DOI QR코드

DOI QR Code

Performance Evaluation of the Complex-Coefficient Adaptive Equalizer Using the Hilbert Transform

  • Park, Kyu-Chil (Department of Information and Communications Engineering, Pukyong National University) ;
  • Yoon, Jong Rak (Department of Information and Communications Engineering, Pukyong National University)
  • Received : 2016.04.19
  • Accepted : 2016.05.11
  • Published : 2016.06.30

Abstract

In underwater acoustic communication, the transmitted signals are severely influenced by the reflections from both the sea surface and the sea bottom. As very large reflection signals from these boundaries cause an inter-symbol interference (ISI) effect, the communication quality worsens. A channel estimation-based equalizer is usually adopted to compensate for the reflected signals under the acoustic communication channel. In this study, a feed-forward equalizer (FFE) with the least mean squares (LMS) algorithm was applied to a quadrature phase-shift keying (QPSK) transmission system. Two different types of equalizers were adopted in the QPSK system, namely a real-coefficient equalizer and a complex-coefficient equalizer. The performance of the complex-coefficient equalizer was better than that of two real-coefficient equalizers. Therefore, a Hilbert transform was applied to the real-coefficient binary phase-shift keying (BPSK) system to obtain a complex-coefficient BPSK system. Consequently, we obtained better results than those of a real-coefficient equalizer.

Keywords

I. INTRODUCTION

Because of the reflections from the boundaries in underwater acoustic communication, the communication channel used is known to exhibit a frequency-selective fading channel with a multipath delay spread [1-3]. The performance of the underwater acoustic communication system degrades because of the inter-symbol interference (ISI) [4,5] caused by the signals reflected from the sea surface and the sea bottom. A channel estimation-based equalizer is usually adopted to compensate for the ISI effect [5,6].

In this study, a feed-forward equalizer (FFE) with the least mean squares (LMS) algorithm is applied to the quadrature phase-shift keying (QPSK) transmission system in order to cancel out the ISI effect [7,8]. Two types of equalizers are introduced, namely a real-coefficient equalizer and a complex-coefficient equalizer. We also introduced a binary phase-shift keying (BPSK) system with two real- and a complex-coefficient equalizers. For the imaginary part such as the quadrature (Q) channel of the QPSK system, a Hilbert transform was used in the BPSK system [9,10].

The rest of this paper is organized as follows: in Section II, a comparison of two types of equalizers is presented. In Section III, simulation configurations are introduced. Section IV presents the concept of the complex-coefficient BPSK system. In Section V, the simulation results and the experimental results of the proposed methods are discussed. A summary of the performance of the proposed method is presented in Section VI.

 

II. COMPARISON OF TWO TYPES OF EQUALIZERS

In general, there are two binary state channels, namely the in-phase (I) channel and the quadrature (Q) channel, in a QPSK modulation and demodulation system, as shown Fig. 1(a). The transmitted signal x(t) on the receiver is separated and demodulated into the output signals yI(t) and yQ(t) by using a cosine signal or a sine signal with the same carrier frequency as that used on the modulation system. Then, the output signals are converted into four-state {1 + j, 1 – j, –1 + j, –1 – j} data from each output yI(t) and yQ(t).

Fig. 1.Block diagrams of the QPSK communication system: (a) QPSK modulation system, (b) QPSK demodulation system with two real-coefficient equalizers, and (c) QPSK demodulation system with a complex-coefficient equalizer.

When an equalizer for the compensation of the channel distortion is applied to the output signals, two types of systems are considered. The first type of system includes two separated real-coefficient equalizers for each output yI(t) and yQ(t), as shown in Fig. 1(b). This system can be considered a separated two BPSK system. The other is a complex-coefficient equalizer for the merged output signal y(t) = yI(t) + jyQ(t), shown in Fig. 1(c).

 

III. SIMULATION CONFIGURATIONS

Fig. 2 shows a layout of the experimental geometry at the bay of the Gwangan Beach located on the east side of Busan city, Korea. The range between the transmitter and the receiver is set to be 50, 100, 200, and 500 m. The depths of the transmitter and the receiver are set to be 7 m and 20 m, respectively. As the temperature and the sound speed of the vertical depth were almost flat, an image method [11] was used for the implementation of the underwater acoustic communication channel, and the related channel impulse responses are shown in Fig. 3.

