Chapter 2 Source Models and Entropy. Any information-generating process can be viewed as. computer program in executed form: binary 0
|
|
- Rosamond French
- 5 years ago
- Views:
Transcription
1 Part II Information Theory Concepts Chapter 2 Source Models and Entropy Any information-generating process can be viewed as a source: { emitting a sequence of symbols { symbols from a nite alphabet text: ASCII symbols computer program in executed form: binary 0 and 1 n-bit image: 2 n symbols 1
2 Discrete Memoryless Sources (DMS) successive symbols statistically independent S = fs 1 ;s 2 ;:::;s n g fp(s 1 );p(s 2 );:::;p(s n )g I(s i ), the information revealed by the occurrence of a certain source symbol, is dened as I(s i ) = log 2 1 p(s i ) Average Information per source symbol, entropy H(s) = P p(si )I(s i )= P p(s i ) log 2 p(s i ) bits/symbol 2
3 Extensions of a Discrete Memoryless Source DMS S with an alphabet of size n the output of the source grouped into blocks of N symbols S N with an alphabet of size n N : the Nth extension of the source S For a memoryless source, the probability of a symbol i =(s i1 ;s i2 ;:::;s in ) from S N is given by p( i )=p(s i1 )p(s i2 ):::p(s in ) H(S N )=NH(S) 3
4 Markov Sources DMS too restrictive In general, the previous part of a message inuences the probabilities for the next symbol, the source has memory. In English text, the letter Q is almost always followed by the letter U. In digital images, the probability of a given pixel taking on a particular code value is dependent on the surrounding pixel values. 4
5 Such a source can be modeled as a Markov source. An mth-order Markov source: p(s i js j1 ;:::;s jm ) s j1 ;:::;s jm preceding to s i i; j k (k =1;2;:::;m)=1;2;:::;n (s j1 ;:::;s jm ): a state for the mth-order Markov source, a total of n m states For an ergodic Markov source, 9 a unique probability distribution over the set of states: stationary or equilibrium distribution. 5
6 H(Sjs j1 ;:::;s jm )= P ip(s i js j1 ;:::;s jm ) log p(s i js j1 ;:::;s jm ) H(S) = P S mh(sjs j 1 ;:::;s jm ) p(s j1 ;:::;s jm ) = P S p(s m+1 j 1 ;:::;s jm )p(s i js j1 ;:::;s jm ) log p(s i js j1 ;:::;s jm ) = P S p(s m+1 j 1 ;:::;s jm ;s i ) log p(s i js j1 ;:::;s jm ) 6
7 p(0 0,0)=0.8 0,0 p(1 0,0)=0.2 p(0 0,1)=0.5 p(0 1,0)=0.5 1,0 0,1 p(1 0,1)=0.5 p(1 1,0)=0.5 p(0 1,1)=0.2 1,1 p(1 1,1)=0.8 p(0; 0) = p(1; 1) = 5 2, p(0; 1) = p(1; 0) = H(S) = 0:801 bit/symbol 7
8 Extensions of a Markov Source and Adjoint Sources The Nth extension of a Markov source, S N,isathorder Markov source with symbols dened as blocks of N symbols from the original source, where = dm=ne As in the case of a DMS, H(S N )=NH(S) 8
9 The Nth extension of a Markov source, S N, with source symbols f 1 ; 2 ;:::; n Ngand stationary probabilities fp( 1 );p( 2 ); ;p( n N)g: a DMS with the same alphabet and the same symbol probabilities is called the adjoint source of S N and denoted by S N. { The adjoint source ignores the conditional probabilities which describe the dependence between the extended symbols. { H( S N ) H(S N ) { H N (S) = H( S N ) N!H(S) 9
10 The Noiseless Source Coding Theorem { S an ergodic source with an alphabet of size n and an entropy H(S) { encoding blocks of N source symbols at a time into binary codewords { For any >0, it is possible, by choosing N large enough, to construct a code so that the average number of bits per original source symbol, L, satises H(S) L H(S)+ 10
11 Chapter 3 Variable-Length Codes Variable-length codes with source extensions to achieve the entropy of a source { a DMS S = fs 1 ;s 2 ;s 3 ;s 4 ; p(s 1 )=0:60, p(s 2 )=0:30, p(s 3 )=0:05, p(s 4 )= 0:05g { each codeword in the sequence is instantaneously decodeable without reference to the succeeding codewords i no codeword be a prex of some other codeword (called by a prex condition code) 11
12 { entropy H(S) = P n p(s i=1 i)i(s i ) with I(s i )= log 2 p(s i ) { average codeword length or average length of the code, L P = n p(s i=1 i)l(s i ) with L(s i ) being the length of the codeword for s i { TohaveLH(S), we need L(s i ) log 2 p(s i )= 1 log bits 2 p(s i ) 1 or L(s i )=dlog e (bits) 2 p(s i ) { Shannon-Fano coding 12
13 Symbol Probability Code I Code II s s s s H(S) = 1:40 bits/symbol L 1 L 2 = 2:0 bits/symbol = 1:5 bits/symbol Acodeis compact (for a given source) if it has the smallest possible average codeword length. 13
14 Code Eciency and Source Extensions { Code II compact on S, its average codeword length is still far greater than H(S) { the code eciency: = H(S) L Code II: = 1:4 1:5 =0:93 { Extension to S 2 of 16 symbols formed as pairs of symbols from S. Table 3.2 shows a compact code of S 2, L =2:86 bits/extended symbol 14
15 = 1:43 bits/original source symbol = 1:40 1:43 =0:98 Human Codes for constructing compact codes { The Human code for a source fs 1 ;s 2 ghas trivial codewords \0" and \1". { Consider S = fs 1 ;s 2 ;:::;s n g (n>2) Let s n 1 ;s n be least probable symbols of this source. 15
