Received 29 March 2016; accepted 14 June 2016; published 17 June 2016

1. Introduction
An expression for a multivariate Student’s t-distribution is presented. This expression, which is different in form than the form that is commonly used, allows the shape parameter
for each marginal probability density function (pdf) of the multivariate pdf to be different.
The form that is typically used is [1]
(1)
This “typical” form attempts to generalize the univariate Student’s t-distribution and is valid when the n marginal distributions have the same shape parameter
. The shape of this multivariate t-distribution arises from the observation that the pdf for
is given by Equation (1) when
is distributed as a multivariate normal distribution with covariance matrix
and
is distributed as chi-squared.
The multivariate Student’s t-distribution put forth here is derived from a Cholesky decomposition of the scale matrix by analogy to the multivariate normal (Gaussian) pdf. The derivation of the multivariate normal pdf is given in Section 2 to provide background. The multivariate Student’s t-distribution and the variances and covariances for the multivariate t-distribution are given in Section 3. Section 4 is a conclusion.
2. Background Information
2.1. Cholesky Decomposition
A method to produce a multivariate pdf with known scale matrix
is presented in this section. For nor- mally distributed variables, the covariance matrix
since the scale factor for a normal distribution is the standard deviation of the distribution. An example with
is used to provide concrete examples.
Consider the transformation
where
and
are
column matrices,
is
square matrix, and the elements of
are independent random variables. The off-diagonal elements of
introduce correlations between the elements of
.
(2)
The scale matrix
. The covariance matrix
has elements
where
is the expectation of
and
. If the
are normally distributed, then
, where the superscript T indicates a transpose of the matrix. If
is known, then
is the Cholesky decomposition of the matrix
[2] .
For the
example of Equation (2),
(3)
From linear algebra,
. For
as defined in Equation (2),
and
whereas
is the va- riance of the zero-mean random variable
and
is the covariance of the zero-mean
random variables
and
.
2.2. Multivariate Normal Probability Density Function
To create a multivariate normal pdf, start with the joint pdf
for n unit normal, zero mean, independent random variables
:
(4)
where
is an n-row column matrix:
.
gives the probability that the random variables
lie in the interval
.
The requirement for zero mean random variables is not a restriction. If
, then
is a zero mean random variable with the same shape and scale parameters as
.
Use Equation (2) to transform the variables. The Jacobian determinant of the transformation relates the products of the infinitesimals of integration such that
(5)
The magnitude of the Jacobian determinant of the transformation
is (Appendix)
(6)
where the equality
has been used.
Since
,
, and since
, the multivariate “z-score”
becomes
, which equals
since
for
normally distributed variables.
The result is that the unit normal, independent, multivariate pdf, Equation (4), becomes under the trans- formation Equation (2)
(7)
where
is a n-row column matrix:
and
.
For the
example,
(8)
from which
can be calculated. In Equation (8),
(9)
The denominator in the expression for
is
.
3. Multivariate Student’s t Probability Density Function
A similar approach can be used to create a multivariate Student’s t pdf. Assume truncated or effectively truncated t-distributions, so that moments exist [3] [4] . For simplicity, assume that support is
where b is a positive, large number,
is the scale factor for the distribution, and
is the location parameter for the distribution. If b is a large number, then a significant portion of the tails of the distribution are included. If
then all of the tails are included.
Start with the joint pdf for n independent, zero-mean (location parameters
) Student’s t pdfs with shape parameters
, and scale parameters
:
(10)
with
.
gives the probability that a random draw of the column matrix
from the joint Student’s t-distribution lies in the interval
. The pdf
is a function of only
and the shape parameter
, and thus is independent of any other
,
.
Use the transformation of Equation (2) to create a multivariate pdf
(11)
The solution
of the transformation Equation (2) was used. The elements of the inverse
matrix
,
, are given in terms of the
by Equation (8) for the
example. Note that the shape parameters
of the constituent distributions need not be the same in the multivariate t-distribution given by
.
gives the probability that a random draw of the column matrix
from the multivariate Student’s t-distribution with shape parameters
lies in the interval
.
From the definition of the exponential function
where
is Euler’s number, then
(12)
and
(13)
In the limit as
, the multivariate Student’s t-distribution
, Equation (11), becomes a multivariate normal distribution.
3.1. Some
for the
Example
In this subsection some examples for the variances and covariances of a multivariate Student’s t-distribution using the
example of Equation (2) are given.
The variance of the random variable
is
(14)
with the limits of the integrations equal to
and
,
.
