# Channel sounding and indoor radio channel characteristics in the W-band

Maria-Teresa Martinez-Ingles, Davy Gaillot, Juan Pascual-Garcia, Jose-Maria Molina-Garcia-Pardo, Jose-Victor Rodriguez, Lorenzo Rubio, Leandro Juan-Llacer

► To cite this version:

Maria-Teresa Martinez-Ingles, Davy Gaillot, Juan Pascual-Garcia, Jose-Maria Molina-Garcia-Pardo, Jose-Victor Rodriguez, et al.. Channel sounding and indoor radio channel characteristics in the W-band. EURASIP Journal on Wireless Communications and Networking, 2016, 2016, pp.30,. 10.1186/s13638-016-0530-7 . hal-03346227

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# Channel sounding and indoor radio channel characteristics in the W-band

Maria-Teresa Martinez-Ingles⁴, Davy P. Gaillot², Juan Pascual-García<fnref n="1" />, Jose-Maria Molina-Garcia-Pardo<fnref n="1" />*, José-Víctor Rodríguez<fnref n="1" />, Lorenzo Rubio³ and Leandro Juan-Llácer<fnref n="1" />

## Abstract

This work presents directional radio channel measurements in the W-band using a commercial versatile channel sounder based on a vector network analyzer (VNA), capable of measuring scattering parameters from 75 to 500 GHz with frequency converters. The commercial setup has been modified by increasing the distance for one of the converters using precision coaxial cables and avoiding the use of amplifiers. Firstly, initial distance-dependent single-input single-output (SISO) measurements of indoor radio channels are presented to assess the validity of the setup in the 75–110 GHz frequency band with highly directive horn antennas. Then, single-input multiple-output (SIMO) radio channels were measured at 94 GHz using one directional and one omnidirectional antenna mounted on two positioners. Initial channel characterization is presented comprising root mean square (rms) delay spread, rms angular spread, K-factor, and path loss in an indoor environment at 94 GHz.

## 1 Introduction

The UE Horizon 2020 considers the extension of wire-less communication systems to frequencies above 60 GHz as one of its priorities (http://ec.europa.eu/programmes/horizon2020/); specifically, it aims to fill the gap between the millimeter and the terahertz spectrum. This frequency range between 60 and 300 GHz is not limited to communications but also finds application in remote sensing, security, and industrial measurement. The use of this band has been proposed for high-speed data links, automotive radar, radar imaging, security screening, substance identification, and non-destructive testing among others [1–3].

In terms of the W-band (75–110 GHz), most of the studies found in the literature date from the 1990s, and all of them are narrowband. In [4], propagation in the evaporation duct at 94 GHz is studied, in [5] a computational study at 94 and 140 GHz for oblate spheroidal and spherical raindrops is performed, and in [6], some propagation studies with rain are performed at 94 GHz. The first indoor propagation (narrowband path loss) measurements at 94 GHz are found in [7] and wideband in [8]. In [9], wideband measurements over the

full W-band are performed but limited to short distances. In addition, body area networks (BANs) have shown interest in these frequencies [10]. Therefore, as far as the authors are concerned, there is little analysis on indoor wideband measurements in the W-band.

In this work, a commercial channel sounder setup designed for sounding a radio propagation channel beyond 67 GHz, which is the limit of coaxial wired typical vector network analyzer (VNA) (few models reach 100 GHz), to up to 500 GHz is described. A link budget of the coaxial cables connection to the converter is presented, which enable wireless measurements from 50 to 500 GHz (depending on the converter model). In this work, we focus on the W-band frequency range.

First, single-input single-output (SISO) in the 75–110 GHz are presented by using two horn antennas used for the SISO measurements in order to validate the developed measurement setup. Later, directional measurements within 3 GHz around 94 GHz are presented in an indoor environment. However, channel sounding for radio characterization is typically performed with omnidirectional antennas. At these frequencies, the required dynamic range is higher than at lower bands, i.e., a path loss of 72.4 dB is theoretically obtained at 1 m for 100 GHz. To alleviate this issue, one omnidirectional

<figure><img src="image_4.png" /></figure>

<footnote>* Correspondence: josemaria.molina@upct.es</footnote>

<footnote n="1">¹Departamento Tecnologías de la Información y las Comunicaciones, Universidad Politécnica de Cartagena, Cartagena, Spain</footnote>

<footnote>Full list of author information is available at the end of the article</footnote>
antenna is used at one side whereas a rotary system with a high directivity horn antenna is used at the other side to construct an omni-like radiation pattern with a higher dynamic range. This approach was used with 70 GHz in [11]. Preliminary results such as root mean square (rms) delay spread, rms angular spread, path loss, and K-factor are presented and discussed.