16 Let Human code for fs 1 s 2 ; ;s n 2 ;fs n 1 ;s n gg be constructed and the codeword for fs n 1 ;s n g be w. Then Human code for fs 1 ; ;s n 1 ;s n g will be Human code for s 1 ; ;s n 2 and w0 for s n 1, w1 for s n. understanding Fig. 3 16
17 Modied Human Codes { Frequently, most of symbols in a large symbol set have very small probabilities. { Lump the less probable symbols into a symbol called \Else" and design a Human code for the reduced symbol set: the modied Human code. { Whenever a symbol in the ELSE category needs to be encoded, the encoder transmits the codeword for ELSE followed 17
18 by extra bits needed to identify the actual message within the ELSE category. the loss in coding eciency very small the storage requirements and the decoding complexity substantially reduced Group 3 international digital facsimile coding standards: { each binary image scan line: a sequence of alternating black and white runs which are encoded with separable variable-length code tables { A run is the number of times a particular value occurs consecutively along a scanline. 18
19 { 1728 pixels for each scanline { each Human table should have 1728 entries { greatly simplied by taking advantage of the fact that the longer runs are highly improbable { The rst 64 entries in each table represent the Human code for runs 0 to 63 { All other runs 64N + M (1 N 27, 0 M 64): entries for 64 to 90 encode N entries for 0 to 63 encode M 19
20 { a run of 213: N = 3 and M = 21 its Human code the entry 67(64 + 3) for N =3 the entry 21 for M =21 {simplifying the search for decoding Limitations of Human Coding { The ideal binary codeword length for a source symbol s i from a DMS is log 2 p(s i ), this condition is met only if p(s i )= 1. 2 k 20
21 { Otherwise, direct encoding of the individual source symbols may result in poor code eciency. p(s 1 ) 1, p(s 2 )=::: =p(s n )0 H(S) = p(s 1 ) log 2 p(s 1 ) P k2 p(s k ) log 2 p(s k ) (n 1)p(s 2 ) log 2 p(s 2 ) = (n 1) (1 p(s 1 )) (1 p(s log 1 )) (n 1) 2 (n 1) = (1 p(s 1 )) log 2 (1 p(s 1 )) (n 1)! 0 as p(s 1 )! 1 L 1 since the shortest codeword length for each individual symbol is one 21
22 { S = f0; 1g The Human codewords for \0" and \1" are \0" and \1", thus L = 1, regardless of the symbol probabilities. { Encoding an extended source may improve the coding eciency, but convergence to the source entropy could be slow. { The numberofentries in the Human code table grows exponentially with the block size. 22
23 { For an mth order Markov source, the conditional probabilities p(s i js i1 ;:::;s im ) vary as the state (s i1 ;:::;s im )changes. Thus, a separable Human table is needed for each state. { The coding eciency may still be low if the symbol conditional probabilities deviate from the ideal case. { Using an extended source and encoding the adjoint, its entropy H N may get close to the entropy H of the Markov source but the block size must be large. 23
24 { The Human coding cannot eciently adapt to changing source statistics { Arithmetic coding is more complex than Human coding, but it can overcome the limitations of Human coding 24
3F1 Information Theory, Lecture 3
3F1 Information Theory, Lecture 3 Jossy Sayir Department of Engineering Michaelmas 2013, 29 November 2013 Memoryless Sources Arithmetic Coding Sources with Memory Markov Example 2 / 21 Encoding the output
More informationUNIT I INFORMATION THEORY. I k log 2
UNIT I INFORMATION THEORY Claude Shannon 1916-2001 Creator of Information Theory, lays the foundation for implementing logic in digital circuits as part of his Masters Thesis! (1939) and published a paper
More informationChapter 3 Source Coding. 3.1 An Introduction to Source Coding 3.2 Optimal Source Codes 3.3 Shannon-Fano Code 3.4 Huffman Code
Chapter 3 Source Coding 3. An Introduction to Source Coding 3.2 Optimal Source Codes 3.3 Shannon-Fano Code 3.4 Huffman Code 3. An Introduction to Source Coding Entropy (in bits per symbol) implies in average
More informationUncertainity, Information, and Entropy
Uncertainity, Information, and Entropy Probabilistic experiment involves the observation of the output emitted by a discrete source during every unit of time. The source output is modeled as a discrete
More informationMotivation for Arithmetic Coding
Motivation for Arithmetic Coding Motivations for arithmetic coding: 1) Huffman coding algorithm can generate prefix codes with a minimum average codeword length. But this length is usually strictly greater
More information3F1 Information Theory, Lecture 3
3F1 Information Theory, Lecture 3 Jossy Sayir Department of Engineering Michaelmas 2011, 28 November 2011 Memoryless Sources Arithmetic Coding Sources with Memory 2 / 19 Summary of last lecture Prefix-free
More informationELEMENT OF INFORMATION THEORY
History Table of Content ELEMENT OF INFORMATION THEORY O. Le Meur olemeur@irisa.fr Univ. of Rennes 1 http://www.irisa.fr/temics/staff/lemeur/ October 2010 1 History Table of Content VERSION: 2009-2010:
More information1 Ex. 1 Verify that the function H(p 1,..., p n ) = k p k log 2 p k satisfies all 8 axioms on H.
