A Primer on Information Theory, with Applications to Neuroscience
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Entropy Rate of Stochastic Processes
Entropy Rate of Stochastic Processes Timo Mulder Jorn Peters [email protected] [email protected] February 8, 2015 The entropy rate of independent and identically distributed events can on average be encoded by H(X) bits per source symbol. However, in reality, series of events (or processes) are often randomly distributed and there can be arbitrary dependence between each event. Such processes with arbitrary dependence between variables are called stochastic processes. This report shows how to calculate the entropy rate for such processes, accompanied with some denitions, proofs and brief examples. 1 Introduction One may be interested in the uncertainty of an event or a series of events. Shannon entropy is a method to compute the uncertainty in an event. This can be used for single events or for several independent and identically distributed events. However, often events or series of events are not independent and identically distributed. In that case the events together form a stochastic process i.e. a process in which multiple outcomes are possible. These processes are omnipresent in all sorts of elds of study. As it turns out, Shannon entropy cannot directly be used to compute the uncertainty in a stochastic process. However, it is easy to extend such that it can be used. Also when a stochastic process satises certain properties, for example if the stochastic process is a Markov process, it is straightforward to compute the entropy of the process. The entropy rate of a stochastic process can be used in various ways. An example of this is given in Section 4.1. -
Entropy Rate Estimation for Markov Chains with Large State Space
Entropy Rate Estimation for Markov Chains with Large State Space Yanjun Han Department of Electrical Engineering Stanford University Stanford, CA 94305 [email protected] Jiantao Jiao Department of Electrical Engineering and Computer Sciences University of California, Berkeley Berkeley, CA 94720 [email protected] Chuan-Zheng Lee, Tsachy Weissman Yihong Wu Department of Electrical Engineering Department of Statistics and Data Science Stanford University Yale University Stanford, CA 94305 New Haven, CT 06511 {czlee, tsachy}@stanford.edu [email protected] Tiancheng Yu Department of Electronic Engineering Tsinghua University Haidian, Beijing 100084 [email protected] Abstract Entropy estimation is one of the prototypicalproblems in distribution property test- ing. To consistently estimate the Shannon entropy of a distribution on S elements with independent samples, the optimal sample complexity scales sublinearly with arXiv:1802.07889v3 [cs.LG] 24 Sep 2018 S S as Θ( log S ) as shown by Valiant and Valiant [41]. Extendingthe theory and algo- rithms for entropy estimation to dependent data, this paper considers the problem of estimating the entropy rate of a stationary reversible Markov chain with S states from a sample path of n observations. We show that Provided the Markov chain mixes not too slowly, i.e., the relaxation time is • S S2 at most O( 3 ), consistent estimation is achievable when n . ln S ≫ log S Provided the Markov chain has some slight dependency, i.e., the relaxation • 2 time is at least 1+Ω( ln S ), consistent estimation is impossible when n . √S S2 log S . Under both assumptions, the optimal estimation accuracy is shown to be S2 2 Θ( n log S ). -
Entropy Power, Autoregressive Models, and Mutual Information
entropy Article Entropy Power, Autoregressive Models, and Mutual Information Jerry Gibson Department of Electrical and Computer Engineering, University of California, Santa Barbara, Santa Barbara, CA 93106, USA; [email protected] Received: 7 August 2018; Accepted: 17 September 2018; Published: 30 September 2018 Abstract: Autoregressive processes play a major role in speech processing (linear prediction), seismic signal processing, biological signal processing, and many other applications. We consider the quantity defined by Shannon in 1948, the entropy rate power, and show that the log ratio of entropy powers equals the difference in the differential entropy of the two processes. Furthermore, we use the log ratio of entropy powers to analyze the change in mutual information as the model order is increased for autoregressive processes. We examine when we can substitute the minimum mean squared prediction error for the entropy power in the log ratio of entropy powers, thus greatly simplifying the calculations to obtain the differential entropy