This paper is organized as follows: Section II focuses on the description of the channel sounder based on a commercial VNA, Section III presents wideband measurements in the W-band using horn antennas to assess the validity of the setup, Section IV focuses on the channel characteristics at the 94 GHz frequency for an indoor environment, and Section V concludes the work.

## 2 Channel sounder

The millimeter-wave channel sounder setup is described in Fig. 1. It is based on a commercial vector network analyzer (VNA), the R&S ZVA 67, and up-converters (http://www.rohde-schwarz.es/product/ZVAZ.html). In this work, the R&S®ZVA-Z110E converter (W-band WR-10, 75 to 110 GHz) was used for both the transmitting and receiving unit. The commercial setup is limited to the separation of the converters up to 1 m. In order to communicate between the converter and the VNA, four signals come out from the VNA to each converter, and they are used to measure different mmW frequency bands (note that each converter slightly differs in these frequencies):

1. Source input (RF, magenta): 12.5 to 18.33 GHz. Input power in the converter: 4 to 10 dBm.

2. Local oscillator input (LO, blue) IN: 9.34 to 13.715 GHz. Input power in the converter: 5 to 10 dBm.

3. Measurement output (MEAS, orange): 10 to 300 MHz.

4. Reference output (REF, green): 10 to 300 MHz.

The output power of the VNA is typically greater than 15 dBm such that a 10 dB margin was used for the cables or amplifiers to separate the converter from the VNA (magenta, blue, green, and orange in Fig. 1). This point is the extension from the application note from the manufacturer.

In order to take measurements in this frequency band, it was decided not to use amplifiers in order to simplify the setup and because the dynamic range was enough for the distances considered in the study. Two RG-58 cables with SMA connector were used for REF and MEAS, and two 8-m TRUCore300 cables were used for RF and LO. These cables had an insertion loss of 7.8 dB at 18 GHz. Figure 2 presents the VNA setup for using the converters.

The system was THROUGH calibrated (Fig. 3), being included the delay and gain of the antennas in the measurements. The measured dynamic range for an intermediate frequency (IF) of 100 Hz was 97 dB. The channel transfer functions were thus measured by the $S_{21}$—scattering parameter in the frequency domain.

<figure><img src="image_5.png" /><figcaption>Fig. 1 Millimeter-wave channel sounder setup</figcaption></figure>
<figure><img src="image_6.png" /><figcaption>**Fig. 2** Photo of cables connected to the VNA</figcaption></figure>

## 3 Channel sounder validation, 75–110 GHz SISO measurements

In this section, we will validate the use of the channel sounder with SISO measurements. Two horn antennas manufactured by Flann Microwave (Model 27240–20 (http://www.flann.com/)) were connected to the channel sounder described in Section II. The antennas operate in the 73.8–112 GHz range with gain values varying between 18 and 21.5 dBi, as shown in Fig. 4. The VNA was configured to measure the $S_{21}$-scattering parameter from 75 to 110 GHz, i.e., 35 GHz of SPAN and a central

frequency equal to 92.5 GHz, with $N_f = 2048$ frequency points and 50 times averaged. A picture of the setup can be seen in Fig. 5.

For these first measurements, near line-of-sight (LOS) channel realizations were measured for distance values ranging between 10 and 70 cm. Figure 6 shows the measured wideband path loss (PL) at each position taking into account the frequency gain of the antennas and the frequency characteristics of free-space propagation. The PL has been calculated as an extension of the Friis formula for the case of ultra wideband as described in [12]. Thus, the PL is derived as the ratio

