Mathematical Methods for Physics and Engineering : A Comprehensive Guide

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30.9 IMPORTANT CONTINUOUS DISTRIBUTIONS


30.9.4 The chi-squared distribution

In subsection 30.6.2, we showed that ifXis Gaussian distributed with meanμand


varianceσ^2 , such thatX∼N(μ, σ^2 ), then the random variableY=(x−μ)^2 /σ^2


is distributed as the gamma distributionY ∼γ(^12 ,^12 ). Let us now considern


independent Gaussian random variablesXi∼N(μi,σi^2 ),i=1, 2 ,...,n, and define


the new variable


χ^2 n=

∑n

i=1

(Xi−μi)^2
σ^2 i

. (30.122)


Using the result (30.121) for multiple gamma distributions,χ^2 nmust be distributed


as the gamma variateχ^2 n∼γ(^12 ,^12 n), which from (30.118) has the PDF


f(χ^2 n)=

1
2
Γ(^12 n)

(^12 χ^2 n)(n/2)−^1 exp(−^12 χ^2 n)

=

1
2 n/^2 Γ(^12 n)

(χ^2 n)(n/2)−^1 exp(−^12 χ^2 n). (30.123)

This is known as thechi-squared distributionof ordernand has numerous


applications in statistics (see chapter 31). Settingλ=^12 andr=^12 nin (30.120),


we find that


E[χ^2 n]=n, V[χ^2 n]=2n.

An important generalisation occurs when thenGaussian variablesXiarenot

linearly independent but are instead required to satisfy a linear constraint of the


form


c 1 X 1 +c 2 X 2 +···+cnXn=0, (30.124)

in which the constantsciare not all zero. In this case, it may be shown (see


exercise 30.40) that the variableχ^2 ndefined in (30.122) is still described by a chi-


squared distribution, but one of ordern−1. Indeed, this result may be trivially


extended to show that if thenGaussian variablesXisatisfymlinear constraints


of the form (30.124) then the variableχ^2 ndefined in (30.122) is described by a


chi-squared distribution of ordern−m.


30.9.5 The Cauchy and Breit–Wigner distributions

A random variableX(in the range−∞to∞) that obeys theCauchy distribution


is described by the PDF


f(x)=

1
π

1
1+x^2

.
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