# A Tutorial on Multivariate Statistical Analysis

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• A Tutorial on

Multivariate

Statistical Analysis

Craig A. Tracy

UC Davis

SAMSI

September 2006

1

• ELEMENTARY STATISTICS

Collection of (real-valued) data from a sequence of experiments

X1, X2, . . . , Xn

Might make assumption underlying law is N(, 2) with unknown

mean and variance 2. Want to estimate and 2 from the data.

Sample Mean & Sample Variance:

X =1

n

j

Xj , S =1

n 1

j

(

Xj X)2

Estimators are unbiased

E(X) = , E(S) = 2

2

• Theorem: If X1, X2, . . . are independent N(, 2) variables then

X and S are independent. We have that X is N(, 2/n) and

(n 1)S/2 is 2(n 1).

Recall 2(d) denotes the chi-squared distribution with d degrees of

freedom. Its density is

f2(x) =1

2d/2 (d/2)xd/21 ex/2 , x 0,

where

(z) =

0

tz1 et dt, (z) > 0.

3

• MULTIVARIATE GENERALIZATIONS

From the classic textbook of Anderson:

Multivariate statistical analysis is concerned with data that

consists of sets of measurements on a number of individuals

or objects. The sample data may be heights and weights of

some individuals drawn randomly from a population of

school children in a given city, or the statistical treatment

may be made on a collection of measurements, such as

lengths and widths of petals and lengths and widths of

sepals of iris plants taken from two species, or one may

study the scores on batteries of mental tests administered

to a number of students.

p = # of sets of measurements on a given individual,

n = # of observations = sample size

4

• Remarks:

In above examples, one can assume that p n since typicallymany measurements will be taken.

Today it is common for p 1, so n/p is no longer necessarilylarge.

Vehicle Sound Signature Recognition: Vehicle noise is a

stochastic signal. The power spectrum is discretized to a

vector of length p = 1200 with n 1200 samples from thesame kind of vehicle.

Astrophysics: Sloan Digital Sky Survey typically has many

observations (say of quasar spectrum) with the spectra of

each quasar binned resulting in a large p.

Financial data: S&P 500 stocks observed over monthly

intervals for twenty years.

5

• GAUSSIAN DATA MATRICES

The data are now n independent column vectors of length p

~x1, ~x2, . . . , ~xn

from which we construct the n p data matrix

X =

~xT1 ~xT2

...

~xTn

The Gaussian assumption is that

~xj Np(,)

Many applications assume the mean has been already substracted

out of the data, i.e. = 0.

6

• Multivariate Gaussian Distribution

If x and y are vectors, the matrix x y is defined by

(x y)jk = xjyk

If = E(x) is the mean of the random vector x, then the

covariance matrix of x is the p p matrix

= E [(x ) (x )]]

is a symmetric, non-negative definite matrix. If > 0 (positive

definite) and X Np(,), then the density function of X is

fX(x) = (2)p/2(det)1/2 exp

[

12

(

x ,1(x )

]

, > x Rp

Sample mean:

x =1

n

j

~xj , E(x) =

7

• Sample covariance matrix:

S =1

n 1

n

j=1

(~xj x) (~xj x)

For = 0 the sample covariance matrix can be written simply as

1

n 1 XTX

Some Notation: If X is a n p data matrix formed from the nindependent column vectors xj , cov(xj) = , we can form one

column vector vec(X) of length pn

vec(X) =

x1

x2...

xn

8

• The covariance of vec(X) is the np np matrix

In =

0 0 00 0 0...

......

...

0 0 0

In this case we say the data matrix X constructed from n

independent xj Np(,) has distribution

Np(M, In )

where M = E(X) = 1 , 1 is the column vector of all 1s.

9

• WISHART DISTRIBUTION

Definition: If A = XTX where the n p matrix X isNp(0, In ), > 0, then A is said to have Wishart distributionwith n degrees of freedom and covariance matrix . We will say A

is Wp(n,).

Remarks:

The Wishart distribution is the multivariate generalization ofthe chi-squared distribution.

A Wp(n,) is positive definite with probability one if andonly if n p. The sample covariance matrix,

S =1

n 1 A

is Wp(n 1, 1n1 ).

10

• WISHART DENSITY FUNCTION, n p

Let Sp denote the space of p p positive definite (symmetric)matrices. If A = (ajk) Sp, let

(dA) = volume element of A =

jk

dajk

The multivariate gamma function is

p(a) =

Sp

etr(A) (detA)a(p+1)/2 (dA),(a) > (p 1)/2.

