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way as Waterhouse et al. [227, 226] by performing a Laplace approximation of
the posterior.
The Laplace approximation aims at finding a Gaussian approximation to the
posterior density, by centring the Gaussian on the mode of the density and
deriving its covariance by a second-order Taylor expansion of the posterior [19].
The mode of the posterior is found by solving
ln q V ( V )
V
=0 ,
(7.46)
which, by using the posterior (7.45) and the definition of g k (7.10), results in
( r nk
g k ( x n )) φ ( x )
E β ( β k ) v k =0 ,
k =1 ,...,K.
(7.47)
n
Note that, besides the addition of the
E β ( β k ) v k term due to the shrinkage prior
on v k , the minimum we seek is equivalent to the one of the prior-less generalised
softmax function, given by (6.11). Therefore, we can find this minimum by ap-
plying the IRLS algorithm (6.5) with error function E ( V )=
ln q V ( V ), where
the required gradient vector and the D V ×
D V blocks H kj of the Hessian matrix
(6.9) are given by
v 1 E ( V )
.
v j E ( V )=
n
V E ( V )=
,
( g j ( x n )
r nj ) φ ( x n )+
E β ( β j ) v j ,
v K E ( V )
(7.48)
and
H kj = H jk =
n
g j ( x n )) φ ( x n ) φ ( x n ) T + I kj E β ( β k ) I .
g k ( x n )( I kj
(7.49)
I kj is the kj th element of the identity matrix, and the second I in the above
expression is an identity matrix of size D V
D V . As the resulting Hessian is
positive definite [173], the posterior density is concave and has a unique maxi-
mum. More details on how to implement the IRLS algorithm are given in the
next chapter.
Let V with components v k denote the parameters that maximise (7.45).
V gives the mode of the posterior density, and thus the mean vector of its
Gaussian approximation. As the logarithm of a Gaussian distribution is a qua-
dratic function of the variables, this quadratic form can be recovered by a
second-order Taylor expansion of ln q V ( V ) [19], which results in the precision
matrix
×
Λ V
ln q V ( V )=
E ( V )= H
=
−∇∇
∇∇
| V = V ,
(7.50)
 
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