# Impacts of Absorber Loadings on Simulating the Multipath Channel in a Reverberation Chamber

Authors: Xin Zhou; Zhangdui Zhong; Xin Bian; Ruisi He; Ke Guan; Ruoyu Sun; Ke Liu; Xiaotao Guo
Journal: International Journal of Antennas and Propagation
 (2017)

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## Abstract

In reverberation chambers, the multipath channels with different delay characteristics can be generated by loading the chamber with different amounts of absorbers. This paper investigates the impacts of absorber loadings on the delay characteristics based on realistic measurements. An efficient method for estimating the root-mean-square (rms) delay spread in the chamber is presented. Furthermore, it is found that the chamber loadings also significantly affect the quality of a digitally modulated signal and the corresponding modulation quality measurements are performed.


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## Body

## 1. Introduction

Reverberation chambers (RCs) are traditionally used for electromagnetic compatibility (EMC) measurements [1, 2], and during the past decade this test facility has also attracted a lot of attentions in the wireless communication field [3–5]. In such applications, the RC is used to simulate a multipath channel. The RC is basically a metal cavity that is stirred to emulate the channel [6].The channel characteristics in the RC have been studied in many works [7–11]. For example, Genender et al. [7] showed how the power delay profile can be measured and controlled inside a RC, and it was shown that changing the loading influences the power delay profile. In [8, 9], root-mean-square (rms) delay spread was measured inside a RC with different amounts of absorber. The measured results were compared with those obtained in some real-world environments. The papers demonstrated that it is possible to simulate various real-world environments inside the RCs by changing the loadings. In [10, 11], theoretical derivation of the relationship of rms delay spread and coherence bandwidths in RC was presented. To verify the theoretical results, measurements in a RC with different loadings were conducted. All these papers showed that the channel characteristics can be adjusted by loading chamber, and some papers, for example, [8, 11], have qualitatively described the relation between the rms delay spread and the amounts of absorbing objects; that is, adding absorber will shorten the rms delay spread. However, in some applications, for example, over-the-air (OTA) test, the delay spread of the channels in the RC significantly affects the test results. Then here is one question: what is the accurate quantitative relation between the amounts of absorbers and the rms delay spread in the RC? This problem has not been well solved in the existing literatures.The absorber loading has a significant impact on the rms delay spread of the generated channel and thus affects the signal quality. Some papers have studied the impact of absorber loading on the bit error rate (BER) [8, 12]; however, modulation quality parameters, for example, Error Vector Magnitude (EVM), as alternative metrics offer several advantages. Firstly, measurements of EVM and related modulation quality parameters can pinpoint the type of degradations in a signal [13, 14]. Secondly, the BER measurement relying on the Monte Carlo approach has a long measurement time, especially at low BERs [8]. By contrast, the modulation quality parameters can be readily evaluated by transmitting fewer symbols, as compared to the BER. Hence, characterizing the performance using modulation quality parameters is preferred. However to the best of the authors’ knowledge, little work has been conducted to address the impact on the modulation quality parameters. This paper aims to fill this gap.The main contributions of this paper may be summarized as follows:(1)
An efficient method to accurately estimate the rms delay spread in the RC with amounts of absorbers is presented.(2)
The influences of heavy loading on the variance of the rms delay spread in the RC are discussed.(3)
The effect of the absorber loading on the modulation quality of a digitally modulated signal is investigated.