Fig. 2.Schematic layout of the experiment: (a) experimental configuration and (b) temperature and sound speed profiles.

Fig. 3.Channel impulse responses according to distances: (a) 50 m, (b) 100 m, (c) 200 m, and (d) 500 m.

We assumed that the channel response had five impulse signals: direct signal, surface-reflected signal, bottom-reflected signal, surface-bottom-reflected signal, and bottom-surface-reflected signal. The sampling frequency and the carrier frequency are set to be 160 kHz and 20 kHz, respectively. The transmission rates are set to be 500, 1000, 2000, and 4000 symbols per second (sps). The transmitted image is a standard Lena image that consists of 50 × 50 pixels with an 8-bit resolution (20,000 bits).

Fig. 4 shows the block diagram of the FFE with the LMS algorithm. Here, m(n), y(n), z(n), e(n), and denote binary data in the modulation system, the channel output, the equalizer output, the error signal, and the decision output, respectively. The LMS algorithm is used for the determination of the coefficient on the equalizer to compensate for the ISI. The FFE consists of a transversal finite impulse response filter with 30 taps. The filter output, the estimation error, and the tap-weight adaptation are represented as discussed in [5].

where H, *, and μ denote the Hermitian form, the complex conjugate, and the step size parameter, respectively.

Fig. 4.FFE with LMS algorithm.

 

IV. CONCEPT OF COMPLEX BPSK SYSTEM

In this section, we introduce a complex BPSK system based on the concept of the QPSK system. The BPSK system has the same structure as the I channel of the QPSK system and has two states {1, –1}. To obtain the Q-channel signal, a Hilbert transform was adopted. The Hilbert transform can be represented as follows [9,10]:

It was obtained using the imaginary signal yQ(t) with a 90° phase shift from the original real signal yI(t). The imaginary part of the binary data in the modulation system m(n) was also calculated for obtaining estimation error in Eq. (2). The BPSK modulation and demodulation system with a real-coefficient equalizer and a complex-coefficient equalizer is shown in Fig. 5.

Fig. 5.BPSK communication system: (a) BPSK modulation system, (b) BPSK demodulation system with a real-coefficient equalizer, and (c) BPSK demodulation system with a complex-coefficient equalizer.

 

V. RESULTS AND DISCUSSIONS

First, the simulation results of two different equalizers of the QPSK system are presented. The bit error rates (BERs) according to the transmission rate and the range are presented in Fig. 6 and Table 1, respectively.

Fig. 6.Comparison of results obtained using two different types of equalizers: (a) no equalizer, (b) with two real-coefficient equalizers, and (c) with a complex-coefficient equalizer.

Table 1.No Eq: no equalizer, R. Eq: real-coefficient equalizer, C. Eq: complex-coefficient equalizer.

In Fig. 6, (a) shows the result obtained without the use of an equalizer; (b) the result obtained using two real-coefficient equalizers; and (c) the result obtained using a complex-coefficient equalizer. The same number of iterations for the training of the coefficient on the FFE is set for each simulation. From the obtained results, we concluded that the complex-coefficient LMS equalizer shows a better performance than the two separated real-coefficient LMS equalizers. The filter’s output signal z(n), error signal e(n), and tap-weight vector w(n) have a cross-coupling system between them, as shown in Eqs. (1)–(3). This implies that a complex LMS algorithm is equivalent to a set of four real LMS algorithms because of the cross-coupling system between the filter output signal, the error signal, and the tap-weight vector. From Fig. 6, we can infer that the results obtained in the case of the low sps and the long range were better than those obtained in the case of the high sps and the short range.

Second, Fig. 7 and Table 2 show the simulation results of two different equalizers in the BPSK system. In Fig. 7, (a) shows the result obtaining without using the equalizer; (b) the result obtained using a real-coefficient equalizer; and (c) the result obtained using a complex-coefficient equalizer. The same number of iterations for the training of the coefficient on the FFE is set for all the simulations. Further, the results obtained using the complex-coefficient LMS equalizer were better than those obtained using the real-coefficient LMS equalizer in the BPSK system.