and the change in mutual information and therefore increasing the utility of the approach. Applications to speech processing and coding are given and potential applications to seismic signal processing, EEG classification, and ECG classification are described. Keywords: autoregressive models; entropy rate power; mutual information 1. Introduction In time series analysis, the autoregressive (AR) model, also called the linear prediction model, has received considerable attention, with a host of results on fitting AR models, AR model prediction performance, and decision-making using time series analysis based on AR models [1–3]. The linear prediction or AR model also plays a major role in many digital signal processing applications, such as linear prediction modeling of speech signals [4–6], geophysical exploration [7,8], electrocardiogram (ECG) classification [9], and electroencephalogram (EEG) classification [10,11]. -
Source Coding: Part I of Fundamentals of Source and Video Coding
Foundations and Trends R in sample Vol. 1, No 1 (2011) 1–217 c 2011 Thomas Wiegand and Heiko Schwarz DOI: xxxxxx Source Coding: Part I of Fundamentals of Source and Video Coding Thomas Wiegand1 and Heiko Schwarz2 1 Berlin Institute of Technology and Fraunhofer Institute for Telecommunica- tions — Heinrich Hertz Institute, Germany, [email protected] 2 Fraunhofer Institute for Telecommunications — Heinrich Hertz Institute, Germany, [email protected] Abstract Digital media technologies have become an integral part of the way we create, communicate, and consume information. At the core of these technologies are source coding methods that are described in this text. Based on the fundamentals of information and rate distortion theory, the most relevant techniques used in source coding algorithms are de- scribed: entropy coding, quantization as well as predictive and trans- form coding. The emphasis is put onto algorithms that are also used in video coding, which will be described in the other text of this two-part monograph. To our families Contents 1 Introduction 1 1.1 The Communication Problem 3 1.2 Scope and Overview of the Text 4 1.3 The Source Coding Principle 5 2 Random Processes 7 2.1 Probability 8 2.2 Random Variables 9 2.2.1 Continuous Random Variables 10 2.2.2 Discrete Random Variables 11 2.2.3 Expectation 13 2.3 Random Processes 14 2.3.1 Markov Processes 16 2.3.2 Gaussian Processes 18 2.3.3 Gauss-Markov Processes 18 2.4 Summary of Random Processes 19 i ii Contents 3 Lossless Source Coding 20 3.1 Classification -
Relative Entropy Rate Between a Markov Chain and Its Corresponding Hidden Markov Chain
⃝c Statistical Research and Training Center دورهی ٨، ﺷﻤﺎرهی ١، ﺑﻬﺎر و ﺗﺎﺑﺴﺘﺎن ١٣٩٠، ﺻﺺ ٩٧–١٠٩ J. Statist. Res. Iran 8 (2011): 97–109 Relative Entropy Rate between a Markov Chain and Its Corresponding Hidden Markov Chain GH. Yariy and Z. Nikooraveshz;∗ y Iran University of Science and Technology z Birjand University of Technology Abstract. In this paper we study the relative entropy rate between a homo- geneous Markov chain and a hidden Markov chain defined by observing the output of a discrete stochastic channel whose input is the finite state space homogeneous stationary Markov chain. For this purpose, we obtain the rela- tive entropy between two finite subsequences of above mentioned chains with the help of the definition of relative entropy between two random variables then we define the relative entropy rate between these stochastic processes and study the convergence of it. Keywords. Relative entropy rate; stochastic channel; Markov chain; hid- den Markov chain. MSC 2010: 60J10, 94A17. 1 Introduction Suppose fXngn2N is a homogeneous stationary Markov chain with finite state space S = f0; 1; 2; :::; N − 1g and fYngn2N is a hidden Markov chain (HMC) which is observed through a discrete stochastic channel where the input of channel is the Markov chain. The output state space of channel is characterized by channel’s statistical properties. From now on we study ∗ Corresponding author 98 Relative Entropy Rate between a Markov Chain and Its ::: the channels state spaces which have been equal to the state spaces of input chains. Let P = fpabg be the one-step transition probability matrix of the Markov chain such that pab = P rfXn = bjXn−1 = ag for a; b 2 S and Q = fqabg be the noisy matrix of channel where qab = P rfYn = bjXn = ag for a; b 2 S. -
Information Content and Error Analysis
