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To simplify the computation of the variational bound, we define
L k ( q )=
E W,τ,Z (ln p ( Y
|
W k k , z k )) +
E W,τ,α (ln p ( W k k |
α k ))
+
E α (ln p ( α k ))
E W,τ (ln q ( W k k ))
E α (ln q ( α k )) ,
(7.88)
which can be evaluated separately for each classifier by observing that all ex-
pectations except for
E V (ln q ( V )) are sums whose components can be evaluated
independently for each classifier. Furthermore,
L k ( q ) can be simplified by using
the relations
D X D Y
2
= a α k
a α ,
(7.89)
a τ k
b τ k
1
2
w kj T w kj + D Y Tr( Λ k 1 )
= b α k
b α ,
(7.90)
j
which results from (7.40) and (7.41). Thus, the final, simplified expression for
L k ( q ) becomes
L k ( q )= D 2
ln 2 π
n
ψ
r nk + D X D Y
2
( a τ k )
ln b τ k
r nk a τ k
2 + D Y x n Λ k 1 x n
2
n
1
W k x n
b τ k
y n
a α k ln b α k + D 2
Λ k 1
ln Γ( a α )+ a α ln b α +lnΓ( a α k )
ln
|
|
b τ a τ k
b τ k
a τ k )
( a τ k )
a τ ln b τ k
+ D Y
ln Γ( a τ )+ a τ ln b τ +( a τ
ψ
+lnΓ( a τ k )+ a τ k .
(7.91)
All leftover terms from (7.75) are assigned to the mixing model, which results
in
L M ( q )=
E Z,V (ln p ( Z
|
V )) +
E V,β (ln p ( V
|
β )) +
E β (ln p ( β ))
E Z (ln q ( Z ))
E V (ln q ( V ))
E β (ln q ( β )) .
(7.92)
We can again derive a simplified expression for
L M ( q ) by using the relations
D V
2
= a β k
a β ,
(7.93)
Tr ( Λ V 1 ) kk + v k T v k = b β k
1
2
b β ,
(7.94)
which result from (7.56) and (7.57). Overall, this leads to the final simplified
expression
L M ( q )=
k
a β k ln b β k
ln Γ( a β )+ a β ln b β +lnΓ( a β k )
(7.95)
+
n
r nk ln g k ( x n )
ln r nk + 1
+ KD V
2
Λ V 1
| v k = v k
2 ln
|
|
.
k
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