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Expanding for the densities and substituting the variational moments results in
E W,τ,α (ln p ( W , τ
|
α ))
D X D Y
2
=
k
ψ
ln 2 π
( a α k )
ln b α k +
( a τ k )
ln b τ k
ψ
a α k
b α k
a τ k
b τ k
1
2
w kj T w kj + D Y Tr( Λ k 1 )
(7.78)
j
.
a τ k
b τ k
( a τ k )
ln b τ k )
+ D Y
ln Γ( a τ )+ a τ ln b τ +( a τ
1)(
ψ
b τ
The negative entropy
E W,τ (ln q ( W , τ )) of
{
W , τ
}
isbasedon(7.29)and
results in
E W,τ (ln q ( W , τ ))
k
w kj , ( τ k Λ k ) 1 )Gam( τ k |
a τ k ,b τ k )
=
E W,τ
ln
N
( w kj |
j
D 2
=
k
D 2
ln 2 π + 1
Λ k |
E τ (ln τ k )
2 ln
|
j
E W,τ
w kj )
τ
2 ( w kj
w kj ) 2 Λ k ( w kj
ln Γ( a τ k )
+
b τ k E τ ( τ k )
+ a τ k ln b τ k +( a τ k
1)
E τ (ln τ k )
a τ k
(
= D Y
k
1+ D 2
D 2
( a τ k )
ln b τ k )
ψ
(ln 2 π +1)
,
+ 1
Λ k |−
ln Γ( a τ k )+ a τ k ln b τ k
a τ k
2 ln
|
(7.79)
where the previously evaluated variational moments and
E W,τ
w kj ) =
τ
2 ( w kj
1
2 D X
w kj ) 2 Λ k ( w kj
(7.80)
was used.
We derive the expression
E α (ln q ( α )) in combination, as that
allows for some simplification. Starting with
E α (ln p ( α ))
E α (ln p ( α )), we get from (7.17) and
(7.9), by expanding the densities and substituting the variational moments,
E α (ln p ( α ))
(7.81)
.
=
k
b α a α k
b α k
( a α k )
ln b α k )
ln Γ( a α )+ a α ln b α +( a α
1)(
ψ
 
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