San Jose State University From the SelectedWorks of Robert Henry Morelos-Zaragoza April, 2015 On Performance Improvements with Odd-Power (Cross) QAM Mappings in Wireless Networks Quyhn Quach Robert H Morelos-Zaragoza Available at: http://works.bepress.com/robert_morelos-zaragoza/46/ On Performance Improvements with Odd-Power (Cross) QAM Mappings in Wireless Networks Quyhn Quach and Robert H. Morelos-Zaragoza AbstractβModern wireless networks use QAM modulation with mappings that are derived from square signal constellations in which the number of signal points is an even power of two. In the particular case of IEEE 802.11 networks, these mappings are 4-QAM, 16-QAM and 64-QAM and are hereto referred as evenpower QAM mappings. This paper considers the performance improvements that are obtained by adding odd-power QAM mappings (obtained from cross QAM constellations) to the set of available mappings. These odd-power mappings are associated with 22m-1-QAM cross constellations that are carved out from larger 22m-QAM square constellations. For the specific cases of 8QAM, 32-QAM and 128-QAM mappings, the improvements in throughput are quantified assuming a Rayleigh fading condition. Furthermore, in order to illustrate the use of bit metrics generated by a demapper, also examined is the performance of bit-interleaved 8-QAM and 32-QAM mappings with binary codes over an AWGN channel. Index TermsβWireless networks; Quadrature-amplitude modulation; Throughput; Demapping; Channel coding. Second, as channel coding forms an integral part of modern wireless networks, illustrative examples of demappers and their application in maximum likelihood decoding of a short ReedMuller code are presented for 8-QAM and 32-QAM mappings. The paper is organized as follows. Section II presents a good approximation on the average bit error probability (ABEP) of QAM mappings under additive white Gaussian noise (AWGN). This expression of the ABEP is used in Section III to determine the increase in throughput that is achieved by the introduction of odd-power QAM mappings. In section IV, for the specific cases of 8-QAM and 32-QAM, the performance is examined of demappers for bit-interleaved odd-power QAM mappings combined with a first-order RM code and a binary LDPC code over an AWGN channel. Finally, section V gives final remarks and directions for future research. II. ODD-POWER π-QAM MAPPINGS The odd-power 2!βπ!! -QAM mappings that are considered in this paper are those associated with cross QAM constellations I. INTRODUCTION carved out from larger square 2!βπ -QAM constellations [4]. HE physical layer of current wireless networks uses bits-to- Figures 1 to 3 show the 8-QAM, 32-QAM and 128-QAM symbol mappings based on square π-QAM constellations signal constellations with βπ = 2, 3 and 4 respectively studied [1-3]. This is to say that the number of signal points is an even in this paper. power of two: π = 2!βπ , 1 β€ βπ β€ 5, with the integer π = 2βπ equals to the number of bits per symbol. These mappings are referred to as even-power QAM mappings. While it is advantageous to have a square QAM constellation in which each signal point coordinate (in-phase and quadrature matchedfilter outputs) is in turn a signal point in a PAM constellation, recent advances in signal processing platforms and algorithms allow for the extension of the set of available mappings to include odd-power π-QAM mappings with π = 2!βπ!! . T The purpose of this paper is to explore the advantages of including odd-power QAM mappings in the set of even-power Fig. 1. 8-QAM signal constellation. QAM mappings that are already implemented. Two aspects are considered: The first one is the improvement in throughput that In this section an overview is given of a good approximation results from adding a new set of odd-power QAM mappings. It is shown in particular that, with data transmission in IEEE on the average bit error probability (ABEP). The expression is 802.11-2012 wireless networks under Rayleigh fading used it to determine ranges of values of the average symbol conditions, up to a 9% increase in throughput is possible. energy-to-noise ratio πΈ! /π! for which a target value of ABEP is not exceeded. This helps to determine the throughput of a wireless network with a given set of available QAM mappings Paper submitted to GLOBECOM 2015 on April 1, 2015. The authors are with the Department of Electrical Engineering, San José and a probability density function of the received signal State University, San Jose, CA 95192-0084 USA. (Contact e-mail: energy. This is discussed in section III. [email protected]). TABLE 1 QAM SIZE, ERROR COEFFICIENT AND NORMALIZED MSED M π! π· ! /πΈ! 4 8 16 32 64 128 256 2 2 9/4 7/2 7/2 15/4 15/4 2 2/3 2/5 2/10 2/21 2/41 2/85 Fig. 2. 32-QAM signal constellation. QAM mappings in Figure 4. In Section III these theoretical expressions are used to estimate the increase in throughput that is achievable by the introduction of odd-power QAM mappings. Fig. 3. 