Theorem: If A is Wp(n,) with n p, then the density functionof A is

1

2np p(n/2) (det)n/2e

12 tr(

1A) (detA)(np1)/2

11

• Sketch of Proof:

The density function for X is the multivariate Gaussian(including volume element (dX))

(2)np/2 (det)n/2

e12 tr(

1XT X) (dX)

Recall the QR factorization : Let X denote an n p matrixwith n p with full column rank. Then there exists an uniquen p matrix Q, QTQ = Ip, and an unique n p uppertriangular matrix R with positive diagonal elements so that

X = QR. Note A = XTX = RTR.

A Jacobian calculation [1, 13]: If A = XTX , then

(dX) = 2p (detA)(np1)/2 (dA)(QTdQ)

12

• where

(QTdQ) =

p

j=1

n

k=j+1

qTk dqj

and Q = (q1, . . . , qp) is the column representation of Q.

Thus the joint distribution of A and Q is

(2)np/2 (det)n/2 e12 tr(

1A)

2p (detA)(np1)/2

(dA)(QT dQ)

Now integrate over all Q. Use fact that

Vn,p

(QT dQ) =2pnp/2

p(n/2)

and Vn,p is the set of real n p matrices Q satisfyingQTQ = Ip. (When n = p this is the orthogonal group.)

13

• Remarks regarding the Wishart density function

Case p = 2 obtain by R. A. Fisher in 1915. General p by J. Wishart in 1928 by geometrical arguments. Proof outlined above came later. (See [1, 13] for complete

proof.)

When Q is a p p orthogonal matrixp(p/2)

2pp2/2(

QT dQ)

is normalized Haar measure for the orthogonal group O(p). Wedenote this Haar measure by (dQ).

Siegel proved (see, e.g. )

p(a) = p(p1)/4

p

j=1

(

a 12(j 1)

)

14

• EIGENVALUES OF A WISHART MATRIX

Theorem: If A is Wp(n,) with n p the joint density functionfor the eigenvalues 1,. . . , p of A is

p2/2 2np/2 (det)n/2

p(p/2) p(n/2)

p

j=1

(np1)/2j

j > p)

where L = diag(1, . . . , p) and (dQ) is normalized Haar measure.

Note that () :=

j

• Proof: Recall that the Wishart density function (times the volume

element) is

1

2np p(n/2) (det)n/2e

12 tr(

1A) (detA)(np1)/2 (dA)

The idea is to diagonalize A by an orthogonal transformation and

then integrate over the orthogonal group thereby giving the density

function for the eigenvalues of A.

Let 1 > > p be the ordered eigenvalues of A.

A = QLQT , L = diag(1, . . . , p), Q O(p)

The jth column of Q is a normalized eigenvector of A. The

transformation is not 11 since Q = [q1, . . . ,qp] works for eachfixed A. The transformation is made 11 by requiring that the 1st

element of each qj is nonnegative. This restricts Q (as A varies) to

a 2p part of O(p). We compensate for this at the end.

16

• We need an expression for the volume element (dA) in terms of Q

and L. First we compute the differential of A

dA = dQLQT +QdLQT +QLdQT

QT dAQ = QT dQL+ dL+ LdQT Q

= dQtQdL+ LdQT Q+ dL=

[

L, dQTQ]

+ dL

(We used QTQ = I implies QT dQ = dQT Q.)We now use the following fact (see, e.g., page 58 in ): If

X = BY BT where X and Y are p p symmetric matrices, B is anonsingular p p matrix, then (dX) = (detB)p+1(dY ). In our caseQ is orthogonal so the volume element (dA) equals the volume

element (QT dAQ). The volume element is the exterior product of

the diagonal elements of QT dAQ times the exterior product of the

elements above the diagonal.

17

• Since L is diagonal, the commutator[

L, dQTQ]

has zero diagonal elements. Thus the exterior product of the

diagonal elements of QT dAQ is

j dj .

The exterior product of the elements coming from the commutator

is

j

• One is interested in limit laws as n, p. For = Ip,Johnstone  proved, using RMT methods, for centering and

scaling constants

np =(n 1 +p

)2,

np =(n 1 +p

)

(

1n 1

+1p

)1/3

that1 npnp

converges in distribution as n, p, n/p

• For 6= Ip, the difficulty in establishing limit theorms comesfrom the integral

O(p)

e12 tr(

1QQT ) (dQ)

Using zonal polynomials infinite series expansions have been

derived for this integral, but these expansions are difficult to

For complex Gaussian data matrices X similar density formulasare known for the eigenvalues of XX . Limit theorems for

6= Ip are known since the analogous group integral, now overthe unitary group, is known explicitlythe Harish

ChandraItzyksonZuber (HCIZ) integral (see, e.g. ). See

the work of Baik, Ben Arous and Peche [2, 3] and El Karoui .

20

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