Fig. 7.Comparison of results using two different types of equalizers: (a) no equalizer, (b) using a real-coefficient equalizer, and (c) using a complex-coefficient equalizer.

Table 2.No Eq: no equalizer, R. Eq: real-coefficient equalizer, C. Eq: complex-coefficient equalizer.

Finally, Fig. 8 shows the results of the equalization of the experimental data, carried out in a shallow ocean. The experimental conditions are the same those as shown in Fig. 1. The distance between the transmitter and the receiver was 10 m, and the bit rate was chosen to be 50 sps. In Fig. 8, (a) shows an original Lena image, (b) presents the result obtained without using an equalizer (BER=0.224), (c) and (d) illustrate the results with two real-coefficient equalizers (BER=0.181) and a complex-coefficient equalizer (BER= 0.123), respectively. Therefore, we can conclude that the complex-coefficient equalizer performs better than the two real-coefficient equalizers.

Fig. 8.Experimental results: (a) original, (b) without the equalizer, (c) with real-coefficient equalizers, and (d) with a complex-coefficient equalizer.

 

VI. CONCLUSIONS

In this study, an FFE with the LMS algorithm was applied to the QPSK system, and two real-coefficient equalizers and a complex-coefficient equalizer were adopted; their results were compared. The performance of a complex-coefficient equalizer was better than that of the two real-coefficient equalizers. On the basis of the results of the QPSK system, a Hilbert transform was applied to the real-coefficient BPSK system in order to obtain the complex-coefficient BPSK system. Further, the performance of a complex-coefficient equalizer was better than that of the two real-coefficient equalizers in the BPSK system.

References

  1. T. C. Yang, “Properties of underwater acoustic communication channels in shallow water,” Journal of the Acoustical Society of America, vol. 131, no. 1, pp. 129-145, 2012. https://doi.org/10.1121/1.3664053
  2. T. B. Aik, Q. S. Sen, and Z. Nan, "Characterization of multipath acoustic channels in very shallow waters for communications," in Proceeding of OCEANS 2006 - Asia Pacific, Singapore, pp. 1-8, 2006.
  3. W. B. Yang and T. C. Yang, “High-frequency channel characterization for M-ary frequency-shift-keying underwater acoustic communications,” Journal of the Acoustical Society of America, vol. 120, no. 5, pp. 2615-2626, 2006. https://doi.org/10.1121/1.2346133
  4. J. Park, J. R. Yoon, and J. S. Park, “Frequency and temporal coherence variation for sea surface fluctuation,” Japanese Journal of Applied Physics, vol. 48, no. 7S, article ID. 07GL03, 2009.
  5. J. Park, K. C. Park, and J. R. Yoon, “Underwater acoustic communication channel simulator for flat fading,” Japanese Journal of Applied Physics, vol. 49, no. 7S, article ID: 07HG10, 2010.
  6. J. Kim, K. C. Park, J. Park, and J. R. Yoon, “Coherence bandwidth effects on underwater image transmission in multipath channel,” Japanese Journal of Applied Physics, vol. 50, no. 7S, article ID. 07HG05, 2011.
  7. Y. H. Yoon and A. Zielinski, "Simulation of the equalizer for shallow water acoustic communication," in Proceeding of OCEANS 1995, San Diego, CA, pp. 1197-1203, 1995.
  8. S. S. Haykin, Adaptive Filter Theory, 3rd ed. Upper Saddle River, NJ: Prentice Hall, 1996.
  9. J. G. Proakis, Digital Communications, 5th ed. New York: McGraw-Hill, 2008.
  10. A. B. Carlson, Communication Systems, 3rd ed. New York: McGraw-Hill, 1986.
  11. F. B. Jenson and W. A. Kuperman, Computational Ocean Acoustics. New York: AIP Press, 1994.

Cited by

  1. Hilbert-Transform-Based Accurate Determination of Ultrashort-Time Delays in Terahertz Time-Domain Spectroscopy vol.7, pp.5, 2017, https://doi.org/10.1109/TTHZ.2017.2713602
  2. Performance Comparison of Acoustic Equalizers using Adaptive Algorithms in Shallow Water Condition vol.22, pp.2, 2016, https://doi.org/10.6109/jkiice.2018.22.2.253