<figure><img src="image_7.png" /><figcaption>**Fig. 3** Calibration process</figcaption></figure>
<figure><img src="image_8.png" /><figcaption>Fig. 4 Horn antenna specifications in the W-band</figcaption></figure>

between the transmit energy and the energy of the received signal over the 35 GHz bandwidth. It is assumed that there are no polarization losses between the antennas being both vertical polarized. The PL can be derived from the antenna gain (g(f)), and S21(f) the scattering parameter as:

$$PL(\text{dB}) = -10 \log_{10} \left( \int_{f_{\min}}^{f_{\max}} \frac{1}{g^2(f)} |S_{21}(f)|^2 df \right) \quad (1)$$

where $f_{min}$ and $f_{max}$ are 75 and 110 GHz, respectively. In discrete form, (1) can be rewritten as

<figure><img src="image_9.png" /><figcaption>Fig. 6 Measured and the upper bound path loss in the W-band</figcaption></figure>

$$PL(\text{dB}) = -10 \log_{10} \left( \frac{1}{N_f} \sum_{n=0}^{N_f-1} \frac{|S_{21}(f_{\min} + n\Delta f)|^2}{g^2(f_{\min} + n\Delta f)} \right) \quad (2)$$

where the frequency resolution used in the measurements is given by:

$$\Delta f = \frac{f_{\max} - f_{\min}}{N_f - 1}. \quad (3)$$

As a comparison, we have also plotted in Fig. 6 the upper bound of the path loss, PLUB, derived when ideal

<figure><img src="image_10.png" /><figcaption>Fig. 5 Picture of one of the first trials</figcaption></figure>
<figure><img src="image_11.png" /></figure>

isotropic antennas are used for a uniform transmit spectrum given by [12]:

$$PL_{UB}(\text{dB}) = -10 \log_{10} \left( \frac{c^2}{(4\pi d)^2 f_{\min} f_{\max}} \right) \quad (4)$$

where c is the velocity of the light and d is the Tx-Rx separation distance. Notice that when $f = f_{\min} = f_{\max}$, (4) is the free-space path loss for a narrowband transmission.

An average 0.84 dB error was measured between both curves, probably due to slight variations between the real gain and the manufacturer datasheet. The maximum dimension of the antenna was 26 mm, and at the W-band meant a far zone distance of $2(0.026)^2/\lambda_{\min} \approx 49$ cm, being $\lambda_{\min} = c/f_{\max}$. Even if between 10 and 50 cm, we do not fulfill the far zone, the ultra wideband formula predicts the path loss accurately.

The time-delay responses and power delay profile (PDP) can be obtained from the complex channel transfer functions via the classical inverse Fourier transform. Figure 7 shows the PDPs for three selected distances (20, 30, and 50 cm). For these distances, the RMS delay spread computed with a 30-dB threshold is 0.12, 0.24, and 0.49 ns, respectively. From these curves, it is also shown that strong SMCs (specular multipath components) lie between 5 and 25 ns and that dense multipath components (DMCs) do not contribute much to the received power. This is mainly due to reflections of close objects such as the table, VNA, or the converters. The dynamic range is shown to be sufficient even by using a 100-kHz intermediate frequency.

## 4 GHz SIMO measurements

In this section, indoor channel characteristics are measured by performing SIMO measurements, carried out with virtual Tx-UCA (Uniform Circular Array) and virtual Rx-URA (Uniform Rectangular Array) systems. The VNA is configured with 1024 frequency points and 10 Hz IF.

For the transmitter, the virtual Tx-UCA uses the same horn antenna as in the previous section. For the virtual Rx-URA, an omnidirectional antenna manufactured by Mi-Wave (WR-10) was selected. This antenna operates at 94 GHz with a 3 GHz bandwidth, 2 dB gain and typical nominal VSWR of 1.5:1 [http://www.miwv.com/]. Vertical polarization has been used for all cases.

The Rx position was fixed whereas the Tx was moved around four different positions in a room. A map of the indoor scenario can be found in Fig. 8.

Figure 9 presents a general photo of the scenario from the Tx antenna. The Tx and Rx antennas were

<figure><img src="image_12.png" /></figure>
<figure><img src="image_13.png" /><figcaption>**Fig. 9** General view of the scenario for 94 GHz measurements</figcaption></figure>

operated with Arricks Robotics positioners (http://www.arrickrobotics.com/). The Tx-Rx distances were 2.552, 0.987, 3.692, and 2.092 m for Tx1, Tx2, Tx3, and Tx4, respectively.

