Better than Rician: modelling millimetre wave channels as two-wave with diffuse power
Zöchmann et al. EURASIP Journal on Wireless Communications and
(2019) 2019:21
Networking
https://doi.org/10.1186/s13638-018-1336-6
RESEARCH
Open Access
Better than Rician: modelling millimetre
wave channels as two-wave with diffuse power
Erich Zöchmann1,2,3* , Sebastian Caban1,2 , Christoph F. Mecklenbräuker2 , Stefan Pratschner1,2 ,
Martin Lerch2 , Stefan Schwarz1,2 and Markus Rupp2
Abstract
This contribution provides experimental evidence for the two-wave with diffuse power (TWDP) fading model. We
have conducted two indoor millimetre wave measurement campaigns with directive horn antennas at both link ends.
One horn antenna is mounted in a corner of our laboratory, while the other is steerable and scans azimuth and
elevation. Our first measurement campaign is based on scalar network analysis with 7 GHz of bandwidth. Our second
measurement campaign obtains magnitude and phase information; it is additionally sampled directionally at several
positions in space. We apply Akaike’s information criterion to decide whether Rician fading sufficiently explains the
data or the generalised TWDP fading model is necessary. Our results indicate that the TWDP fading hypothesis is
favoured over Rician fading in situations where the steerable antenna is pointing towards reflecting objects or is
slightly misaligned at line-of-sight. We demonstrate TWDP fading in several different domains, namely, frequency,
space, and time.
Keywords: Millimetre wave, 60 GHz, Measurements, Fading, Hypothesis testing, Rician fading, TWDP fading
1 Introduction
Accurate modelling of wireless propagation effects is a
fundamental prerequisite for a proper communication
system design. After the introduction of the doubledirectional radio channel model [1], wireless propagation
research (< 6 GHz) started to model the wireless channel agnostic to the antennas used. More than a decade
later, propagation research focusses now on millimetre
wave bands to unlock the large bandwidths available in
this regime [2–5]. At millimetre waves (mmWaves), omnidirectional antennas have small effective antenna areas,
resulting in a high path loss [6–10]. To overcome this high
path loss, researchers have proposed to apply highly directive antennas on both link ends [11–14]. Most researchers
aim to achieve high directivity with antenna arrays
[15–20] and a few with dielectric lenses [21–23]. When
the link quality depends so much on the achieved beamforming gain, antennas must be considered as part of the
*Correspondence:
Christian Doppler Laboratory for Dependable Wireless Connectivity for the
Society in Motion, TU Wien, Gußhaustraße 25, 1040 Vienna, Austria
2
Institute of Telecommunications, TU Wien, Gußhaustraße 25, 1040 Vienna,
Austria
Full list of author information is available at the end of the article
1
wireless channel again. Small-scale fading is then influenced by the antenna.
According to Durgin [24, p. 137], “The use of directive
antennas or arrays at a receiver, for example, amplifies
several of the strongest multipath waves that arrive in
one particular direction while attenuating the remaining waves. This effectively increases the ratio of specular
to nonspecular received power, turning a Rayleigh or
Rician fading channel into a TWDP fading channel.” The
mentioned two-wave with diffuse power (TWDP) fading
channel describes this spatial filtering effect by two nonfluctuating receive signals together with many smaller
diffuse components.
1.1 Related work
The authors of [25] investigated a simple wall scattering scenario and analysed how fading scales with various
antenna directivities and different bandwidths. Increasing directivity [25], as well as increasing bandwidth
[25, 26], results in an increased Rician K-factor. The
authors of [27] analysed fading at 28 GHz with high gain
horn antennas on both link ends. They observe high
Rician K-factors even at non-line-of-sight (NLOS). This
effect is explained by spatial filtering of directive antennas,
© The Author(s). 2019 Open Access This article is distributed under the terms of the Creative Commons Attribution 4.0
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Zöchmann et al. EURASIP Journal on Wireless Communications and Networking
as they suppress many multipath components [25]. Outdoor measurements in [28, 29], show a graphical agreement with the Rice fit, but especially Fig. 10 in [29] might
be better explained as TWDP fading.
TWDP fading has already successfully been applied to
describe 60 GHz near body shadowing [30]. Furthermore,
as quoted above, TWDP must be considered for arrays, as
they act as spatial filters [24, 31]. While theoretical work
on TWDP fading is already advanced [32–37], experimental evidence, especially at millimetre waves, is still limited.
For enclosed structures, such as aircraft cabins and buses,
the applicability of the TWDP model is demonstrated
by Frolik [38–42]. A deterministic two ray behaviour in
ray tracing data of mmWave train-to-infrastructure communications is shown in [43]. A further extension of
the TWDP-fading model, the so-called fluctuating tworay fading model, was also successfully applied to fit
mmWave measurement data [44–46]. This model brings
in another degree of freedom and allows for common
shadowing of both specular waves. The wireless channels
in this present study are unblocked; thus, this model is not
considered here.
Our group has conducted two measurement campaigns
[47, 48] to directionally analyse receive power and smallscale fading parameters for mmWaves. This contribution
is based on the measurement data gathered in [47, 48].
1.2 Outline and contributions
With this contribution, we aim to bring scientific rigour
to the small-scale fading analysis of millimetre wave
indoor channels. We show in Section 2 —by means of
an information-theoretic approach [49] and null hypothesis testing [50]—that the TWDP model has evidence in
mmWave communications.
We have conducted two measurement campaigns
within the same laboratory with different channel sounding concepts. Our measurements are carried out in the
V-band; the applied centre frequency is 60 GHz. For both
measurement campaigns, 20 dBi horn antennas are used
at the transmitter and at the receiver. The first measurement campaign (MC1) samples the channel in azimuth
(ϕ) and elevation (θ), keeping the antenna’s (apparent)
phase centre ([51, pp. 799] ) at a fixed (x, y) coordinate.
The transmitter is mounted in a corner of our laboratory. The sounded environment as well as the mechanical
set-ups are explained in Section 3. For MC1, we sounded
the channel in the frequency domain by aid of scalar
network analysis, described in Section 4. These channel
measurements span over 7 GHz bandwidth, supporting (...truncated)