Digital Signal Processing Reference
In-Depth Information
the oscillator in the receiver has a phase offset of
θ
with respect to the trans-
mitter; when we retrieve the baseband signal b
[
n
]
from
c
ˆ
[
n
]
we have
b
e −j ( ω c n− θ ) =
e −j ( ω c n− θ ) =
e j θ
[
n
]=ˆ
c
[
n
]
c
[
n
]
b
[
n
]
l g r , y i d . , © , L s
where we have neglected both distortion and noise and assumed c [ n ]=
c
. Such a phase offset translates to a rotation of the constellation points
in the complex plane since, after downsampling, we have a [ n ]= a [ n ] e j θ .
Visually, the received constellation looks like in Figure 12.22, where
[
n
]
θ =
π/
9 . If we look at the decision regions plotted in Figure 12.22, it is clear
that in the rotated constellation some points are shifted closer to the deci-
sion boundaries; for these, a smaller amount of noise is sufficient to cause
slicing errors. An even worse situation happens when the receiver's carrier
frequency is slightly different than the transmitter's carrier frequency; in this
case the phase offset changes over time and the points in the constellation
start to rotate with an angular speed equal to the difference between fre-
quencies. In both cases, data transmission becomes highly unreliable: car-
rier recovery is then a fundamental part of modem design.
20
=
Im
·
·
·
·
·
·
·
·
Re
·
·
·
·
·
·
·
·
Figure 12.22 Rational effect of a phase offset on the received symbols.
The most common technique for QAM carrier recovery over well-
behaved channels is a decision directed loop ;justasinthecaseoftheadap-
tive equalizer, this works when the overall SNR is sufficiently high and the
distortion is mild so that the slicer's output is an almost error-free sequence
of symbols. Consider a system with a phase offset of
θ
; in Figure 12.23 the
 
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