For the virtual Tx-UCA, a 110° range was measured with a 10° step while the phase center of the antenna was kept fixed for all orientations. In all cases, and for comparison purposes, the horn antenna coordinate system was aligned such that the maximum received gain could be obtained for 55° angles between the UCA and URA (see Fig. 8), i.e., the mean angle is always facing the Rx, and it will be plotted in such a way for all results. The rotation of the UCA is clockwise. For the virtual URA, measurements were performed over a 6 × 6 uniform rectangular grid with 1.4 mm spacing along X and Y, corresponding to 0.4λ at 94 GHz. Table 1 summarizes the coordinates of each Tx and the Rx.

The relative received power, computed as the averaged received power in the frequency domain (over the 3 GHz bandwidth), is shown in Fig. 10 for all considered positions and horn antenna angles. We can see how maximum values of the received power are obtained between 50° and 60°, since the UCA was aligned at 55° for all cases. This received power can be compared with the

power computed from the free-space path loss with the optimum orientation (including 18.5 dB of the horn antenna and 2 dB for the omni antenna). Indeed, at 94 GHz with a 3-GHz bandwidth, the transmission is narrowband and the Friis formula converges to the upper bound for wideband free-space path loss. The received power for Tx1, Tx2, Tx3, and T4 are 61.4 (59.5), 57.7 (51.3), 64.5 (62.7), and 54.8 (57.8) dB, respectively, being the simulated received power inside the parenthesis. The difference was attributed to an additional complexity in both delay and angular domain (i.e., presence of multipath components). Also, another reason is attributed to the mismatch between the 55° alignment and the measured angles of 50° and 60° due to the selected 10° angular step.

<table><caption>**Table 1** Coordinates of Tx and Rx</caption><thead><tr><td></td><td>X (m)</td><td>Y (m)</td></tr></thead><tbody><tr><td>Rx</td><td>2.75</td><td>1.2</td></tr><tr><td>Tx1</td><td>4.79</td><td>2.97</td></tr><tr><td>Tx2</td><td>3.95</td><td>1.7</td></tr><tr><td>Tx3</td><td>6.3</td><td>2.63</td></tr><tr><td>Tx4</td><td>1.81</td><td>2.98</td></tr></tbody></table>

<figure><img src="image_14.png" /><figcaption>**Fig. 10** Relative received power (in dB) as a function of the UCA horn antenna angle (in °)</figcaption></figure>
<figure><img src="image_15.png" /></figure>

The rms delay spread was also computed with a 30-dB threshold (Fig. 11). A minimum in the rms values was clearly observed when the horn antenna axis was facing the URA with values of 1.58, 0.74, 1.3, and 1.61 ns for position 1 to 4, respectively. However, when the axes were not aligned, values up to 30 ns were obtained because of multiple reflections in the scenario.

In addition, the maximum-likelihood estimation (MLE) parameters of the Ricean distribution were computed from the frequency domain data [13]. Figure 12 shows the K-factor of the best-fitting distribution for all Tx positions. As observed in Fig. 11, large values of K were measured when the horn antenna faced the URA with maximum values of 14.3, 11.12, 6.9, and 11.4 dB for position 1 to 4, respectively. On the other hand, Rayleigh distributions were obtained for the side angles.

All previous results strongly indicate that the complexity of the measured radio channels depends on the horn

antenna angle with respect to the Rx. To analyze this effect, high-resolution MLE RiMAX [14] was subsequently applied to the measured SIMO radio channels to extract the SMCs for each position and horn antenna angle. For instance, the time-of-arrival (TOA), direction-of-arrival (DOA), and complex gain were jointly estimated for each path, as well as the DMCs.

As an example, Fig. 13 presents the SMCs estimation results for Tx3 with 0°, 40°, 50°, and 110° horn antenna angles. The power of each SMC is proportional to the circle radius and is also presented with a color scale. From this information, the rms angular spread was also computed with a 30-dB threshold (Fig. 14). Again, the data show that the angular spread reaches its minimum value (72.8°, 54.1°, 62.2°, and 69.6° for position 1 to 4) when the horn antenna is aligned with the URA array.