Perform the integrations as listed. The integral over
is unity since only
depends on
(c.f. Equation (2)) and
factors into a product
―see Equation (10). Write
(15)
(16)
where the
are the elements of the inverse of matrix
and are as given by
, Equation (8), and
is a constant as far as the integral over
is concerned.
Repeat the procedure for the integrals for
,
, and
. These integrals are not equal to unity owing to the presence of the
term.
The variance of the random variable
for the multivariate Student's t-distribution with support
and with
for all i is given by
(17)
The expression for
is valid only for
. The expression would be valid for
if the region of support was
rather than
where
is a scale factor and
[3] - [5] . Note that the scale factors for the multivariate t-distribution are
.
Truncation or effective truncation of the pdf keeps the moments finite [3] - [5] . For example, the second central moment for a
Student’s t-distribution with scale factor
and support
is
(18)
which is finite provided that
.
In the interest of brevity, only variances and covariances that were calculated for support of
will be discussed. The requirement that
will be understood to be waived if the pdf is truncated or effectively truncated. It is also to be understood that the variances and covariances as calculated for support of
provide upper limits for variances and covariances calculated for truncation or effective truncation of the pdf.
If the
are not equal, then for the
example of Equation (2)
(19)
The covariance
for the
for all i is given by
(20)
If the
are not equal, then the covariance ![]()
(21)
The expression for
, which is valid for the
not equal, is
(22)
The expressions for
,
, and
show a simple pattern for the relationship between the covariance matrix
, the scale matrix
Equation (3), and the matrix
Equation (2).
3.2. General Expressions for ![]()
Given a matrix
that is an
square matrix with elements
, an expression for the variance (assuming support
,
for all i, and
) for the multivariate Student’s t-distribution
is
(23)
A general expression for the covariance (assuming support
,
for all i, and
) for the multivariate Student’s t-distribution
is
(24)
If support is
, then the general expressions need to be multiplied by functions that depend on b and
. Truncation or effective truncation keeps the moments finite and defined for all
[3] - [5] . The general expressions for the covariance, Equation (24), yields, when
, the general expression for the variance, Equation (23). The general expression for the variance, Equation (23), is given to emphasize the
nature of the variance.
Unlike normally distributed random variables, the correlation matrix
for random variables that are distributed as Student’s t is not equal to
. For normally distributed variables, the scale parameter
equals the standard deviation
. For Student’s t distributed variables, the standard deviation
does not equal the scale parameter
. For a Student’s t distribution with shape parameter
, scale parameter
, and support
,
. If the region of support for the Student’s t distribution is truncated to
then the variance
for all
and is finite for all
[3] - [5] .
Given a matrix of the variances and the covariances,
, and a column matrix of the shape parameters
associated with each variable, the scale matrix
would in principle be determined sequentially, starting with
and
. The shape parameters
would be obtained from the marginal distributions or from other knowledge.
4. Conclusion
A multivariate Student’s t-distribution is derived by analogy to the derivation for a multivariate normal (or Gaussian) pdf. The variances and covariances for the multivariate t-distribution are given. It is noteworthy that the shape parameters
of the constituent Student’s t-distributions of the multivariate t-distribution, Equation (11), need not be the same.
Acknowledgements
This work was funded by the Natural Science and Engineering Research Council (NSERC) Canada.
Appendix: The Jacobian
The Jacobian determinant is used in physics, mathematics, and statistics. Many of these uses can be traced to the Jacobian determinate as a measure of the volume of an infinitesimially small, n-dimensional parallelepiped.
1. Volume of a Parallelepiped
The volume of an n-dimensional parallelepiped is given by the absolute value of the determinant of the com- ponents of the edge vectors that form the parallelepiped.
The area of a parallelogram with edge vectors
and
is
.
The volume of a parallelepiped with edge vectors
,
, and
is given by the determinant
(25)
2. Inversion Exists
Assume that there are n functions
. The necessary and sufficient condition that the func- tions can be inverted to find
is that the Jacobian determinant is nonzero, i.e.,
(26)
where
(27)
To simplify the notation, assume that
so that
,
. The total differential is
(28)
These equations can be put in matrix form
(29)
These three equations can be solved for the
if the determinant of the
matrix is non-zero. This is a standard result from linear algebra. The determinant of the
matrix is called the Jacobian determinant of the transformation.
3. Change of Variables
The Jacobian determinant of the transformation is used in change of variables in integration:
(30)
The absolute value sign is required since the determinant could be negative (i.e., the volume could decrease).
The Jacobian determinant for the inverse transformation (to obtain
as functions of
) given by Eq- uation (8) is
(31)
which equals
(32)