability for an event, larger the entropy. Entropy of a six-headed fair dice is log26. Entropy : Properties Primer on Probability Fundamentals ● Random Variable ● Probability ● Expectation ● Linearity of Expectation Entropy : Properties Primer on Probability Fundamentals ● Jensen’s Inequality Ex:- Subject to the constraint that, f is a convex function. Entropy : Properties ● H(U) >= 0, Where, U = {u , u , …, u } 1 2 M ● H(U) <= log(M) Entropy between pair of R.Vs ● Joint Entropy ● Conditional Entropy Relative Entropy aka Kullback Leibler Distance D(p||q) is a measure of the inefficiency of assuming that the distribution is q, when the true distribution is p. ● H(p) : avg description length when true distribution. ● H(p) + D(p||q) : avg description length when approximated distribution. If X is a random variable and p(x), q(x) are probability mass functions, Relative Entropy/ K-L Divergence : Properties D(p||q) is a measure of the inefficiency of assuming that the distribution is q, when the true distribution is p. Properties: ● Non-negative. ● D(p||q) = 0 if p=q. ● Non-symmetric and does not satisfy triangular inequality - it is rather divergence than distance. Relative Entropy/ K-L Divergence : Properties Asymmetricity: Let, X = {0, 1} be a random variable. Consider two distributions p, q on X. Assume, p(0) = 1-r, p(1) = r ; q(0) = 1-s, q(1) = s; If, r=s, then D(p||q) = D(q||p) = 0, else for r!=s, D(p||q) != D(q||p) Relative Entropy/ K-L Divergence : Properties Non-negativity: Relative Entropy/ K-L Divergence : Properties Relative Entropy of joint distributions as Mutual Information Mutual Information, which is a measure of the amount of information that one random variable contains about another random variable. -
Information Theory & Coding
INFORMATION THEORY & CODING Week 2 : Entropy Dr. Rui Wang Department of Electrical and Electronic Engineering Southern Univ. of Science and Technology (SUSTech) Email: [email protected] September 14, 2021 Dr. Rui Wang (EEE) INFORMATION THEORY & CODING September 14, 2021 1 / 25 Outline Most of the basic definitions will be introduced. Entropy, Joint Entropy, Conditional Entropy, Relative Entropy, Mutual Information, etc. Relationships among basic definitions. Chain Rules. Dr. Rui Wang (EEE) INFORMATION THEORY & CODING September 14, 2021 2 / 25 What is Information? To have a quantitative measure of information contained in an event, we consider intuitively the following: Information contained in events should be defined in terms of the uncertainty/probability of the events. Monotonous: Less certain (small probability) events should contain more information. Additive: The total information of unrelated/independent events should equal the sum of the information of each individual event. Dr. Rui Wang (EEE) INFORMATION THEORY & CODING September 14, 2021 3 / 25 Information Measure of Random Events A natural measure of the uncertainty of an event A is the probability Pr(A) of A. To satisfy the monotonous and additive properties, the information in the event A could be defined as I (A)self-info = − log Pr(A): If Pr(A) > Pr(B), then I (A) < I (B). If A, B are independent, then I (A + B) = I (A) + I (B). Dr. Rui Wang (EEE) INFORMATION THEORY & CODING September 14, 2021 4 / 25 Information Unit log2 : bit loge : nat log10 : Hartley logb X loga X = = loga b · logb X logb a Dr. Rui Wang (EEE) INFORMATION THEORY & CODING September 14, 2021 5 / 25 Average Information Measure of a Discrete R.V. -
Lecture 2 Entropy and Mutual Information Instructor: Yichen Wang Ph.D./Associate Professor
Elements of Information Theory Lecture 2 Entropy and Mutual Information Instructor: Yichen Wang Ph.D./Associate Professor School of Information and Communications Engineering Division of Electronics and Information Xi’an Jiaotong University Outlines Entropy, Joint Entropy, and Conditional Entropy Mutual Information Convexity Analysis for Entropy and Mutual Information Entropy and Mutual Information in Communications Systems Xi’an Jiaotong University 3 Entropy Entropy —— 熵 Entropy in Thermodynamics(热力学) It was first developed in the early 1850s by Rudolf Clausius (French Physicist). System is composed of a very large number of constituents (atoms, molecule…). It is a measure of the number of the microscopic configurations that corresponds to a thermodynamic system in a state specified by certain macroscopic variables. It can be understood as a measure of molecular disorder within a macroscopic system. Xi’an Jiaotong University 4 Entropy Entropy in Statistical Mechanics(统计力学) The statistical definition was developed by Ludwig Boltzmann in the 1870s by analyzing the statistical behavior of the microscopic components of the system. Boltzmann showed that this definition of entropy was equivalent to the thermodynamic entropy to within a constant number which has since been known as Boltzmann's constant. Entropy is associated with the number of the microstates of a system. How to define ENTROPY in information theory? Xi’an Jiaotong University 5 Entropy Definition The entropy H(X) of a discrete random variable X is defined by p(x) is the probability mass function(概率质量函数)which can be written as The base of the logarithm is 2 and the unit is bits. If the base of the logarithm is e, then the unit is nats. -
Noisy-Channel Coding Copyright Cambridge University Press 2003
Copyright Cambridge University Press 2003. On-screen viewing permitted. Printing not permitted. http://www.cambridge.org/0521642981 You can buy this book for 30 pounds or $50. See http://www.inference.phy.cam.ac.uk/mackay/itila/ for links. Part II Noisy-Channel Coding Copyright Cambridge University Press 2003. On-screen viewing permitted. Printing not permitted. http://www.cambridge.org/0521642981 You can buy this book for 30 pounds or $50. See http://www.inference.phy.cam.ac.uk/mackay/itila/ for links. 8 Dependent Random Variables In the last three chapters on data compression we concentrated on random vectors x coming from an extremely simple probability distribution, namely the separable distribution in which each component xn is independent of the others. In this chapter, we consider joint ensembles in which the random variables are dependent. This material has two motivations. First, data from the real world have interesting correlations, so to do data compression well, we need to know how to work with models that include dependences. Second, a noisy channel with input x and output y defines a joint ensemble in which x and y are dependent { if they were independent, it would be impossible to communicate over the channel { so communication over noisy channels (the topic of chapters 9{11) is described in terms of the entropy of joint ensembles. 8.1 More about entropy This section gives definitions and exercises to do with entropy, carrying on from section 2.4. The joint entropy of X; Y is: 1 H(X; Y ) = P (x; y) log : (8.1) P (x; y) xy2AXX AY Entropy is additive for independent random variables: H(X; Y ) = H(X) + H(Y ) iff P (x; y) = P (x)P (y): (8.2) The conditional entropy of X given y = bk is the entropy of the proba- bility distribution P (x y = b ).