Problem sheet Ex. Verify that the function H(p,..., p n ) = k p k log p k satisfies all 8 axioms on H. Ex. (Not to be handed in). looking at the notes). List as many of the 8 axioms as you can, (without
More informationBandwidth: Communicate large complex & highly detailed 3D models through lowbandwidth connection (e.g. VRML over the Internet)
Compression Motivation Bandwidth: Communicate large complex & highly detailed 3D models through lowbandwidth connection (e.g. VRML over the Internet) Storage: Store large & complex 3D models (e.g. 3D scanner
More informationLecture 4 : Adaptive source coding algorithms
Lecture 4 : Adaptive source coding algorithms February 2, 28 Information Theory Outline 1. Motivation ; 2. adaptive Huffman encoding ; 3. Gallager and Knuth s method ; 4. Dictionary methods : Lempel-Ziv
More informationAn instantaneous code (prefix code, tree code) with the codeword lengths l 1,..., l N exists if and only if. 2 l i. i=1
Kraft s inequality An instantaneous code (prefix code, tree code) with the codeword lengths l 1,..., l N exists if and only if N 2 l i 1 Proof: Suppose that we have a tree code. Let l max = max{l 1,...,
More informationInformation and Entropy
Information and Entropy Shannon s Separation Principle Source Coding Principles Entropy Variable Length Codes Huffman Codes Joint Sources Arithmetic Codes Adaptive Codes Thomas Wiegand: Digital Image Communication
More informationChapter 2 Date Compression: Source Coding. 2.1 An Introduction to Source Coding 2.2 Optimal Source Codes 2.3 Huffman Code
Chapter 2 Date Compression: Source Coding 2.1 An Introduction to Source Coding 2.2 Optimal Source Codes 2.3 Huffman Code 2.1 An Introduction to Source Coding Source coding can be seen as an efficient way
More informationMultimedia Communications. Mathematical Preliminaries for Lossless Compression
Multimedia Communications Mathematical Preliminaries for Lossless Compression What we will see in this chapter Definition of information and entropy Modeling a data source Definition of coding and when
More informationDigital Communications III (ECE 154C) Introduction to Coding and Information Theory
Digital Communications III (ECE 154C) Introduction to Coding and Information Theory Tara Javidi These lecture notes were originally developed by late Prof. J. K. Wolf. UC San Diego Spring 2014 1 / 8 I
More informationCSCI 2570 Introduction to Nanocomputing
CSCI 2570 Introduction to Nanocomputing Information Theory John E Savage What is Information Theory Introduced by Claude Shannon. See Wikipedia Two foci: a) data compression and b) reliable communication
More informationIntroduction to Information Theory. By Prof. S.J. Soni Asst. Professor, CE Department, SPCE, Visnagar
Introduction to Information Theory By Prof. S.J. Soni Asst. Professor, CE Department, SPCE, Visnagar Introduction [B.P. Lathi] Almost in all the means of communication, none produces error-free communication.
