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pf X|1
qf X|−1
qf X|−1
pf X|1
x 0
x 0
x 0
δ
x 0
δ
(a)
(b)
Fig. 4.1 The two intersection cases of qf X|− 1 and pf X| 1 . The light shadowed areas
correspond to P e ( x 0 ) . The dark shadowed area is the amount of error probability
added to P e ( x 0 ) when the split point moves to x 0 − δ . The dashed area is the
amount of error probability subtracted from P e ( x 0 ) when the split point moves to
x 0 − δ .
P e ( x )= x
−∞
pf X| 1 dx + +
x
qf X|− 1 dx.
(4.8)
If there is no intersection of qf X|− 1 with pf X| 1 ,thenmin P e =min( p, q )
1 / 2
occurs at +
.
For intersecting posterior densities, one has to distinguish two cases. First,
assume that for δ> 0
or
−∞
pf X| 1 ( x ) <qf X|− 1 ( x )
x
[ x 0
δ, x 0 ]
(4.9)
pf X| 1 ( x ) >qf X|− 1 ( x )
x
[ x 0 ,x 0 + δ ] ,
(4.10)
where x 0 is an intersection point of qf X|− 1 with pf X| 1 as illustrated in
Fig. 4.1a.
The probabilities of error at x 0 and x 0
δ are
P e ( x 0 )= p x 0 −δ
−∞
f X| 1 ( x ) dx + q +
x 0
f X| 1 ( x ) dx + x 0
x 0 −δ
f X|− 1 ( x ) dx,
(4.11)
P e ( x 0 − δ )= p x 0 −δ
−∞
f X| 1 ( x ) dx +
+ q x 0
x 0 −δ
f X|− 1 ( x ) dx + +
x 0
f X|− 1 ( x ) dx .
(4.12)
Hence,
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