43 INFORMATION CONTENT AND ERROR ANALYSIS Clive D Rodgers Atmospheric, Oceanic and Planetary Physics University of Oxford ESA Advanced Atmospheric Training Course September 15th – 20th, 2008 44 INFORMATION CONTENT OF A MEASUREMENT Information in a general qualitative sense: Conceptually, what does y tell you about x? We need to answer this to determine if a conceptual instrument design actually works • to optimise designs • Use the linear problem for simplicity to illustrate the ideas. y = Kx + ! 45 SHANNON INFORMATION The Shannon information content of a measurement of x is the change in the entropy of the • probability density function describing our knowledge of x. Entropy is defined by: • S P = P (x) log(P (x)/M (x))dx { } − Z M(x) is a measure function. We will take it to be constant. Compare this with the statistical mechanics definition of entropy: • S = k p ln p − i i i X P (x)dx corresponds to pi. 1/M (x) is a kind of scale for dx. The Shannon information content of a measurement is the change in entropy between the p.d.f. • before, P (x), and the p.d.f. after, P (x y), the measurement: | H = S P (x) S P (x y) { }− { | } What does this all mean? 46 ENTROPY OF A BOXCAR PDF Consider a uniform p.d.f in one dimension, constant in (0,a): P (x)=1/a 0 <x<a and zero outside.The entropy is given by a 1 1 S = ln dx = ln a − a a Z0 „ « Similarly, the entropy of any constant pdf in a finite volume V of arbitrary shape is: 1 1 S = ln dv = ln V − V V ZV „ « i.e the entropy is the log of the volume of state space occupied by the p.d.f. -
Chapter 4 Information Theory
Chapter Information Theory Intro duction This lecture covers entropy joint entropy mutual information and minimum descrip tion length See the texts by Cover and Mackay for a more comprehensive treatment Measures of Information Information on a computer is represented by binary bit strings Decimal numb ers can b e represented using the following enco ding The p osition of the binary digit 3 2 1 0 Bit Bit Bit Bit Decimal Table Binary encoding indicates its decimal equivalent such that if there are N bits the ith bit represents N i the decimal numb er Bit is referred to as the most signicant bit and bit N as the least signicant bit To enco de M dierent messages requires log M bits 2 Signal Pro cessing Course WD Penny April Entropy The table b elow shows the probability of o ccurrence px to two decimal places of i selected letters x in the English alphab et These statistics were taken from Mackays i b o ok on Information Theory The table also shows the information content of a x px hx i i i a e j q t z Table Probability and Information content of letters letter hx log i px i which is a measure of surprise if we had to guess what a randomly chosen letter of the English alphab et was going to b e wed say it was an A E T or other frequently o ccuring letter If it turned out to b e a Z wed b e surprised The letter E is so common that it is unusual to nd a sentence without one An exception is the page novel Gadsby by Ernest Vincent Wright in which -
Entropy Rates & Markov Chains Information Theory Duke University, Fall 2020
ECE 587 / STA 563: Lecture 4 { Entropy Rates & Markov Chains Information Theory Duke University, Fall 2020 Author: Galen Reeves Last Modified: September 1, 2020 Outline of lecture: 4.1 Entropy Rate........................................1 4.2 Markov Chains.......................................3 4.3 Card Shuffling and MCMC................................4 4.4 Entropy of the English Language [Optional].......................6 4.1 Entropy Rate • A stochastic process fXig is an indexed sequence of random variables. They need not be in- n dependent nor identically distributed. For each n the distribution on X = (X1;X2; ··· ;Xn) is characterized by the joint pmf n pXn (x ) = p(x1; x2; ··· ; xn) • A stochastic process provides a useful probabilistic model. Examples include: ◦ the state of a deck of cards after each shuffle ◦ location of a molecule each millisecond. ◦ temperature each day ◦ sequence of letters in a book ◦ the closing price of the stock market each day. • With dependent sequences, hows does the entropy H(Xn) grow with n? (1) Definition 1: Average entropy per symbol H(X ;X ; ··· ;X ) H(X ) = lim 1 2 n n!1 n (2) Definition 2: Rate of information innovation 0 H (X ) = lim H(XnjX1;X2; ··· ;Xn−1) n!1 • If fXig are iid ∼ p(x), then both limits exists and are equal to H(X). nH(X) H(X ) = lim = H(X) n!1 n 0 H (X ) = lim H(XnjX1;X2; ··· ;Xn−1) = H(X) n!1 But what if the symbols are not iid? 2 ECE 587 / STA 563: Lecture 4 • A stochastic process is stationary if the joint distribution of subsets is invariant to shifts in the time index, i.e. -
Shannon Entropy and Kolmogorov Complexity