More informationEntropy as a measure of surprise
Entropy as a measure of surprise Lecture 5: Sam Roweis September 26, 25 What does information do? It removes uncertainty. Information Conveyed = Uncertainty Removed = Surprise Yielded. How should we quantify
More informationCOMM901 Source Coding and Compression. Quiz 1
German University in Cairo - GUC Faculty of Information Engineering & Technology - IET Department of Communication Engineering Winter Semester 2013/2014 Students Name: Students ID: COMM901 Source Coding
More informationEE 121: Introduction to Digital Communication Systems. 1. Consider the following discrete-time communication system. There are two equallly likely
EE 11: Introduction to Digital Communication Systems Midterm Solutions 1. Consider the following discrete-time communication system. There are two equallly likely messages to be transmitted, and they are
More information54 D. S. HOODA AND U. S. BHAKER Belis and Guiasu [2] observed that a source is not completely specied by the probability distribution P over the sourc
SOOCHOW JOURNAL OF MATHEMATICS Volume 23, No. 1, pp. 53-62, January 1997 A GENERALIZED `USEFUL' INFORMATION MEASURE AND CODING THEOREMS BY D. S. HOODA AND U. S. BHAKER Abstract. In the present communication
More informationDigital communication system. Shannon s separation principle
Digital communication system Representation of the source signal by a stream of (binary) symbols Adaptation to the properties of the transmission channel information source source coder channel coder modulation
More informationCompression and Coding
Compression and Coding Theory and Applications Part 1: Fundamentals Gloria Menegaz 1 Transmitter (Encoder) What is the problem? Receiver (Decoder) Transformation information unit Channel Ordering (significance)
More informationData Compression Techniques
Data Compression Techniques Part 2: Text Compression Lecture 5: Context-Based Compression Juha Kärkkäinen 14.11.2017 1 / 19 Text Compression We will now look at techniques for text compression. These techniques
More informationCh 0 Introduction. 0.1 Overview of Information Theory and Coding
Ch 0 Introduction 0.1 Overview of Information Theory and Coding Overview The information theory was founded by Shannon in 1948. This theory is for transmission (communication system) or recording (storage
More informationRun-length & Entropy Coding. Redundancy Removal. Sampling. Quantization. Perform inverse operations at the receiver EEE
General e Image Coder Structure Motion Video x(s 1,s 2,t) or x(s 1,s 2 ) Natural Image Sampling A form of data compression; usually lossless, but can be lossy Redundancy Removal Lossless compression: predictive
More informationMultimedia. Multimedia Data Compression (Lossless Compression Algorithms)
Course Code 005636 (Fall 2017) Multimedia Multimedia Data Compression (Lossless Compression Algorithms) Prof. S. M. Riazul Islam, Dept. of Computer Engineering, Sejong University, Korea E-mail: riaz@sejong.ac.kr
More informationMARKOV CHAINS A finite state Markov chain is a sequence of discrete cv s from a finite alphabet where is a pmf on and for
MARKOV CHAINS A finite state Markov chain is a sequence S 0,S 1,... of discrete cv s from a finite alphabet S where q 0 (s) is a pmf on S 0 and for n 1, Q(s s ) = Pr(S n =s S n 1 =s ) = Pr(S n =s S n 1
More informationECE Advanced Communication Theory, Spring 2009 Homework #1 (INCOMPLETE)
ECE 74 - Advanced Communication Theory, Spring 2009 Homework #1 (INCOMPLETE) 1. A Huffman code finds the optimal codeword to assign to a given block of source symbols. (a) Show that cannot be a Huffman
More informationChapter 2: Source coding
Chapter 2: meghdadi@ensil.unilim.fr University of Limoges Chapter 2: Entropy of Markov Source Chapter 2: Entropy of Markov Source Markov model for information sources Given the present, the future is independent
More information2018/5/3. YU Xiangyu
2018/5/3 YU Xiangyu yuxy@scut.edu.cn Entropy Huffman Code Entropy of Discrete Source Definition of entropy: If an information source X can generate n different messages x 1, x 2,, x i,, x n, then the
More informationCS6304 / Analog and Digital Communication UNIT IV - SOURCE AND ERROR CONTROL CODING PART A 1. What is the use of error control coding? The main use of error control coding is to reduce the overall probability
More informationIntroduction to information theory and coding
Introduction to information theory and coding Louis WEHENKEL Set of slides No 4 Source modeling and source coding Stochastic processes and models for information sources First Shannon theorem : data compression
More informationChapter 5: Data Compression
Chapter 5: Data Compression Definition. A source code C for a random variable X is a mapping from the range of X to the set of finite length strings of symbols from a D-ary alphabet. ˆX: source alphabet,
More informationGeneralized Kraft Inequality and Arithmetic Coding
J. J. Rissanen Generalized Kraft Inequality and Arithmetic Coding Abstract: Algorithms for encoding and decoding finite strings over a finite alphabet are described. The coding operations are arithmetic
More informationBasic Principles of Lossless Coding. Universal Lossless coding. Lempel-Ziv Coding. 2. Exploit dependences between successive symbols.