## 2. Impact on rms Delay Spread

The rms delay spread is widely used to characterize the delay dispersion of the channel [15]. To study the effects of the absorber loading on the rms delay spread, we used the measurement system as shown in Figure 1. The test chamber was the National Institute of Metrology (NIM) reverberation chamber, having a dimension of 5.09 m × 6.43 m × 5.57 m, as shown in Figure 2. The large size yields a generated channel with large rms delay spread and is suitable for replicating environments with a large number of multipath components, for example, urban environments [16]. The transmitting antenna was a horn antenna directed into a corner of the chamber, and the receiving antenna was a biconical antenna placed in the middle of the RC. The mechanical stirring was performed by two metal plates that were moved stepwise. We used two sizes of absorbers. As shown in Figure 3, for the small one, each piece is with 6 cones in a 3×2 array, the cone width is 10.2 cm, and the cone height is 30.5 cm. For the large one, each piece is with 81 cones in a 9×9 array, the cone width is 6.8 cm, and the cone height is 17.8 cm.Figure 1
The rms delay spread measurement setup.Figure 2
Reverberation chamber configuration.Figure 3
Absorbers used in our measurements. (a) Small absorber. (b) Large absorber.
(a)
(b)Measurements were conducted in the frequency domain by measuring the channel transfer function (CTF) over a frequency ranging from 4.9 GHz to 5.1 GHz, using the vector network analyzer- (VNA-) based measurement system as shown in Figure1 [17]. We can get the empirical channel impulse responses (CIRs), h(τ), by performing an inverse fast Fourier transform algorithm (IFFT) of the measured CTF, H(f), as [17](1)hτ=IFFTHfand the CIR can be expressed as(2)hτ=∑i=1Naie-jϕiδτ-τi,where ai, ϕi, and τi denote the amplitude, phase, and delay of the ith multipath component (MPC), respectively, N is the total number of MPCs, and δ(·) is the Dirac delta function. The power delay profile (PDP) of the channel is defined as the square magnitude of the CIR as follows:(3)PDPτ=hτ2.Then the rms delay spread can be calculated as(4)τrms=∑i=1NPDPτiτi2∑i=1NPDPτi-∑i=1NPDPτiτi∑i=1NPDPτi2,where τi and PDPτi represent the delay and corresponding delay power of theith MPC measured, respectively. When computing the rms delay spread, we set the power of all the MPCs below a threshold to zero to reduce the impact of the noise. The threshold is set to be 6 dB above the noise floor [18].The measurement was repeated for 100 different fixed paddle positions spaced by360°/100=3.6°. The large number of paddle positions provides sufficient measurement data for the analysis of the variance of the rms delay spread. For the rms delay spread estimation, the 100 measurement results were averaged to obtain the mean values for various amounts of absorbers. To show the variance of the rms delay spread, the maximum, minimum, standard deviation (SD), and relative standard deviation (RSD, equal to SD/mean) of the rms delay spread are also summarized in Table 1.Table 1
Statistics of rms delay spread for different numbers of absorbers.
Number of absorbers
RMS delay spread
Mean (ns)
Max (ns)
Min (ns)
SD (ns)
RSD
error
r
0
3050
3121
2946
31.11
1.02%
/
Large absorbers
1
1859
1976
1781
37.37
2.01%
0%
2
1365
1592
1300
52.42
3.84%
2.06%
3
1081
1323
977
72.43
6.70%
3.44%
4
892
1128
789
74.30
8.33%
4.03%
Small absorbers
1
2660
2780
2582
40.43
1.52%
0%
2
2374
2507
2291
45.34
1.91%
0.65%
3
2143
2307
2066
46.29
2.16%
1.15%
4
1999
2213
1932
50.37
2.52%