128-QAM signal constellation. A. Bit error probability of M-QAM mappings π Assuming Gray bits-to-signal mappings of 2 βQAM signal constellations, the ABEP π! that is well approximated by the expression π! π! = π π π·! , (1) 2π! Fig. 4. Average bit error probability of BPSK mapping and 2! -QAM mappings, for 2 β€ π β€ 8. III. THROUGHPUT IMPROVEMENT UNDER RAYLEIGH FADING To illustrate the improvements in throughput that can be obtained with the inclusion of a set of odd-power QAM where π· ! is the minimum squared Euclidean distance (MSED) mappings, a simple Rayleigh fading condition is assumed such between signal points expressed in terms of the average symbol that the signal energy-to-noise ratio Ξ has an exponential energy πΈ! , π! /2 is the AWGN power spectral density and π! probability density function: is the error coefficient (i.e., the average number of nearest 1 πΎ π! πΎ = exp β π’(πΎ), neighbors). Figure 4 shows the ABEP curves based on Eq. (1) πΎ! πΎ! π for BPSK mapping and 2 βQAM mappings with 2 β€ π β€ 8. In the figures, the curves with dashed lines correspond to the where πΎ! is the average symbol energy-to-noise ratio. BEP of the even-power QAM mappings that are currently used A value of signal energy-to-noise ratio Ξ inside an interval in 802.11 networks [1], while curves with solid lines to [πΎ! , πΎ! ], corresponds to a transmission rate π (πΎ! , πΎ! ) in bits per indicate the BEP of odd-power QAM mappings. symbol, or bps/Hz, using the error performance curves of Table 1 shows the values of constellation size π, error QAM mappings in Figure 4, such that the ABEP is lower than coefficient π! , and normalized MSED π· ! /πΈ! , for each of the a target maximum ABEP value. is implemented with a binary first-order Reed-Muller code of length π = 8, denoted RM(3.1) code. The idea is simply to illustrate the use of bit metrics with maximum-likelihood softdecision decoding for odd-power mappings. TABLE 2 INTERVALS AND TRANSMISSION RATES FOR A TRAGET π! = 0.01 π πΎ!! πΎ!! π (πΎ!! , πΎ!! ) 1 2 3 4 5 6 7 8 4 7.4 11.5 13 17 19.5 22.5 25.5 7.4 11.5 13 17 19.5 22.5 25.5 β 1 2 3 4 5 6 7 8 For a given set of available QAM mappings, the average throughput is readily obtained as π =πΈ π = π Ξ³!! , πΎ!! !β! = π !β! = !!! !!! !!! !!! π! πΎ ππΎ π! πΎ ππΎ π exp β !β! πΎ!! πΎ!! β exp β πΎ! πΎ! , where πΌ denotes the set of available QAM constellations and for simplicity it is assumed that no channel coding is used. In the case of even-power mappings, πΌ! = 1,2,4,6,8 , while with the inclusion of odd-power mappings the set is larger and given by πΌ! = 1,2,3,4,5,6,7,8 . Table 2 shows the set of values of interval limits πΎ! , πΎ! and transmission rate π (πΎ! , πΎ! ) for all the QAM mappings in Figure 1 and a target ABEP π! = 0.01. Let π ! and π ! denote the average throughput of a wireless network with even-power QAM mappings only and with all QAM mappings. Since the set of available QAM constellations is larger when including cross constellations, πΌ! β πΌ! , it is expected that the throughput will be higher. To quantify this increase in information rate, define the rate increase as Fig. 5. Rate increase Ξπ (%) versus average symbol energy-to-noise ratio πΎ! (dB), under Rayleigh fading, for a target ABEP of 0.01 A. Bit-interleaving and Demapping For a given π-QAM mapping with π = 2! , a rectangular interleaver is used heretofore. A total of π binary codewords out of a channel encoder are arranged in an array of π rows and π columns, where π is the code length. The QAM mapper then takes as input every column of the array and maps it to a symbol to be modulated. Therefore, with a binary RM(3,1) code and 8-QAM and 32-QAM mappings respectively, the interleavers are of size 3-by-8 and 5-by-8. The transmitted QAM symbol sequences are of length eight. As pointed out in [5], it is essential that Gray mapping of bits to symbols be applied so that an equivalent wireless link with π parallel and independent binary channels is created. At the receiver end of the link, the eight in-phase and quadrature matched-filter outputs (π¦! , π¦! ) are input to a π ! Ξπ = β 1. demapper that produces π bit metrics, one metric for every bit π ! used to label the QAM constellation points. A bit metric is Figure 5 shows the value of Ξπ as a percentage plotted as a given by the logarithm of the ratio of two a-posteriori function of πΎ! for a target ABEP of 0.01 with the QAM probabilities, conditioned to bit values 0 and 1 [5], mappings in Figure 4. The results show that the maximum rate π!! ! increase is 9% and corresponds to an average signal energy-to! exp ! ! ! π π΅! = log , noise ratio of approximately 17 dB. π!! ! ! exp ! ! ! IV. DEMAPPING AND CHANNEL CODING where πΌ represents a signal point with π΅! = 0, π½ represents a In this section, the error performance with bit interleaving signal point with π΅! = 1, and π¦ = (π¦! , π¦! ) is the pair of and channel coding, in conjunction with odd-power QAM matched-filter outputs from the quadrature demodulator. mappings, is illustrated. For simplicity of exposition, attention is focused on 8-QAM and 32-QAM mappings. Channel coding Figure 6 shows the metrics for the two