
230 SPACE–TIME CODES
the DoD of a waveform leaving the transmitting antenna array. Obviously, both angles
depend on the orientation of the antenna arrays at transmitter and receiver as well as on the
location of the scatterers. For the purpose of this book it is sufficient to presuppose a one-
to-one correspondence between θ
R
and θ
T
. In this case, the DoD is a function of the DoA
and the channel impulse response has to be parameterised by only one additional param-
eter, the azimuth angle θ
R
. Hence, the generally time-varying channel impulse response
h(t, τ ) known from Chapter 1 is extended by a third parameter, the direction of arrival θ
R
.
1
Therefore, the augmented channel impulse response h(t,τ,θ
R
) bears information about the
angular power distribution.
Principally, Line of Sight (LoS) and non-line of sight (NLoS) scenarios are distin-
guished. In Figure 5.12, an LoS path with azimuth angles θ
T,LoS
and θ
R,LoS
exists. Those
paths are mainly modelled by a Ricean fading process and occur for rural outdoor areas.
NLoS scenarios typically occur in indoor environments and urban areas with rich scatter-
ing, and the corresponding channel coefficients are generally modelled as Rayleigh fading
processes.
Statistical Characterisation
As the spatial channel represents a stochastic process, we can follow the derivation in
Chapter 1 and describe it by statistical means. According to Figure 5.13, we start with the
autocorrelation function φ
HH
(t,τ,θ
R
) of h(t,τ,θ
R
) which depends on three parameters,
the temporal shift t, the delay τ and the DoA θ
R
. Performing a Fourier transformation with
respect to t delivers the three-dimensional Doppler delay-angle scattering function defined
in Equation (5.24) (Paulraj et al., 2003). It describes the power distribution with respect
to its three parameters. If
HH
(f
d
,τ,θ
R
) is narrow, the angular spread is small, while a
broad function with significant contributions over the whole range −π<θ
R
≤ π indicates
a rather diffuse scattering environment. Hence, we can distinguish between space-selective
and non-selective environments.
Similarly to scalar channels, integrations over undesired variables deliver marginal
spectra. As an example, the delay-angle scattering function is shown in Equation (5.25).
Similarly, we obtain the power Doppler spectrum
HH
(f
d
) =
π
-
−π
∞
-
0
HH
(f
d
,τ,θ
R
)dτ dθ
R
,
the power delay profile
HH
(τ ) =
π
-
−π
HH
(τ, θ
R
)dθ
R
or the power azimuth spectrum
HH
(θ) =
∞
-
0
HH
(τ, θ) dτ .
1
In order to simplify notation, we will use in this subsection a channel representation assuming that all
parameters are continuously distributed.