3.82%It has been shown that the rms delay spread is directly related to the chamber quality factor by the following [8]:(5)τrms=Q2πf,where f is the carrier frequency and the quality factor, Q, is the proportion of energy stored to the energy dissipated. The value of Q, that is, Qtotal in (6), is given by [19](6)Qtotal-1=Qwall-1+Qantenna-1+Qabsorber-1,where Qwall is associated with the wall loss, Qantenna is associated with energy dissipated in the antenna, and Qabsorber is associated with absorber loss. This paper focuses on the relation between the number of absorbing objects and the generated rms delay spread. Then (6) is rewritten as(7)Qtotal-1=Qtest_system-1+Qabsorber_n-1,where Qtest_system-1 equals Qwall-1+Qantenna-1 and the subscript “n” of Qabsorber_n-1 indicates the number of absorbers. The combination of (5) and (7) makes it possible to relate the number of absorbers and the rms delay spread; that is,(8)τrmstotal_n-1=τrmstest_system-1+τrmsabsorber_n-1,where τrms(total_n) is the rms delay spread for the RC with n absorbers, that is, the mean values in Table 1. τrms(test_system) is the rms delay spread for the RC with unloading.Thenτrms(absorber_n)-1 (equal to τrms(total_n)-1-τrms(test_system)-1) can be calculated from the measurement results. The calculated τrms(absorber_n)-1 is shown in Figure 4. By fitting the experimental data with a least squares regression curve, a linear model is suggested:(9)τrmsabsorber_n-1=n·τrmsabsorber_1-1.Figure 4
τ
rms
(
absorber
_
n
)
-
1 with different numbers of absorbers, together with the least square fit curves.The combination of (8) and (9) yields(10)τrmstotal_n-1=τrmstest_system-1+n·τrmsabsorber1-1,where (10), the rms delay spread for the RC (mean value) with n absorbers, τrms(total_n), can be estimated. In the model of (10), τrms(test_system) and τrms(absorber_1) can be obtained from the measurements with unloading and one loading in the RC, respectively. In our measurements, τrms(test_system)=3050 (ns); and for the large absorber case, τrms(absorber_1)=1/τrmstotal_1-1-τrmstest_system-1=4760 (ns), and for the small absorber case, τrms(absorber_1)=20802 (ns).For the proposed model of (10) applied to all the chamber loadings in Table 1, the estimated relative error for n absorbers can be calculated as(11)errorr_n=τrmstotal_n-τrmsmeas_nτrmsmeas_n,where τrms(total_n) is the estimated rms delay spread for n absorbers and τrms(meas⁡_n) is the measured rms delay spread, that is, the mean values in Table 1. In Table 1, errorr for different numbers of absorbers was also listed. The mean relative error is 2.52%. The maximum relative error is 4.02% corresponding to the four large absorbers loaded, which is more accurate compared with other methods [19].Furthermore, in Table1, we find that SD and RSD increase monotonically with the increasing amount of absorbers for both the large absorbers and small absorbers. A potential explanation is that the heavy loading decreases the uniformity in the RC and leads to the variance of the rms delay spread. The decrease of uniformity also increases the measurement uncertainty. As suggested in [20, 21], the intrinsic field uncertainty (IFU) associated with random fields inside the RC is the major contribution to the overall measurement uncertainty and the IFU at receiver can be evaluated as [20](12)uτrms=SDM,where M is number of paddle positions, that is, the average number. In our measurements, the maximum uτrms is 7.4 ns corresponding to the four large absorbers loaded, which is much less than the measurement results (the mean values in Table 1).


