1. Error-Correcting Codes 2. Sphere Packings and Lattices 3. Sporadic Simple Groups
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Hamming Code - Wikipedia, the Free Encyclopedia Hamming Code Hamming Code
Hamming code - Wikipedia, the free encyclopedia Hamming code Hamming code From Wikipedia, the free encyclopedia In telecommunication, a Hamming code is a linear error-correcting code named after its inventor, Richard Hamming. Hamming codes can detect and correct single-bit errors, and can detect (but not correct) double-bit errors. In contrast, the simple parity code cannot detect errors where two bits are transposed, nor can it correct the errors it can find. Contents [hide] • 1 History • 2 Codes predating Hamming ♦ 2.1 Parity ♦ 2.2 Two-out-of-five code ♦ 2.3 Repetition • 3 Hamming codes • 4 Example using the (11,7) Hamming code • 5 Hamming code (7,4) ♦ 5.1 Hamming matrices ♦ 5.2 Channel coding ♦ 5.3 Parity check ♦ 5.4 Error correction • 6 Hamming codes with additional parity • 7 See also • 8 References • 9 External links History Hamming worked at Bell Labs in the 1940s on the Bell Model V computer, an electromechanical relay-based machine with cycle times in seconds. Input was fed in on punch cards, which would invariably have read errors. During weekdays, special code would find errors and flash lights so the operators could correct the problem. During after-hours periods and on weekends, when there were no operators, the machine simply moved on to the next job. Hamming worked on weekends, and grew increasingly frustrated with having to restart his programs from scratch due to the unreliability of the card reader. Over the next few years he worked on the problem of error-correction, developing an increasingly powerful array of algorithms. -
Reed-Solomon Error Correction
R&D White Paper WHP 031 July 2002 Reed-Solomon error correction C.K.P. Clarke Research & Development BRITISH BROADCASTING CORPORATION BBC Research & Development White Paper WHP 031 Reed-Solomon Error Correction C. K. P. Clarke Abstract Reed-Solomon error correction has several applications in broadcasting, in particular forming part of the specification for the ETSI digital terrestrial television standard, known as DVB-T. Hardware implementations of coders and decoders for Reed-Solomon error correction are complicated and require some knowledge of the theory of Galois fields on which they are based. This note describes the underlying mathematics and the algorithms used for coding and decoding, with particular emphasis on their realisation in logic circuits. Worked examples are provided to illustrate the processes involved. Key words: digital television, error-correcting codes, DVB-T, hardware implementation, Galois field arithmetic © BBC 2002. All rights reserved. BBC Research & Development White Paper WHP 031 Reed-Solomon Error Correction C. K. P. Clarke Contents 1 Introduction ................................................................................................................................1 2 Background Theory....................................................................................................................2 2.1 Classification of Reed-Solomon codes ...................................................................................2 2.2 Galois fields............................................................................................................................3 -
Linear Block Codes
Linear Block codes (n, k) Block codes k – information bits n - encoded bits Block Coder Encoding operation n-digit codeword made up of k-information digits and (n-k) redundant parity check digits. The rate or efficiency for this code is k/n. 푘 푁푢푚푏푒푟 표푓 푛푓표푟푚푎푡표푛 푏푡푠 퐶표푑푒 푒푓푓푐푒푛푐푦 푟 = = 푛 푇표푡푎푙 푛푢푚푏푒푟 표푓 푏푡푠 푛 푐표푑푒푤표푟푑 Note: unlike source coding, in which data is compressed, here redundancy is deliberately added, to achieve error detection. SYSTEMATIC BLOCK CODES A systematic block code consists of vectors whose 1st k elements (or last k-elements) are identical to the message bits, the remaining (n-k) elements being check bits. A code vector then takes the form: X = (m0, m1, m2,……mk-1, c0, c1, c2,…..cn-k) Or X = (c0, c1, c2,…..cn-k, m0, m1, m2,……mk-1) Systematic code: information digits are explicitly transmitted together with the parity check bits. For the code to be systematic, the k-information bits must be transmitted contiguously as a block, with the parity check bits making up the code word as another contiguous block. Information bits Parity bits A systematic linear block code will have a generator matrix of the form: G = [P | Ik] Systematic codewords are sometimes written so that the message bits occupy the left-hand portion of the codeword and the parity bits occupy the right-hand portion. Parity check matrix (H) Will enable us to decode the received vectors. For each (kxn) generator matrix G, there exists an (n-k)xn matrix H, such that rows of G are orthogonal to rows of H i.e., GHT = 0, where HT is the transpose of H. -
An Introduction to Coding Theory