Information and Computation: Shannon Entropy and Kolmogorov Complexity Satyadev Nandakumar Department of Computer Science. IIT Kanpur October 19, 2016 This measures the average uncertainty of X in terms of the number of bits. Shannon Entropy Definition Let X be a random variable taking finitely many values, and P be its probability distribution. The Shannon Entropy of X is X 1 H(X ) = p(i) log : 2 p(i) i2X Shannon Entropy Definition Let X be a random variable taking finitely many values, and P be its probability distribution. The Shannon Entropy of X is X 1 H(X ) = p(i) log : 2 p(i) i2X This measures the average uncertainty of X in terms of the number of bits. The Triad Figure: Claude Shannon Figure: A. N. Kolmogorov Figure: Alan Turing Just Electrical Engineering \Shannon's contribution to pure mathematics was denied immediate recognition. I can recall now that even at the International Mathematical Congress, Amsterdam, 1954, my American colleagues in probability seemed rather doubtful about my allegedly exaggerated interest in Shannon's work, as they believed it consisted more of techniques than of mathematics itself. However, Shannon did not provide rigorous mathematical justification of the complicated cases and left it all to his followers. Still his mathematical intuition is amazingly correct." A. N. Kolmogorov, as quoted in [Shi89]. Kolmogorov and Entropy Kolmogorov's later work was fundamentally influenced by Shannon's. 1 Foundations: Kolmogorov Complexity - using the theory of algorithms to give a combinatorial interpretation of Shannon Entropy. 2 Analogy: Kolmogorov-Sinai Entropy, the only finitely-observable isomorphism-invariant property of dynamical systems. -
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 -
Understanding Shannon's Entropy Metric for Information
Understanding Shannon's Entropy metric for Information Sriram Vajapeyam [email protected] 24 March 2014 1. Overview Shannon's metric of "Entropy" of information is a foundational concept of information theory [1, 2]. Here is an intuitive way of understanding, remembering, and/or reconstructing Shannon's Entropy metric for information. Conceptually, information can be thought of as being stored in or transmitted as variables that can take on different values. A variable can be thought of as a unit of storage that can take on, at different times, one of several different specified values, following some process for taking on those values. Informally, we get information from a variable by looking at its value, just as we get information from an email by reading its contents. In the case of the variable, the information is about the process behind the variable. The entropy of a variable is the "amount of information" contained in the variable. This amount is determined not just by the number of different values the variable can take on, just as the information in an email is quantified not just by the number of words in the email or the different possible words in the language of the email. Informally, the amount of information in an email is proportional to the amount of “surprise” its reading causes. For example, if an email is simply a repeat of an earlier email, then it is not informative at all. On the other hand, if say the email reveals the outcome of a cliff-hanger election, then it is highly informative. -
Information Theory 1 Entropy 2 Mutual Information
CS769 Spring 2010 Advanced Natural Language Processing Information Theory Lecturer: Xiaojin Zhu [email protected] In this lecture we will learn about entropy, mutual information, KL-divergence, etc., which are useful concepts for information processing systems. 1 Entropy Entropy of a discrete distribution p(x) over the event space X is X H(p) = − p(x) log p(x). (1) x∈X When the log has base 2, entropy has unit bits. Properties: H(p) ≥ 0, with equality only if p is deterministic (use the fact 0 log 0 = 0). Entropy is the average number of 0/1 questions needed to describe an outcome from p(x) (the Twenty Questions game). Entropy is a concave function of p. 1 1 1 1 7 For example, let X = {x1, x2, x3, x4} and p(x1) = 2 , p(x2) = 4 , p(x3) = 8 , p(x4) = 8 . H(p) = 4 bits. This definition naturally extends to joint distributions. Assuming (x, y) ∼ p(x, y), X X H(p) = − p(x, y) log p(x, y). (2) x∈X y∈Y We sometimes write H(X) instead of H(p) with the understanding that p is the underlying distribution. The conditional entropy H(Y |X) is the amount of information needed to determine Y , if the other party knows X. X X X H(Y |X) = p(x)H(Y |X = x) = − p(x, y) log p(y|x). (3) x∈X x∈X y∈Y From above, we can derive the chain rule for entropy: H(X1:n) = H(X1) + H(X2|X1) + ..