LOS and NLOS Channel Modeling for Terahertz
Wireless Communication with Scattered Rays
Anamaria Moldovan
1
, Michael A. Ruder
1
, Ian F. Akyildiz
2
, and Wolfgang H. Gerstacker
1
1
Institute for Digital Communications, Friedrich-Alexander-University Erlangen-Nürnberg (FAU),
Cauerstr. 7, D-91058 Erlangen, Germany, {moldovan, ruder, gersta}@LNT.de
2
Broadband Wireless Networking Lab, Georgia Institute of Technology, Atlanta, USA, ian.akyildiz@ee.gatech.edu
Abstract—In this paper, the wireless communication over
indoor Terahertz (THz) channels is studied. The physical mech-
anisms governing a wireless transmission in the 0.1 – 10 THz
band are a very high molecular absorption and spreading loss
which result in a very high and frequency-selective path loss for
the line-of-sight (LOS) links. For the non-line-of-sight (NLOS)
propagation, a very high reflection loss depending on the shape,
material, and roughness of the reflecting surface affects the THz
wave propagation. Taking these peculiarities of the THz radiation
into account and applying a ray tracing approach for scattered
rays, a novel deterministic equivalent channel model is developed
that accounts for both the LOS and NLOS propagation cases.
Furthermore, the channel capacity of the proposed model is
investigated. Simulation results demonstrate that for distances,
up to 1 m, data rates in the order of Terabit per second (Tbps)
are obtained for a transmit power of 1 Watt. Moreover, the
capacity of only the NLOS component is around 100 Gigabit per
second (Gbps). These results are highly motivating to develop
future wireless THz communication systems.
I. I NTRODUCTION
To satisfy the growing demands for high data rates in
wireless communication systems, the network capacity has been
enhanced by increasing the spectral efficiency by means of
advanced modulation schemes and signal processing techniques
[1]. However, the efficiency of these methods is limited due to
the narrow bandwidth of legacy systems. Another approach for
throughput enhancement is increasing the operation frequency.
In this respect significant effort is devoted to research in the
field of millimeter-waves, which allow for data rates up to
10 Gigabit per second (Gbps) [2]. Yet, the increasing demand
for even higher data rates in wireless communications will
eventually lead to the allocation of wider bandwidths in the
Terahertz (THz) frequency range. For this purpose, the IEEE
802.15 Terahertz Interest Group (IGthz) has been established
in 2008 to explore the feasibility of the Terahertz band for
wireless communications [3]. Since January 2014 there is an
official IEEE standardization committee called 100Gbps.
The THz band, or so-called sub-millimeter band, covers
the frequency range between 100 GHz and 10 THz, with
corresponding wavelengths between 3 mm and 30 μm. In
contrast to X-ray radiation, THz radiation is non-ionizing and
therefore it can be used in close proximity to the human
body. Other important advantages of THz radiation include the
penetration of many opaque materials and the high selectivity
due to the fact that many molecules have resonance frequencies
within the THz band, enabling their detection when they are
present.
Many applications of THz waves, some of them already
available, like THz body scanners at airports or medical
imaging, are based on these properties. So far, THz waves have
not been utilized for wireless communications because of the
lack of devices for generating and detecting them [1]. Currently,
though there are three major technologies such as Silicon-
Germanium (SiGe), Galium-Nitride (GaN), and Graphene that
are being considered for the development of ultra-high-speed
transceivers in the THz band [4].
The physical mechanisms governing a wireless transmission
in the THz band are different from those which affect schemes
operating in the lower frequency bands where the propagation
is mainly influenced by the spreading loss. Therefore, already
existing channel models cannot be re-used for THz commu-
nications. The peculiarities of THz radiation are a very high
molecular absorption and spreading loss which result in a very
high and frequency-selective path loss for line-of-sight (LOS)
links. For non-line-of-sight (NLOS) propagation, a very high
reflection loss depending on the shape, material, and roughness
of the reflecting surface governs the THz wave propagation.
So far, the existing literature on the channel modeling in
the THz band is sparse. In [5], an LOS propagation model
for the entire THz band was developed by analyzing the
impact of molecular absorption on the path loss. To account
for the NLOS propagation, it is necessary to characterize the
reflection of electromagnetic (EM) waves at obstacles in the
THz frequency range. The properties of typical indoor materials
have been measured in the 0.1 to 1 THz frequency range [6],
[7]. Furthermore, the scattering behavior of rough surfaces
both in the specular [8] and non-specular [9], [10] directions
has been analyzed at 300 GHz band. To this end, these works
employ Kirchhoff scattering from rough surfaces theory [11].
The few existing channel models in the THz band [12], [13]
characterize the multipath channel at 0.3 THz based on ray-
tracing simulations. They are mainly based on measurements
and consider specular reflections only.
In this paper, we propose a novel deterministic channel
model for the 0.1 to 1 THz frequency range, based on Kirchhoff
scattering theory and ray tracing that includes the effects of
LOS and NLOS propagation. We improve the LOS propagation
model proposed in [5] by adopting an updated molecular High
Resolution Transmission (HITRAN) 2012 database and realistic
values for the fraction of water vapor in the air. Our improved
LOS propagation model in Section II shows a significantly
lower molecular absorption loss as compared to [4]. For the
NLOS propagation, in Section III we model the reflection
loss as discussed in [10], including also the effects of the
molecular absorption loss and spreading loss on the indirect
paths. Furthermore, the channel capacity is determined in
Section V by employing the proposed deterministic channel
model for LOS and NLOS propagation from Section IV and
optimizing the transmit power allocation via water-filling. Our
simulation results show that for relatively short distances, up
to 1 m, data rates in the order of Terabit per second (Tbps)
can be obtained for a transmit power of 1 Watt. This result
encourages the use of the THz band for wireless short range
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