Safwan El Assad - Digital Communications 1

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Digital Communications 1: краткое содержание, описание и аннотация

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It is a complete training in digital communications in the same book with all the aspects involved in such training: courses, tutorials with many typical problems targeted with detailed solutions, practical work concretely illustrating various aspects of technical implementation implemented. It breaks down into three parts. The Theory of information itself, which concerns both the sources of information and the channels of its transmission, taking into account the errors they introduce in the transmission of information and the means of protect by the use of appropriate coding methods. Then for the technical aspects of transmission, first the baseband transmission is presented with the important concept and fundamental technique of equalization. The performance evaluation in terms of probability of errors is systematically developed and detailed as well as the online codes used. Finally, the third part presents the Transmissions with digital modulation of carriers used in radio transmissions but also on electric cables. A second important aspect in learning a learner's knowledge and skills is this book. It concerns the «Directed Work» aspect of a training. This is an ordered set of 33 typical problems with detailed solutions covering the different parts of the course with practical work. Finally, the last aspect concerns the practical aspects in the proper sense of the term, an essential complement to training going as far as know-how. We propose here a set of 5 practical works.

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2

Measurement of Information of a Discrete Source and Channel Capacity

2.1. Introduction and definitions

The purpose of a message is to provide information to a recipient. Information, like energy, for that matter, is a fundamental notion, which is part of our daily life. It can be transported (transmitted), stored (memorized) and transformed (processed).

The value of information lies in the surprise effect it causes; it is all the more interesting because it is less predictable . As a result, information is assimilated to an event of a random nature, considered, in the following, as a random variable.

The measure of the information is then given by measuring the uncertainty of an event system , that is to say, the random choice of an event in a set of possible and distinct events.

We will use the terms message or sequence to indicate any finite sequence of symbols taken in an alphabet A = { } of a discrete source: a finite set of predetermined symbols, for example:

We will use the term discrete source of information Sn to indicate the system - фото 14

We will use the term discrete source of information Sn to indicate the system selecting, from the set of symbols from As = S , the symbols to transmit:

The choice of smn is carried out according to a given probability law which - фото 15

The choice of sm,n is carried out according to a given probability law, which can be steady temporally or variable over time.

2.2. Examples of discrete sources

2.2.1. Simple source (memoryless)

This is a source for which the probability of the occurrence of a symbol does not depend on the previous symbols:

[2.1] 22 222 Discrete source with memory It is a source for which the - фото 16

[2.2] 222 Discrete source with memory It is a source for which the probability - фото 17

2.2.2. Discrete source with memory

It is a source for which the probability of occurrence of a symbol depends on the symbols already emitted (statistical dependence) and on instants 1, 2, ..., n where they have been emitted:

[2.3] If the source is in addition stationary then the dependence is only on the - фото 18

If the source is in addition stationary then the dependence is only on the ranks and not on the moments when the symbols have been transmitted, so:

[2.4] that is the statistical properties are independent of any temporal translation - фото 19

that is, the statistical properties are independent of any temporal translation . We can consider that a text written in any language is an example of such a source.

2.2.3. Ergodic source: stationary source with finite memory

The ergodicity of an information source implies that a temporal average calculated over an infinite duration is equal to the statistical average.

2.2.4. First order Markovian source (first order Markov chain)

First order Markov sources play an important role in several domains, for example, in (Caragata et al . 2015), the authors used such a source to model the cryptanalysis of a digital watermarking algorithm.

It is characterized by:

[2.5] with The probability plk is called transi - фото 20

with:

The probability plk is called transition probability from state l to state k - фото 21

The probability Digital Communications 1 - изображение 22= pl,k is called transition probability from state l to state k , and:

[2.6] Digital Communications 1 - изображение 23

The probability that at time n the source is in the state k is:

[2.7] By introducing matrix notations 28 Taking into account the relationship - фото 24

By introducing matrix notations:

[2.8] Digital Communications 1 - изображение 25

Taking into account the relationship [2.8], the relation [2.7]is also written as:

[2.9] Digital Communications 1 - изображение 26

where Tt is the transposed matrix of transition probabilities.

Moreover, if the source is, stationary, then:

Digital Communications 1 - изображение 27

in other words, the probabilities of the occurrence of the symbols do not depend on n. It is the same for the transition probabilities pl,k , then the relation [2.9]is written:

[2.10] Digital Communications 1 - изображение 28

where P 0is the matrix of probabilities governing the generation of symbols by the source at the initial instant n = 0.

2.3. Uncertainty, amount of information and entropy (Shannon’s 1948 theorem)

The realization of an event x of probability p(x) conveys a quantity of information h(x) related to its uncertainty. h(x) is an increasing function of its improbability 1/ p ( x ):

Digital Communications 1 - изображение 29

If an event x is certain, then p( x ) = 1, the uncertainty is zero and therefore the quantity of information h( x ) brought by its realization is null.

Moreover, let us consider the realization of a pair of independent events x and y . Their joint realization leads to the amount of information it brings being the sum of the quantities of information brought by each of them:

[2.11] but ft xy is also written 212 so from the relationships 211and - фото 30

but ft( x,y ) is also written:

[2.12] so from the relationships 211and 212 the form of the function f is of - фото 31

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