Universal Lossless coding Lempel-Ziv Coding Basic principles of lossless compression Historical review Variable-length-to-block coding Lempel-Ziv coding 1 Basic Principles of Lossless Coding 1. Exploit
More informationITCT Lecture IV.3: Markov Processes and Sources with Memory
ITCT Lecture IV.3: Markov Processes and Sources with Memory 4. Markov Processes Thus far, we have been occupied with memoryless sources and channels. We must now turn our attention to sources with memory.
More informationEntropies & Information Theory
Entropies & Information Theory LECTURE I Nilanjana Datta University of Cambridge,U.K. See lecture notes on: http://www.qi.damtp.cam.ac.uk/node/223 Quantum Information Theory Born out of Classical Information
More informationEC2252 COMMUNICATION THEORY UNIT 5 INFORMATION THEORY
EC2252 COMMUNICATION THEORY UNIT 5 INFORMATION THEORY Discrete Messages and Information Content, Concept of Amount of Information, Average information, Entropy, Information rate, Source coding to increase
More informationChapter 4. Data Transmission and Channel Capacity. Po-Ning Chen, Professor. Department of Communications Engineering. National Chiao Tung University
Chapter 4 Data Transmission and Channel Capacity Po-Ning Chen, Professor Department of Communications Engineering National Chiao Tung University Hsin Chu, Taiwan 30050, R.O.C. Principle of Data Transmission
More informationExercise 1. = P(y a 1)P(a 1 )
Chapter 7 Channel Capacity Exercise 1 A source produces independent, equally probable symbols from an alphabet {a 1, a 2 } at a rate of one symbol every 3 seconds. These symbols are transmitted over a
More information! Where are we on course map? ! What we did in lab last week. " How it relates to this week. ! Compression. " What is it, examples, classifications
Lecture #3 Compression! Where are we on course map?! What we did in lab last week " How it relates to this week! Compression " What is it, examples, classifications " Probability based compression # Huffman
More informationSource Coding. Master Universitario en Ingeniería de Telecomunicación. I. Santamaría Universidad de Cantabria
Source Coding Master Universitario en Ingeniería de Telecomunicación I. Santamaría Universidad de Cantabria Contents Introduction Asymptotic Equipartition Property Optimal Codes (Huffman Coding) Universal
More informationIntroduction to information theory and coding
Introduction to information theory and coding Louis WEHENKEL Set of slides No 5 State of the art in data compression Stochastic processes and models for information sources First Shannon theorem : data
More informationData Compression Techniques
Data Compression Techniques Part 1: Entropy Coding Lecture 4: Asymmetric Numeral Systems Juha Kärkkäinen 08.11.2017 1 / 19 Asymmetric Numeral Systems Asymmetric numeral systems (ANS) is a recent entropy
More informationImplementation of Lossless Huffman Coding: Image compression using K-Means algorithm and comparison vs. Random numbers and Message source
Implementation of Lossless Huffman Coding: Image compression using K-Means algorithm and comparison vs. Random numbers and Message source Ali Tariq Bhatti 1, Dr. Jung Kim 2 1,2 Department of Electrical
More informationMAHALAKSHMI ENGINEERING COLLEGE-TRICHY QUESTION BANK UNIT V PART-A. 1. What is binary symmetric channel (AUC DEC 2006)
MAHALAKSHMI ENGINEERING COLLEGE-TRICHY QUESTION BANK SATELLITE COMMUNICATION DEPT./SEM.:ECE/VIII UNIT V PART-A 1. What is binary symmetric channel (AUC DEC 2006) 2. Define information rate? (AUC DEC 2007)
More informationEE376A: Homework #3 Due by 11:59pm Saturday, February 10th, 2018
Please submit the solutions on Gradescope. EE376A: Homework #3 Due by 11:59pm Saturday, February 10th, 2018 1. Optimal codeword lengths. Although the codeword lengths of an optimal variable length code
More informationHuffman Coding. C.M. Liu Perceptual Lab, College of Computer Science National Chiao-Tung University
Huffman Coding C.M. Liu Perceptual Lab, College of Computer Science National Chiao-Tung University http://www.csie.nctu.edu.tw/~cmliu/courses/compression/ Office: EC538 (03)573877 cmliu@cs.nctu.edu.tw
More informationSIGNAL COMPRESSION Lecture Shannon-Fano-Elias Codes and Arithmetic Coding
SIGNAL COMPRESSION Lecture 3 4.9.2007 Shannon-Fano-Elias Codes and Arithmetic Coding 1 Shannon-Fano-Elias Coding We discuss how to encode the symbols {a 1, a 2,..., a m }, knowing their probabilities,
More informationCommunications Theory and Engineering
Communications Theory and Engineering Master's Degree in Electronic Engineering Sapienza University of Rome A.A. 2018-2019 AEP Asymptotic Equipartition Property AEP In information theory, the analog of
More informationChapter 9 Fundamental Limits in Information Theory