An introduction to coding theory Adrish Banerjee Department of Electrical Engineering Indian Institute of Technology Kanpur Kanpur, Uttar Pradesh India Feb. 6, 2017 Lecture #6A: Some simple linear block codes -I Adrish Banerjee Department of Electrical Engineering Indian Institute of Technology Kanpur Kanpur, Uttar Pradesh India An introduction to coding theory Outline of the lecture Dual code. Adrish Banerjee Department of Electrical Engineering Indian Institute of Technology Kanpur Kanpur, Uttar Pradesh India An introduction to coding theory Outline of the lecture Dual code. Examples of linear block codes Adrish Banerjee Department of Electrical Engineering Indian Institute of Technology Kanpur Kanpur, Uttar Pradesh India An introduction to coding theory Outline of the lecture Dual code. Examples of linear block codes Repetition code Adrish Banerjee Department of Electrical Engineering Indian Institute of Technology Kanpur Kanpur, Uttar Pradesh India An introduction to coding theory Outline of the lecture Dual code. Examples of linear block codes Repetition code Single parity check code Adrish Banerjee Department of Electrical Engineering Indian Institute of Technology Kanpur Kanpur, Uttar Pradesh India An introduction to coding theory Outline of the lecture Dual code. Examples of linear block codes Repetition code Single parity check code Hamming code Adrish Banerjee Department of Electrical Engineering Indian Institute of Technology Kanpur Kanpur, Uttar Pradesh India An introduction to coding theory Dual code Two n-tuples u and v are orthogonal if their inner product (u, v)is zero, i.e., n (u, v)= (ui · vi )=0 i=1 Adrish Banerjee Department of Electrical Engineering Indian Institute of Technology Kanpur Kanpur, Uttar Pradesh India An introduction to coding theory Dual code Two n-tuples u and v are orthogonal if their inner product (u, v)is zero, i.e., n (u, v)= (ui · vi )=0 i=1 For a binary linear (n, k) block code C,the(n, n − k) dual code, Cd is defined as set of all codewords, v that are orthogonal to all the codewords u ∈ C. -
Error-Correction and the Binary Golay Code
London Mathematical Society Impact150 Stories 1 (2016) 51{58 C 2016 Author(s) doi:10.1112/i150lms/t.0003 e Error-correction and the binary Golay code R.T.Curtis Abstract Linear algebra and, in particular, the theory of vector spaces over finite fields has provided a rich source of error-correcting codes which enable the receiver of a corrupted message to deduce what was originally sent. Although more efficient codes have been devised in recent years, the 12- dimensional binary Golay code remains one of the most mathematically fascinating such codes: not only has it been used to send messages back to earth from the Voyager space probes, but it is also involved in many of the most extraordinary and beautiful algebraic structures. This article describes how the code can be obtained in two elementary ways, and explains how it can be used to correct errors which arise during transmission 1. Introduction Whenever a message is sent - along a telephone wire, over the internet, or simply by shouting across a crowded room - there is always the possibly that the message will be damaged during transmission. This may be caused by electronic noise or static, by electromagnetic radiation, or simply by the hubbub of people in the room chattering to one another. An error-correcting code is a means by which the original message can be recovered by the recipient even though it has been corrupted en route. Most commonly a message is sent as a sequence of 0s and 1s. Usually when a 0 is sent a 0 is received, and when a 1 is sent a 1 is received; however occasionally, and hopefully rarely, a 0 is sent but a 1 is received, or vice versa. -
The Binary Golay Code and the Leech Lattice
The binary Golay code and the Leech lattice Recall from previous talks: Def 1: (linear code) A code C over a field F is called linear if the code contains any linear combinations of its codewords A k-dimensional linear code of length n with minimal Hamming distance d is said to be an [n, k, d]-code. Why are linear codes interesting? ● Error-correcting codes have a wide range of applications in telecommunication. ● A field where transmissions are particularly important is space probes, due to a combination of a harsh environment and cost restrictions. ● Linear codes were used for space-probes because they allowed for just-in-time encoding, as memory was error-prone and heavy. Space-probe example The Hamming weight enumerator Def 2: (weight of a codeword) The weight w(u) of a codeword u is the number of its nonzero coordinates. Def 3: (Hamming weight enumerator) The Hamming weight enumerator of C is the polynomial: n n−i i W C (X ,Y )=∑ Ai X Y i=0 where Ai is the number of codeword of weight i. Example (Example 2.1, [8]) For the binary Hamming code of length 7 the weight enumerator is given by: 7 4 3 3 4 7 W H (X ,Y )= X +7 X Y +7 X Y +Y Dual and doubly even codes Def 4: (dual code) For a code C we define the dual code C˚ to be the linear code of codewords orthogonal to all of C. Def 5: (doubly even code) A binary code C is called doubly even if the weights of all its codewords are divisible by 4. -
