Digital Signal Processing Reference
In-Depth Information
Q
1
j
ω
n
hnl
()
;=
h le
()
,=, +,,+−,
n
1
T
1
(2.15)
q
nn
n
q
kk
k
B
q
=
where one chooses ( l = 0, 1, , L , and K is an integer)
T TK
B
:= , ≥1
(2.16)
Qf T ds
2
+ ,
1
(2.17)
2
π
( )
, =,, ,,
ω
:=
qQ
12
q
12
Q
(2.18)
q
T
L
:=
τ /
ds
.
(2.19)
The BEM coefficients h q ( l ) remain invariant during this block, but are allowed to
change at the next block, and the Fourier basis functions { e j ω q n } ( q = 1, 2, , Q ) are com-
mon for each block. If the delay spread τ d and the Doppler spread f d of the channel (or at
least their upper bounds) are known, one can infer the basis functions of the CE-BEM
[36]. Treating the basis functions as known, estimation of a time-varying process is
reduced to estimating the invariant coefficients over a block of length T B symbols. Note
that the BEM period is T = KT B , whereas the block size is T B symbols. If K > 1 (e.g., K = 2
or K = 3), then the Doppler spectrum is said to be oversampled [32] compared to the case
K = 1, where the Doppler spectrum is said to be critically sampled. In [13, 36] only K = 1
(henceforth called CE-BEM) is considered, whereas [32] considers K ≥ 2 (henceforth
called oversampled CE-BEM).
CE-BEM has a finite impulse response (FIR) structure in both time and frequency
domains [46]. This unique time-frequency duality makes it a widely used model depict-
ing the temporal variations of wireless channels. For K = 1, the rectangular window
of this truncated discrete Fourier transform (DFT)-based model introduces spectral
leakage [43]. The energy at each individual frequency leaks to the full-frequency range,
resulting in significant amplitude and phase distortion at the beginning and the end of
the observation window [61]. To mitigate this leakage, the oversampled CE-BEM with
K = 2 or 3 has been considered in [32].
Equation (2.15) applies to single-input single-output systems—one user and one
receiver with symbol-rate sampling. It is easily modified to handle multiuser, multiple-
transmit and -receive antennas, and higher-than-symbol-rate sampling—the basic rep-
resentation remains essentially unchanged.
The representation h ( n ; l ) in (2.15) is a special case of a more general representation:
Q
1
hnl
()
;=
=
h l
() ()
φ ,
n
(2.20)
q
q
q
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