Chapter 9 Fundamental Limits in Information Theory Information Theory is the fundamental theory behind information manipulation, including data compression and data transmission. 9.1 Introduction o For
More informationCoding for Discrete Source
EGR 544 Communication Theory 3. Coding for Discrete Sources Z. Aliyazicioglu Electrical and Computer Engineering Department Cal Poly Pomona Coding for Discrete Source Coding Represent source data effectively
More information1 Introduction to information theory
1 Introduction to information theory 1.1 Introduction In this chapter we present some of the basic concepts of information theory. The situations we have in mind involve the exchange of information through
More informationMAHALAKSHMI ENGINEERING COLLEGE QUESTION BANK. SUBJECT CODE / Name: EC2252 COMMUNICATION THEORY UNIT-V INFORMATION THEORY PART-A
MAHALAKSHMI ENGINEERING COLLEGE QUESTION BANK DEPARTMENT: ECE SEMESTER: IV SUBJECT CODE / Name: EC2252 COMMUNICATION THEORY UNIT-V INFORMATION THEORY PART-A 1. What is binary symmetric channel (AUC DEC
More informationInformation Theory - Entropy. Figure 3
Concept of Information Information Theory - Entropy Figure 3 A typical binary coded digital communication system is shown in Figure 3. What is involved in the transmission of information? - The system
More informationImage and Multidimensional Signal Processing
Image and Multidimensional Signal Processing Professor William Hoff Dept of Electrical Engineering &Computer Science http://inside.mines.edu/~whoff/ Image Compression 2 Image Compression Goal: Reduce amount
More informationU Logo Use Guidelines
COMP2610/6261 - Information Theory Lecture 15: Arithmetic Coding U Logo Use Guidelines Mark Reid and Aditya Menon logo is a contemporary n of our heritage. presents our name, d and our motto: arn the nature
More informationBasic information theory
Basic information theory Communication system performance is limited by Available signal power Background noise Bandwidth limits. Can we postulate an ideal system based on physical principles, against
More informationAlon Orlitsky. AT&T Bell Laboratories. March 22, Abstract
Average-case interactive communication Alon Orlitsky AT&T Bell Laboratories March 22, 1996 Abstract and Y are random variables. Person P knows, Person P Y knows Y, and both know the joint probability distribution
More informationLecture 4 Noisy Channel Coding
Lecture 4 Noisy Channel Coding I-Hsiang Wang Department of Electrical Engineering National Taiwan University ihwang@ntu.edu.tw October 9, 2015 1 / 56 I-Hsiang Wang IT Lecture 4 The Channel Coding Problem
More informationInformation Theory and Coding Techniques
Information Theory and Coding Techniques Lecture 1.2: Introduction and Course Outlines Information Theory 1 Information Theory and Coding Techniques Prof. Ja-Ling Wu Department of Computer Science and
More informationUpper Bounds on the Capacity of Binary Intermittent Communication
Upper Bounds on the Capacity of Binary Intermittent Communication Mostafa Khoshnevisan and J. Nicholas Laneman Department of Electrical Engineering University of Notre Dame Notre Dame, Indiana 46556 Email:{mhoshne,
More informationSource Coding Techniques
Source Coding Techniques. Huffman Code. 2. Two-pass Huffman Code. 3. Lemple-Ziv Code. 4. Fano code. 5. Shannon Code. 6. Arithmetic Code. Source Coding Techniques. Huffman Code. 2. Two-path Huffman Code.
More informationExercises with solutions (Set B)
Exercises with solutions (Set B) 3. A fair coin is tossed an infinite number of times. Let Y n be a random variable, with n Z, that describes the outcome of the n-th coin toss. If the outcome of the n-th
More informationDCSP-3: Minimal Length Coding. Jianfeng Feng
DCSP-3: Minimal Length Coding Jianfeng Feng Department of Computer Science Warwick Univ., UK Jianfeng.feng@warwick.ac.uk http://www.dcs.warwick.ac.uk/~feng/dcsp.html Automatic Image Caption (better than
More informationAn introduction to basic information theory. Hampus Wessman
An introduction to basic information theory Hampus Wessman Abstract We give a short and simple introduction to basic information theory, by stripping away all the non-essentials. Theoretical bounds on
More informationSummary of Last Lectures
Lossless Coding IV a k p k b k a 0.16 111 b 0.04 0001 c 0.04 0000 d 0.16 110 e 0.23 01 f 0.07 1001 g 0.06 1000 h 0.09 001 i 0.15 101 100 root 1 60 1 0 0 1 40 0 32 28 23 e 17 1 0 1 0 1 0 16 a 16 d 15 i
More informationCMPT 365 Multimedia Systems. Lossless Compression
CMPT 365 Multimedia Systems Lossless Compression Spring 2017 Edited from slides by Dr. Jiangchuan Liu CMPT365 Multimedia Systems 1 Outline Why compression? Entropy Variable Length Coding Shannon-Fano Coding
More informationOptimal codes - I. A code is optimal if it has the shortest codeword length L. i i. This can be seen as an optimization problem. min.