Tcom 370 Notes 99-8 Error Control: Block Codes
TCOM 370 NOTES 99-8 ERROR CONTROL: BLOCK CODES THE NEED FOR ERROR CONTROL The physical link is always subject to imperfections (noise/interference, limited bandwidth/distortion, timing errors) so that individual bits sent over the physical link cannot be received with zero error probability. A bit error -6 rate (BER) of 10 , which may sound quite low and very good, actually leads 1 on the average to an error every -th second for transmission at 10 Mbps. 10 -7 Even with better links, say BER=10 , one would make on the average one error in transferring a binary file of size 1.25 Mbytes. This is not acceptable for "reliable" data transmission. We need to provide in the data link control protocols (Layer 2 of the ISO 7- layer OSI protocol architecture) a means for obtaining better reliability than can be guaranteed by the physical link itself. Note: Error control can be (and is) also incorporated at a higher layer, the transport layer. ERROR CONTROL TECHNIQUES Error Detection and Automatic Request for Retransmission (ARQ) This is a "feedback" mode of operation and depends on the receiver being able to detect that an error has occurred. (Error detection is easier than error correction at the receiver). Upon detecting an error in a frame of transmitted bits, the receiver asks for a retransmission of the frame. This may happen at the data link layer or at the transport layer. The characteristics of ARQ techniques will be discussed in more detail in a subsequent set of notes, where the delays introduced by the ARQ process will be considered explicitly. -
OPTIMIZING SIZES of CODES 1. Introduction to Coding Theory Error
OPTIMIZING SIZES OF CODES LINDA MUMMY Abstract. This paper shows how to determine if codes are of optimal size. We discuss coding theory terms and techniques, including Hamming codes, perfect codes, cyclic codes, dual codes, and parity-check matrices. 1. Introduction to Coding Theory Error correcting codes and check digits were developed to counter the effects of static interference in transmissions. For example, consider the use of the most basic code. Let 0 stand for \no" and 1 stand for \yes." A mistake in one digit relaying this message can change the entire meaning. Therefore, this is a poor code. One option to increase the probability that the correct message is received is to send the message multiple times, like 000000 or 111111, hoping that enough instances of the correct message get through that the receiver is able to comprehend the original meaning. This, however, is an inefficient method of relaying data. While some might associate \coding theory" with cryptography and \secret codes," the two fields are very different. Coding theory deals with transmitting a codeword, say x, and ensuring that the receiver is able to determine the original message x even if there is some static or interference in transmission. Cryptogra- phy deals with methods to ensure that besides the sender and the receiver of the message, no one is able to encode or decode the message. We begin by discussing a real life example of the error checking codes (ISBN numbers) which appear on all books printed after 1964. We go on to discuss different types of codes and the mathematical theories behind their structures. -
Low-Density Parity-Check Codes—A Statistical Physics Perspective
ADVANCES IN IMAGING AND ELECTRON PHYSICS, VOL. 125 Low-Density Parity-Check Codes—A Statistical Physics Perspective 1, 1 RENATO VICENTE, ∗ DAVID SAAD AND YOSHIYUKI KABASHIMA2 1Neural Computing Research Group, University of Aston, Birmingham B4 7ET, United Kingdom 2Department of Computational Intelligence and Systems Science, Tokyo Institute of Technology, Yokohama 2268502, Japan I. Introduction ............................. 232 A. Error Correction .......................... 232 B. Statistical Physics of Coding ..................... 236 C. Outline ............................. 236 II. Coding and Statistical Physics ..................... 237 A. Mathematical Model for a Communication System ........... 237 1. Data Source and Sink ...................... 238 2. Source Encoder and Decoder ................... 238 3. Noisy Channels ......................... 239 4. Channel Encoder and Decoder ................... 241 B. Linear Error-Correcting Codes and the Decoding Problem ........ 242 C. Probability Propagation Algorithm .................. 244 D. Low-Density Parity-Check Codes .................. 250 E. Decoding and Statistical Physics ................... 250 III. Sourlas Codes ............................ 252 A. Lower Bound for the Probability of Bit Error .............. 254 B. Replica Theory for the Typical Performance of Sourlas Codes ....... 256 C. Shannon’s Bound ......................... 262 D. Decoding with Probability Propagation ................ 266 IV. Gallager Codes ........................... 270 A. Upper Bound on Achievable Rates -
