13.07.2015 Views

Mathematical Methods for Physics and Engineering - Matematica.NET

Mathematical Methods for Physics and Engineering - Matematica.NET

Mathematical Methods for Physics and Engineering - Matematica.NET

SHOW MORE
SHOW LESS

You also want an ePaper? Increase the reach of your titles

YUMPU automatically turns print PDFs into web optimized ePapers that Google loves.

30.15 IMPORTANT JOINT DISTRIBUTIONSwhere∣ ∣∣∣∣∣∣∣∣∣ ∂x 1 ∂x∣n ∣∣∣∣∣∣∣∣∣...J ≡ ∂(x ∂y 1 ∂y 11,x 2 ...,x n )∂(y 1 ,y 2 ,...,y n ) = .. .. . ,∂x 1 ∂x n...∂y n ∂y nis the Jacobian of the x i with respect to the y j .◮Suppose that the r<strong>and</strong>om variables X i , i =1, 2,...,n, are independent <strong>and</strong> Gaussian distributedwith means µ i <strong>and</strong> variances σi2 respectively. Find the PDF <strong>for</strong> the new variablesZ i =(X i − µ i )/σ i , i =1, 2,...,n. By considering an elemental spherical shell in Z-space,find the PDF of the chi-squared r<strong>and</strong>om variable χ 2 n = ∑ ni=1 Z i 2 .Since the X i are independent r<strong>and</strong>om variables,[]1n∑ (x i − µ i ) 2f(x 1 ,x 2 ,...,x n )=f(x 1 )f(x 2 ) ···f(x n )=exp −.(2π) n/2 σ 1 σ 2 ···σ n 2σ 2 i=1 iTo derive the PDF <strong>for</strong> the variables Z i ,werequire|f(x 1 ,x 2 ,...,x n ) dx 1 dx 2 ···dx n | = |g(z 1 ,z 2 ,...,z n ) dz 1 dz 2 ···dz n |,<strong>and</strong>, noting that dz i = dx i /σ i ,weobtain)1g(z 1 ,z 2 ,...,z n )=(−(2π) exp 1 n∑z n/2 i2 .2i=1Let us now consider the r<strong>and</strong>om variable χ 2 n = ∑ ni=1 Z i 2 , which we may regard as thesquare of the distance from the origin in the n-dimensional Z-space. We now require thatg(z 1 ,z 2 ,...,z n ) dz 1 dz 2 ···dz n = h(χ 2 n)dχ 2 n.If we consider the infinitesimal volume dV = dz 1 dz 2 ···dz n to be that enclosed by then-dimensional spherical shell of radius χ n <strong>and</strong> thickness dχ n then we may write dV =dχ n , <strong>for</strong> some constant A. We thus obtainAχ n−1nh(χ 2 n)dχ 2 n ∝ exp(− 1 2 χ2 n)χ n−1n dχ n ∝ exp(− 1 2 χ2 n)χn n−2 dχ 2 n,where we have used the fact that dχ 2 n =2χ n dχ n . Thus we see that the PDF <strong>for</strong> χ 2 n is givenbyh(χ 2 n)=B exp(− 1 2 χ2 n)χ n−2n ,<strong>for</strong> some constant B. This constant may be determined from the normalisation condition∫ ∞h(χ 2 n) dχ 2 n =10<strong>and</strong> is found to be B = [2 n/2 Γ( 1 2 n)]−1 . This is the nth-order chi-squared distributiondiscussed in subsection 30.9.4. ◭30.15 Important joint distributionsIn this section we will examine two important multivariate distributions, themultinomial distribution, which is an extension of the binomial distribution, <strong>and</strong>the multivariate Gaussian distribution.1207

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!