Huffman coding Optimal codes - I A code is optimal if it has the shortest codeword length L L m = i= pl i i This can be seen as an optimization problem min i= li subject to D m m i= lp Gabriele Monfardini
More information17.1 Binary Codes Normal numbers we use are in base 10, which are called decimal numbers. Each digit can be 10 possible numbers: 0, 1, 2, 9.
( c ) E p s t e i n, C a r t e r, B o l l i n g e r, A u r i s p a C h a p t e r 17: I n f o r m a t i o n S c i e n c e P a g e 1 CHAPTER 17: Information Science 17.1 Binary Codes Normal numbers we use
More informationFibonacci Coding for Lossless Data Compression A Review
RESEARCH ARTICLE OPEN ACCESS Fibonacci Coding for Lossless Data Compression A Review Ezhilarasu P Associate Professor Department of Computer Science and Engineering Hindusthan College of Engineering and
More informationModule 1. Introduction to Digital Communications and Information Theory. Version 2 ECE IIT, Kharagpur
Module ntroduction to Digital Communications and nformation Theory Lesson 3 nformation Theoretic Approach to Digital Communications After reading this lesson, you will learn about Scope of nformation Theory
More informationInformation Sources. Professor A. Manikas. Imperial College London. EE303 - Communication Systems An Overview of Fundamentals
Information Sources Professor A. Manikas Imperial College London EE303 - Communication Systems An Overview of Fundamentals Prof. A. Manikas (Imperial College) EE303: Information Sources 24 Oct. 2011 1
More informationlossless, optimal compressor
6. Variable-length Lossless Compression The principal engineering goal of compression is to represent a given sequence a, a 2,..., a n produced by a source as a sequence of bits of minimal possible length.
More informationInformation Theory CHAPTER. 5.1 Introduction. 5.2 Entropy
Haykin_ch05_pp3.fm Page 207 Monday, November 26, 202 2:44 PM CHAPTER 5 Information Theory 5. Introduction As mentioned in Chapter and reiterated along the way, the purpose of a communication system is
More informationMATH 433 Applied Algebra Lecture 21: Linear codes (continued). Classification of groups.
MATH 433 Applied Algebra Lecture 21: Linear codes (continued). Classification of groups. Binary codes Let us assume that a message to be transmitted is in binary form. That is, it is a word in the alphabet
More informationChannel capacity. Outline : 1. Source entropy 2. Discrete memoryless channel 3. Mutual information 4. Channel capacity 5.
Channel capacity Outline : 1. Source entropy 2. Discrete memoryless channel 3. Mutual information 4. Channel capacity 5. Exercices Exercise session 11 : Channel capacity 1 1. Source entropy Given X a memoryless
More informationLecture 4 Channel Coding
Capacity and the Weak Converse Lecture 4 Coding I-Hsiang Wang Department of Electrical Engineering National Taiwan University ihwang@ntu.edu.tw October 15, 2014 1 / 16 I-Hsiang Wang NIT Lecture 4 Capacity
More informationShannon s noisy-channel theorem
Shannon s noisy-channel theorem Information theory Amon Elders Korteweg de Vries Institute for Mathematics University of Amsterdam. Tuesday, 26th of Januari Amon Elders (Korteweg de Vries Institute for
More informationELEC 515 Information Theory. Distortionless Source Coding
ELEC 515 Information Theory Distortionless Source Coding 1 Source Coding Output Alphabet Y={y 1,,y J } Source Encoder Lengths 2 Source Coding Two coding requirements The source sequence can be recovered
More informationBasic Principles of Video Coding
Basic Principles of Video Coding Introduction Categories of Video Coding Schemes Information Theory Overview of Video Coding Techniques Predictive coding Transform coding Quantization Entropy coding Motion
More informationEECS 229A Spring 2007 * * (a) By stationarity and the chain rule for entropy, we have
EECS 229A Spring 2007 * * Solutions to Homework 3 1. Problem 4.11 on pg. 93 of the text. Stationary processes (a) By stationarity and the chain rule for entropy, we have H(X 0 ) + H(X n X 0 ) = H(X 0,
More informationModule 2 LOSSLESS IMAGE COMPRESSION SYSTEMS. Version 2 ECE IIT, Kharagpur
Module 2 LOSSLESS IMAGE COMPRESSION SYSTEMS Lesson 5 Other Coding Techniques Instructional Objectives At the end of this lesson, the students should be able to:. Convert a gray-scale image into bit-plane
More informationReduce the amount of data required to represent a given quantity of information Data vs information R = 1 1 C
Image Compression Background Reduce the amount of data to represent a digital image Storage and transmission Consider the live streaming of a movie at standard definition video A color frame is 720 480
