3 The exponential family

3.3 Examples of linear EF distributions

The following are well known examples of EF distributions familiar in classical statistics.

 
Exercise 3.19
Find the mgf of the Poisson distribution

q(y)=exp{-1}/y!fory=0,1,2,,

and determine when it is finite.

 

 
Exercise 3.20
Show that the Poisson distribution is in the linear exponential family generated from

q(y)=exp{-1}/y!fory=0,1,2,.

 

To check this is the Poisson pmf transform to the parameter μ by

log(μ)=θ,soμ=exp{θ}.

Substituting gives the more usual formulation:

f(y|μ)=exp{-μ}μy/y!,fory=0,1,2,,μ>0,

in which μ is the mean. Note that the relation logμ=θ between the canonical parameter and the mean parameter is invertible.

 
Exercise 3.21
Show that the Bernoulli density function

f(y|p)=py(1-p)1-y,fory=0,1,

can be derived by exponential tilting q(y)=1/2 for y=0,1.

 

To ascertain the relationship between the mean parameter p=𝔼[Y] and the canonical parameter θ consider (Y=1). As f(1|p)=p and f(1|θ)=exp{θ}1+exp{θ}, both equal (Y=1) it follows

p=exp{θ}1+exp{θ},

the logistic function. The inverse of this function is the logit function

logit(p)=log(p1-p)=θ,

so that the canonical parameter is the familiar log odds.

 
Exercise 3.22
Find the mgf of the normal pdf with an arbitrary mean.

 

The cumulant generating function is

κ(θ) = log(exp{θ2/2})=12θ2,

and Θ is the whole real line.

 
Exercise 3.23
Show that the normal density function with an arbitrary mean can be derived by exponentially tilting q for which YN(0,1).

 

This can be expressed in the more usual form

f(y|θ)=12πexp{-12(y-θ)2}.

We conclude that YN(θ,1) is EF generated by q=N(0,1) and tilted with Y. As μ=𝔼[Y]=θ, the mean parameter of Y under f is identical to the canonical parameter.

 
Exercise 3.24
Show that the exponential pdf

f(y|λ)=λexp{-λy},fory>0andλ>0,

is a member of the exponential family.

 

Alternatively starting with q(y)=2exp{-2y}, we may generate a family with canonical parameter θ and λ=2-θ.

This example of the exponential density indicates that some values of θ do not lead to a finite moment generating function, i.e. when θ>1, and that Θ may not be the full real line. Some pdfs/pmfs have no finite moments, such as the Cauchy density function

q(y)=1π(1+y2)for-<y<.

whose mgf Mq(θ)=exp{θy}q(y)𝑑y is infinite except for the only permissible value θ=0 with Mq(θ)=1.