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The expression for
E α (ln q ( α )) can be derived by observing that
E α (ln q ( α k ))
is the entropy of q α ( α k ). Thus, using q α ( α )= k q α ( α k ), substituting (7.39) for
q α ( α k ), and applying the entropy of the Gamma distribution [19], we get
ln Γ( a α k )
ln b α k + a α k
( a α k
( a α k )
E α (ln q ( α )) =
1)
ψ
(7.82)
k
Combining the above expressions and removing the terms that cancel out results
in
E α (ln q ( α )) =
k
a α k )
( a α k )
E α (ln p ( α ))
ln Γ( a α )+ a α ln b α +( a α
ψ
+lnΓ( a α k )+ a α k . (7.83)
b α a α k
b α k
a α ln b α k
E Z (ln q ( Z )) is also derived in combination
by using (7.12), (7.11) and (7.63), from which we get
The expression
E Z,V (ln p ( Z
|
V ))
E Z (ln q ( Z )) =
n
r nk ln g k ( x )
| v k = v k
r nk
E Z,V (ln p ( Z
|
V ))
,
(7.84)
k
where we have, as previously, approximated
E V (ln g k ( x n )) by ln g k ( x n )
| v k = v k .
β )) is again based on simple expansion
of the distribution given by (7.18) and (7.13), and substituting the variational
moments, which results in
The derivation to get
E V,β (ln p ( V
|
E V,β (ln p ( V
|
β ))
(7.85)
D V
2
v k T v k +Tr(( Λ V 1 ) kk ) .
=
k
a β k
b β k
ψ
ln 2 π
1
2
( a β k )
ln b β k
E V (ln q ( V )) by observing that it is the negative entropy of the Gaus-
sian (7.51), and thus evaluates to [19]
We get
1
2 ln
(1 + ln 2 π ) .
+ KD V
2
Λ V 1
E V (ln q ( V )) =
|
|
(7.86)
As the priors on β k are of the same distribution form as the ones on α k ,the
expectations of their log-density results in a similar expression as (7.65) and is
given by
E β (ln q ( β )) =
k
a β k )
( a β k )
E β (ln p ( β ))
ln Γ( a β )+ a β ln b β +( a β
ψ
+lnΓ( a β k )+ a β k . (7.87)
a β k
b β k
a β ln b β k
b β
This completes the evaluation of the expectations required to compute the
variational bound (7.75).
 
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