More informationShannon-Fano-Elias coding
Shannon-Fano-Elias coding Suppose that we have a memoryless source X t taking values in the alphabet {1, 2,..., L}. Suppose that the probabilities for all symbols are strictly positive: p(i) > 0, i. The
More informationCapacity of the Discrete Memoryless Energy Harvesting Channel with Side Information
204 IEEE International Symposium on Information Theory Capacity of the Discrete Memoryless Energy Harvesting Channel with Side Information Omur Ozel, Kaya Tutuncuoglu 2, Sennur Ulukus, and Aylin Yener
More informationA Comparison of Methods for Redundancy Reduction in Recurrence Time Coding
1 1 A Comparison of Methods for Redundancy Reduction in Recurrence Time Coding Hidetoshi Yokoo, Member, IEEE Abstract Recurrence time of a symbol in a string is defined as the number of symbols that have
More informationBASICS OF COMPRESSION THEORY
BASICS OF COMPRESSION THEORY Why Compression? Task: storage and transport of multimedia information. E.g.: non-interlaced HDTV: 0x0x0x = Mb/s!! Solutions: Develop technologies for higher bandwidth Find
More informationPART III. Outline. Codes and Cryptography. Sources. Optimal Codes (I) Jorge L. Villar. MAMME, Fall 2015
Outline Codes and Cryptography 1 Information Sources and Optimal Codes 2 Building Optimal Codes: Huffman Codes MAMME, Fall 2015 3 Shannon Entropy and Mutual Information PART III Sources Information source:
More informationText Compression. Jayadev Misra The University of Texas at Austin December 5, A Very Incomplete Introduction to Information Theory 2
Text Compression Jayadev Misra The University of Texas at Austin December 5, 2003 Contents 1 Introduction 1 2 A Very Incomplete Introduction to Information Theory 2 3 Huffman Coding 5 3.1 Uniquely Decodable
More informationX 1 : X Table 1: Y = X X 2
ECE 534: Elements of Information Theory, Fall 200 Homework 3 Solutions (ALL DUE to Kenneth S. Palacio Baus) December, 200. Problem 5.20. Multiple access (a) Find the capacity region for the multiple-access
More informationEntropy Coding. Connectivity coding. Entropy coding. Definitions. Lossles coder. Input: a set of symbols Output: bitstream. Idea
Connectivity coding Entropy Coding dd 7, dd 6, dd 7, dd 5,... TG output... CRRRLSLECRRE Entropy coder output Connectivity data Edgebreaker output Digital Geometry Processing - Spring 8, Technion Digital
More informationAutumn Coping with NP-completeness (Conclusion) Introduction to Data Compression
Autumn Coping with NP-completeness (Conclusion) Introduction to Data Compression Kirkpatrick (984) Analogy from thermodynamics. The best crystals are found by annealing. First heat up the material to let
More informationLecture 5: Channel Capacity. Copyright G. Caire (Sample Lectures) 122
Lecture 5: Channel Capacity Copyright G. Caire (Sample Lectures) 122 M Definitions and Problem Setup 2 X n Y n Encoder p(y x) Decoder ˆM Message Channel Estimate Definition 11. Discrete Memoryless Channel
More informationSIDDHARTH GROUP OF INSTITUTIONS :: PUTTUR Siddharth Nagar, Narayanavanam Road UNIT I
SIDDHARTH GROUP OF INSTITUTIONS :: PUTTUR Siddharth Nagar, Narayanavanam Road 517583 QUESTION BANK (DESCRIPTIVE) Subject with Code : CODING THEORY & TECHNIQUES(16EC3810) Course & Branch: M.Tech - DECS
More informationLecture 2: Introduction to Audio, Video & Image Coding Techniques (I) -- Fundaments
Lecture 2: Introduction to Audio, Video & Image Coding Techniques (I) -- Fundaments Dr. Jian Zhang Conjoint Associate Professor NICTA & CSE UNSW COMP9519 Multimedia Systems S2 2006 jzhang@cse.unsw.edu.au
More information10-704: Information Processing and Learning Fall Lecture 9: Sept 28
10-704: Information Processing and Learning Fall 2016 Lecturer: Siheng Chen Lecture 9: Sept 28 Note: These notes are based on scribed notes from Spring15 offering of this course. LaTeX template courtesy
More informationFeedback Capacity of a Class of Symmetric Finite-State Markov Channels
Feedback Capacity of a Class of Symmetric Finite-State Markov Channels Nevroz Şen, Fady Alajaji and Serdar Yüksel Department of Mathematics and Statistics Queen s University Kingston, ON K7L 3N6, Canada
More informationData Compression Techniques (Spring 2012) Model Solutions for Exercise 2
582487 Data Compression Techniques (Spring 22) Model Solutions for Exercise 2 If you have any feedback or corrections, please contact nvalimak at cs.helsinki.fi.. Problem: Construct a canonical prefix
More information