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at instant i , on all of the transitions between instants i
1 and i for which the
j -th bit making up the symbol associated with these transitions equals 0 or 1.
Thus,
Pr( s ,s, y )
( s ,s ) /x i,j =1
L ( x i,j )=ln
(11.7)
Pr( s ,s, y )
( s ,s ) /x i,j =0
Adopting a similar approach now to the one presented in the original article
by Bahl et al . [11.3], we can show that the joint probability Pr( s ,s, y ) associated
with each transition considered can be decomposed into a product of 3 terms:
Pr( s ,s, y )= α i− 1 ( s ) γ i− 1 ( s ,s ) β i ( s )
(11.8)
Figure 11.12 shows the conventions of notation used here.
Figure 11.12 - Conventions of notation used to describe the MAP equalizer.
Forward and backward state probabilities α i− 1 ( s ) and β i ( s ) can be calcu-
lated recursively for each state and at each instant in the trellis, by applying the
following update equations:
α i ( s )=
( s ,s )
α i− 1 ( s ) γ i− 1 ( s ,s )
(11.9)
β i ( s )=
( s ,s )
γ i ( s ,s ) β i +1 ( s )
(11.10)
These two steps are called forward recursion and backward recursion , respec-
tively. Summations are performed over all the couples of states with indices ( s ,
s ) for which there is a valid transition between two consecutive instants in the
trellis. Forward recursion uses the following initial condition:
α 0 (0) = 1 ,
α 0 ( s )=1 for s
=0
(11.11)
This condition translates the fact that the initial state in the trellis (with
index 0 , by convention) is perfectly known. Concerning the backward recursion,
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