## 3. Impact on Modulation Quality

In order to investigate the impact of chamber loading on the quality of digitally modulated signals, we carried out modulation quality measurements inside the RC with different loadings.EVM is a key measure used to quantify the performance of a digital signal [13, 22]. An ideal signal would have all constellation points precisely at the ideal locations; however various imperfections including the influence of channel characteristics cause the actual constellation points to deviate from the ideal locations. Figure 6 shows a vectorial representation using the constellation diagram. The error vector between the ideal complex-valued symbol r(l)=rI(l)+j·rQ(l) and the received symbol s(l)=sI(l)+j·sQ(l) is defined as e(l)=s(l)-r(l). For our measurements, a total number of 1000 symbols are measured, and then EVMrms can be expressed as follows:(13)EVMrms=1/L∑l=1Lsl-rl2P0,where P0 is average symbol power and L is number of measured symbols. As one of the most important modulation quality parameters, EVMrms has been used to study the effects of the physical propagation channel on a digitally modulated signal [14, 23].The measurement setup for obtaining the EVM is shown in Figure5. A vector signal generator (VSG) was used to generate the Quadrature Phase Shift Keying (QPSK) signals with different symbol rates (15 ks/s and 60 ks/s). The output power of the VSG was 10 dBm. The center frequency of the modulated signals was 5 GHz. Up to four large absorbers were used to investigate the impact of the chamber loading on the modulation quality. A vector signal analyzer (VSA) was used to receive waveforms, demodulate them, and measure the modulation quality. Again, we placed a horn antenna directed into a corner as the transmitting antenna and a discone antenna in the middle of the RC as the receiving antenna. The EVMrms measurement was also repeated for 100 different fixed paddle positions as the rms delay spread measurements.Figure 5
Modulation quality measurement setup.Figure 6
Constellation diagram and EVM.Before conducting the measurements in the RC, modulation quality measurements were performed with connecting the VSA and VSG directly with a cable, whereEVMrms is found to be 0.25% and 0.27% for 15 ks/s and 60 ks/s, respectively. The low residual errors enable the study of RC-induced effects rather than receiver-induced effects on the modulation quality.The measurement results of the mean values ofEVMrms are shown in Figure 7. Firstly, it can be seen that low symbol rate leads to a better modulation quality. The lower symbol rate essentially implies a narrower bandwidth, which is less sensitive to frequency selectivity of channel. This is the reason that the signal with lower symbol rate will degrade less for given absorbers. Furthermore, as shown in Figure 7, heavy loading leads to better modulation quality. As mentioned above, heavy loading leads to smaller delay spread. It has been shown that the coherence bandwidth (as the measure of the frequency selectivity) is reversely proportional to the rms delay spread [10, 11]. Therefore, adding absorber will widen the coherence bandwidth and finally leads to better modulation quality [12].Figure 7
The mean values ofEVMrms with different numbers of absorbers, together with the least square fit curves.As observed in Figure7, the mean value of EVMrms fits to a rational function well, which can be written as(14)EVMrms=pn+q,where n indicates the number of absorbers. p and q are the coefficients for the rational function. For the symbol rate of 15 ks/s, p=0.15 and q=1.82; for the symbol rate of 60 ks/s, p=0.38 and q=1.85. Note that this model is heuristic, whose ultimate justification lies in its ability to fit the measurement data.Table2 shows the statistics of EVMrms. It is found that the SD and RSD are considerably high. The reason is that EVMrms values at some paddle positions are much higher than the mean values; for example, see column Max in Table 2. The high EVMrms values may come from the fact that the reflected signals cause the receiver to experience a severe fading at some paddle positions. The modulation quality of the digitally modulated signals in the RC is sensitive to the paddle positions.Table 2
Statistics ofEVMrms for different numbers of absorbers.
Symbol rate
Number of absorbers
EVMrms
Mean (%)
Max (%)
Min (%)
SD (%)
RSD
15 ks/s
0
8.24
42.81
1.14
8.57
104%
1
4.66
35.73
1.26
5.77
124%
2
3.59
30.85
1.21
3.77
105%
3
3.37
16.31
1.18
2.57
76%
4
3.05
26.59
1.24
3.02
99%
60 ks/s
0
20.61
49.60
4.66
11.36
55%
1
12.76
48.73
2.67
10.13
79%
2
9.07
39.38
1.81
6.85
75%
3
8.49
45.28
2.53
7.44
87%
4
7.01
47.79
2.07
6.12
87%The EVM is the total error and contains various degradations [13]. In order to pinpoint the degradations, four main modulation quality parameters, that is, magnitude error (ME), phase error (PE), gain imbalance (GI), and quadrature imbalance (QI) [13, 14], were measured with the same measurement setup as the EVM measurement. Figure 8 shows the mean values over the 100 paddle positions of these modulation quality parameters for different loadings. It is found that heavy loading decreases the magnitude error and phase error but the quadrature imbalance and gain imbalance do not decrease monotonically with the amount of absorbers.Figure 8
Scatter plots of the mean values of the modulation quality parameters. (a) Magnitude error. (b) Phase error. (c) Gain imbalance. (d) Quadrature imbalance.
(a)
(b)
(c)
(d)


## 4. Conclusions

This paper investigates the impacts of the absorber loadings on the delay spread and modulation quality in the RC. Based on the measurements, an efficient method for estimating the rms delay spread in the RC with the amounts of absorbing objects is presented. In addition, it is found that heavy loading leads to an increase of the variance of the rms delay spread in the chamber.The chamber loadings are found to affect the quality of the digitally modulated signals due to different channel conditions of the generated multipath channels. The modulation quality measurements show that heavy loading leads to a better modulation quality and the modulation quality is sensitive to the paddle positions.This paper presents implementation-specific details necessary for the use of RCs. Our analysis is based on realistic measurements, which makes the conclusion sufficiently reliable and can be applied when using a RC to simulate wireless propagation environments.



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