<figure><img src="image_16.png" /></figure>

<figure><img src="image_17.png" /></figure>

<figure><img src="image_18.png" /></figure>
# 5 Conclusions

This paper presents initial investigations of the radio channel characteristics in the W-band with a commercial VNA. The initial limited distance range of the setup has been successfully increased to much longer distances using longer precision cables between the VNA and converters. Initial SISO W-band measurements with horn antennas are shown for distance values up to 70 cm to validate the system. Then, SIMO measurements are presented at 94 GHz with an omnidirectional antenna and a horn antenna mounted on a rotary system. Further work includes extensive measurement campaigns at 94 GHz for indoor scenarios and deeper analysis of the DMC contribution to the radio channels.

# Acknowledgements

This work was supported by MINECO, Spain (TEC2013-47360-C3-2-P TEC2013-47360-C3-3-P) and by European FEDER funds.

# Author details

¹Departamento Tecnologías de la Información y las Comunicaciones, Universidad Politécnica de Cartagena, Cartagena, Spain. ²IEMN/TELICE, University of Lille 1, Villeneuve d'Ascq, France. ³Universitat Polècnica de València, Camino de Vera, Spain. ⁴University Center of Defense, San Javier Air Force Base, MDE-UPCT, C/Coronel López Peña, s/n, 30720, Santiago de la Ribera, Murcia, Spain.

Received: 28 July 2015 Accepted: 18 January 2016

Published online: 28 January 2016

# References

1. D Zico, Ultra-wideband and 60 GHz communications for biomedical applications. Springer. http://link.springer.com/book/10.1007%2F978-1-4614-8896-5.

2. L Jofre, J Romeu, S Capdevila, J Abril, E Nova, M Alonso, The "challenging" world of Terahertz radiation and imaging. Proceedings of the 5th European Conference on Antennas and Propagation (EUCAP), 2011, pp. 3470-3475

3. M Kawase, "Non-destructive evaluation method of pharmaceutical tablet by terahertz-time-domain spectroscopy: application to sound-alike medicines", J. Infrared Millimeter Terahertz Waves, 34(9), 566-571

4. KD Anderson, 94 GHz propagation in the evaporation duct. IEEE Trans. Antennas Propag. 38(5), 746-753 (1990)

5. K Aydin, Y-M Lure, Millimeter wave scattering and propagation in rain: a computational study at 94 and 140 GHz for oblate spheroidal and spherical raindrops. IEEE Trans. Geosci. Remote Sens. 29(1), 593-601 (1991)

6. C Gloaguen, An experiment for propagation studies at 94 GHz. Eighth Int. Conf. Antennas Propagation 1, 406-409 (1993)

7. A Kajiwara, "Indoor propagation measurements at 94 GHz," personal, indoor and mobile radio communications, 1995. Sixth IEEE Int. Symp PIMRC'95. Wireless Merging Inf. Superhighway 3, 1026 (1995)

8. J Helminger, J Detlefsen, H Groll, Propagation properties of an indoor-channel at 94 GHz. Int. Conf. Microw Millimeter Wave Technol.Proc 98, 9-14 (1998)

9. R Piesiewicz, R Geise, M Jacob, J Jemai, T Kurner, "Indoor channel measurements of point-to-point ultra broadband short range links between 75 GHz and 110 GHz", in International Symposium Antennas and Propagation Society, 2008, pp. 1-4

10. A Brizzi, A Pellegrini, Y Hao, "Experimental characterization of the propagation on the human torso at W band", in Radio Science Meeting (Joint with AP-S Symposium), USNC-URSI, 2013, p. 39

11. K Haneda, J Järveläinen, A Karttunen, M Kyro, J Putkonen, Indoor short-range radio propagation measurements At 60 and 70 GHz, in EuCAP 2014, The Hague, The Netherlands, 2014, pp. 1-4

12. S Promwong, J Takada, Free space link budget estimation scheme for ultra wideband impulse radio with imperfect antennas. IEICE Electronics Express 1(7), 188-192 (2004)

13. NL Johnson, S Kotz, N Balakrishnan, Continuous univariate distributions, vol. 1 (Wiley-Interscience, Hoboken, 1993)

14. A Richter, Estimation of radio channel parameters: models and algorithms (Dr.-Ing. dissertation, TU Ilmenau, Ilmenau, Germany, 2005)

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