most-significant AWGN channel and one with either Rayleigh or Rician fading. label bits π΅! and π΅! for the three odd-power mapings examined The results are shown in Figure 8 with BER representing the in this paper. These metrics are the same as QPSK mapping, bit error rate and πΈ! /π! the average bit energy-to-noise ratio. since these two bits identify the quadrant in which the signal point lies. On the other hand, as opposed to even-power mappings based on square π-QAM signal constellations that be expressed as the Cartesian product of two π-PAM signal constellations, the bit metrics of the π β 2 least-significant bits in odd-power QAM mappings depend on both matched filter outputs (π¦! , π¦! ). The computation of these metrics is therefore slightly more complex compared to even-power mappings. Figure 7 shows the bit metric for the least significant bit π΅! for 8-QAM mapping. After the demapping process, the bit metrics are written column-by-column into an π-by-π rectangular array. This process is known as deinterleaving. Each element in a row of this metric array (π metrics) constitutes a BPSK-mapped noisy binary codeword bit that is fed into a binary channel decoder in order to estimate its value. Fig. 7. Bit metric of the least-significant bit of 8-QAM mapping. The simulated BER performance curves in Figure 8 show that the bit-interleaved 32-QAM, with a block interleaver of length eight, degrades and eventually reaches an error floor. The reason for this behavior is that, as mentioned in [5], the interleaver length π is not sufficiently long relative to the number of bits per symbol π. Since π = 8 and π = 5 for 32QAM mapping and the binary RM(3,1) code, the bits metrics become highly correlated and error performance does not improve at higher values of signal energy. The performance of a longer binary projective geometry (273,191) low-density parity-check (LDPC) code [6] with a block interleaver and 32QAM, shown in Figure 9, does not show a floor because the length of the code is now much larger than the number of bits per symbol. In the simulations, the number of iterations was set to 8 and decoding performed with belief propagation using Fig. 6. Bit metrics of the two most-significant bits of all the π-QAM LLR metrics from the demmaper. mappings considered in this paper. V. CONCLUSIONS B. Performance with a binary RM(3,1) code In this section, simulation results are presented on the performance of bit-interleaved 8-QAM and 32-QAM mappings using the rectangular interleaver and bit metrics generated by a rectangular demapper described in the pervious section. In the computer simulations, maximum-likelihood decoding was implemented with a Green machine (equivalent to a trellis decoder [6]) for the first-order binary RM(3,1) code of length π = 8. The channel model was assumed is AWGN (i.e., no fading), as the relative difference in error performance with channel coding does not change significantly between an It has been shown that augmenting the set of available mappings in a wireless network, with the inclusion of oddpower QAM mappings, results in an increased throughput. As an illustration, the improvement in throughput was quantified for data transmission under Rayleigh fading conditions. The results show that augmenting the set of modulations in the IEEE 802.11 standard [1] by 8-QAM, 32-QAM and 128-QAM mappings can possibly yield an increase of up to 9% in throughput compared to the use of even-power QAM mappings alone, with a relatively low complexity cost incurred in the computation of bit metrics at the demapper. Moreover, the error performance of the combination of bit interlaving and channel coding was examined for the cases of 8-QAM and 32QAM mappings with a binary RM(3,1) code and 32-QAM with a binary finite-geometry (273,191) LDPC code. Future work includes a theoretical analysis of the rate increase obtained by augmenting the set of available mappings under different signal energy probability density functions due to different fading scenarios. Also contemplated is a more comprehensive study of the combination of odd-power QAM mappings, their associated demappers and binary low-density parity-check (LDPC) codes from the IEEE 802.11 standard [1]. Fig. 9. Error performance of a binary PG (273,191) LDPC code with a rectangular bit-interleaver and 32-QAM mapping. REFERENCES [1] [2] [3] Fig. 8. Error performance of a binary RM(3,1) code with a rectangular bit-interleaver and 8-QAM and 32-QAM mappings. [4] [5] [6] Part 11: Wireless LAN Medium Access Control (MAC) and Physical Layer (PHY) Specifications, IEEE Standard 802.11-2012. Part 11: Wireless LAN Medium Access Control (MAC) and Physical Layer (PHY) Specifications, Amendment 3: Enhancements for Very High Throughput in the 60 GHz Band, IEEE Standard 802.11ad-2012. Part 11: Wireless LAN Medium Access Control (MAC) and Physical Layer (PHY) Specifications, Amendment 4: Enhancements for Very High Throughput for Operation in Bands below 6 GHz, IEEE Standard 802.11ac-2013. G. J. 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