An Introduction to Coding Theory
An introduction to coding theory Adrish Banerjee Department of Electrical Engineering Indian Institute of Technology Kanpur Kanpur, Uttar Pradesh India Feb. 6, 2017 Lecture #7A: Bounds on the size of a code Adrish Banerjee Department of Electrical Engineering Indian Institute of Technology Kanpur Kanpur, Uttar Pradesh India An introduction to coding theory Outline of the lecture Hamming bound Adrish Banerjee Department of Electrical Engineering Indian Institute of Technology Kanpur Kanpur, Uttar Pradesh India An introduction to coding theory Outline of the lecture Hamming bound Perfect codes Adrish Banerjee Department of Electrical Engineering Indian Institute of Technology Kanpur Kanpur, Uttar Pradesh India An introduction to coding theory Outline of the lecture Hamming bound Perfect codes Singleton bound Adrish Banerjee Department of Electrical Engineering Indian Institute of Technology Kanpur Kanpur, Uttar Pradesh India An introduction to coding theory Outline of the lecture Hamming bound Perfect codes Singleton bound Maximum distance separable codes Adrish Banerjee Department of Electrical Engineering Indian Institute of Technology Kanpur Kanpur, Uttar Pradesh India An introduction to coding theory Outline of the lecture Hamming bound Perfect codes Singleton bound Maximum distance separable codes Plotkin Bound Adrish Banerjee Department of Electrical Engineering Indian Institute of Technology Kanpur Kanpur, Uttar Pradesh India An introduction to coding theory Outline of the lecture Hamming bound Perfect codes Singleton bound Maximum distance separable codes Plotkin Bound Gilbert-Varshamov bound Adrish Banerjee Department of Electrical Engineering Indian Institute of Technology Kanpur Kanpur, Uttar Pradesh India An introduction to coding theory Bounds on the size of a code The basic problem is to find the largest code of a given length, n and minimum distance, d. -
Coding Theory: Linear-Error Correcting Codes 1 Basic Definitions
Anna Dovzhik 1 Coding Theory: Linear-Error Correcting Codes Anna Dovzhik Math 420: Advanced Linear Algebra Spring 2014 Sharing data across channels, such as satellite, television, or compact disc, often comes at the risk of error due to noise. A well-known example is the task of relaying images of planets from space; given the incredible distance that this data must travel, it is be to expected that interference will occur. Since about 1948, coding theory has been utilized to help detect and correct corrupted messages such as these, by introducing redundancy into an encoded message, which provides a means by which to detect errors. Although non-linear codes exist, the focus here will be on algebraic coding, which is efficient and often used in practice. 1 Basic Definitions The following build up a basic vocabulary of coding theory. Definition 1.1 If A = a1; a2; : : : ; aq, then A is a code alphabet of size q and an 2 A is a code symbol. For our purposes, A will be a finite field Fq. Definition 1.2 A q-ary word w of length n is a vector that has each of its components in the code alphabet. Definition 1.3 A q-ary block code is a set C over an alphabet A, where each element, or codeword, is a q-ary word of length n. Note that jCj is the size of C. A code of length n and size M is called an (n; M)-code. Example 1.1 [3, p.6] C = f00; 01; 10; 11g is a binary (2,4)-code taken over the code alphabet F2 = f0; 1g . -
CSCI 234 - Design of Internet Protocols Error Detection and Correction
CSCI 234 - Design of Internet Protocols Error Detection and Correction CSCI 234 Design of Internet Protocols: Error Detection and Correction George Blankenship Error Detection and George Blankenship 1 Correction Outline • Effect of Transmission Errors • Cause of Transmission Errors • Detection of Transmission Errors • Correction of Transmission Errors Error Detection and George Blankenship 2 Correction Effects of Errors • Data may distorted (bit inversion) • Data may be deleted (unrecognizable) • Data may be added (merged messages) • Data may be reordered (queuing delays) Error Detection and George Blankenship 3 Correction George Blankenship 1 CSCI 234 - Design of Internet Protocols Error Detection and Correction Place of Errors (Layered Model) • All errors are bit-based • Bit insertion and distortion takes place at Physical Layer (PHY) – transmission errors • Data Link (DL) Layer, provides well- defined service interface to the Network Layer and recovers from transmission errors • Network Layer and above suffer from implementation (software/hardware) errors Error Detection and George Blankenship 4 Correction Impact of Transmission Error • Problem: some data sent from A Æ B may get ‘corrupted’ – Why is this a big problem? How will the receiver know they received “bad data”? • “bad data” is directly proportional to the probability of a transmission error Error detection and Correction reduce the impact of a transmission error Error Detection and George Blankenship 5 Correction Handling Transmission Errors • Example: – “hello, world” is