The Gamma Variate with Random Shape Parameter and Some Applications

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ITSUBISHI ELECTRIC RESEARCH LABORATORIES http://www.merl.com The Gamma Variate with Random Shape Parameter and Some Applications aaref, A.: Annavajjala, R. TR211-7 December 21 Abstract This letter provides a new outlook at the Gamma distribution and its involvement in the performance analysis of digital communications over wireless fading channels. Whereas the Gamma distribution is usually regarded as a two-parameter distribution with a scale and shape factors that are deterministic parameters, we investigate the implications and insight that can be drawn from considering a Gamma variate with a random shape factor. Applications of such a distribution in the context of information transmission over a wireless fading channel are provided and novel average symbol error probability SEP) expressions for single and multi-channel reception are derived involving the Laplace transform of the new distribution. We analytically prove and verify via numerical simulations that the average SEP results induced by the random shape parameter are lower bounded by those obtained using a deterministic fading severity whose value equals the expected value of the random shape parameter. IEEE Communications Letters This work may not be copied or reproduced in whole or in part for any commercial purpose. Permission to copy in whole or in part without payment of fee is granted for nonprofit educational and research purposes provided that all such whole or partial copies include the following: a notice that such copying is by permission of itsubishi Electric Research Laboratories, Inc.; an acknowledgment of the authors and individual contributions to the work; and all applicable portions of the copyright notice. Copying, reproduction, or republishing for any other purpose shall require a license with payment of fee to itsubishi Electric Research Laboratories, Inc. All rights reserved. Copyright c itsubishi Electric Research Laboratories, Inc., 21 21 Broadway, Cambridge, assachusetts 2139

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The Gamma Variate with Random Shape Parameter and Some Applications Amine aaref, ember, IEEE, and Ramesh Annavajjala, Senior ember, IEEE Abstract This letter provides a new outlook at the Gamma distribution and its involvement in the performance analysis of digital communications over wireless fading channels. Whereas the Gamma distribution is usually regarded as a two-parameter distribution with a scale and shape factors that are deterministic parameters, we investigate the implications and insight that can be drawn from considering a Gamma variate with a random shape factor. Applications of such a distribution in the context of information transmission over a wireless fading channel are provided and novel average symbol error probability SEP) expressions for single and multi-channel reception are derived involving the Laplace transform of the new distribution. We analytically prove and verify via numerical simulations that the average SEP results induced by the random shape parameter are lower bounded by those obtained using a deterministic fading severity whose value equals the expected value of the random shape parameter. Index Terms Gamma distribution, digital communication systems, fading/shadowing channel models, receiver performance analysis. I. INTRODUCTION The Gamma variate which belongs to the family of continuous distributions, has long been associated with the modeling of wireless fading channels and as such has played an important role in the performance analysis of digital communication systems over fading channels. As a notable example, smallscale fading of the wireless channel gain is often modeled by the versatile Nakagami-m distribution which has been shown to fit experimental data 1] and whose corresponding power statistics are Gamma distributed 2]. The appeal of the Gamma distribution owes as much to its simplicity as to its mathematical tractability compared to other distributions which may not always lend themselves to further analytical derivations. A Gamma-distributed random variable RV) β is denoted as β Υk, Ω), with k > being the shape factor and Ω > the scale parameter. In the context of information transmission over wireless fading channels, the scale parameter Ω relates to the average fading power whereas the fading/shadowing severity is captured by the shape parameter k. In many practical scenarios, notably those involving user/scatterer mobility where the fading environment is constantly changing, it may not be possible to determine the fading severity a priori. Unsurprisingly, recent measurement campaigns conducted in the Amine aaref is with INRS, University of Quebec, ontreal, QC, H5A1K6 Canada e-mail: maaref@ieee.org). Ramesh Annavajjala is with itsubishi Electric Research Laboratories ERL), 21 Broadway, Cambridge, A, 2139 USA e-mail: ramesh.annavajjala@gmail.com). urban area of Valencia in Spain 3] prove that the Nakagamim parameter, hence the shape factor of the underlying Gamma random variable used to model the fading channel, is inherently variable even when observed within the confines of the same urban environment. A normalized histogram of the m parameter at 9Hz band 3, Fig. 3] reveals that m actually ranges from m min =.5 to m max = 3.5 with an average value of µ m = 1.56 and a standard deviation of σ m =.34. Hence the fading severity does indeed vary from severely fading to lightly fading. In general, the fading severity is influenced by a number of parameters such as the environment type, the operating frequency, the transmitter and receiver antenna heights, polarizations and separation distance as well as the relative position of the scatterers. In practice, all these parameters are subject to change even assuming a low mobility or static fading environment. Therefore, instead of treating the fading severity index as deterministic, we propose to model it as a RV and evaluate the Laplace transform LT) of the ensuing Gamma variate when its shape parameter is drawn from some distribution that is known a priori, thereby revealing interesting insights on the Gamma distribution when leveraged from this new angle. The remainder of this letter is as follows. In Section II, we present the Gamma distribution with random shape parameter and determine its Laplace transform. In Section III, we provide applications of the new distribution to the performance analysis and average SEP evaluation of digital modulations over fading channels with and without diversity reception. Section IV provides numerical results along with an associated technical discussion and finally concluding remarks are presented in Section V. II. GAA DISTRIBUTION WITH RANDO SHAPE PARAETER Let β Υk, Ω). Hence, the probability density function PDF) of β is given by f β x) = e x Ω x k 1 Ω k, k 1 and x, 1) Γk) where Γn) = e u u n 1 du is the standard Gamma function. The LT of the PDF 1), L β s) = Ee sβ ], can be expressed as L β s) = 1 + sω) k, R{s}. 2) Note that 1) and 2) are valid when Ω and k are deterministic parameters.

When the shape parameter k is drawn from a probability distribution, 1) and 2) represent the conditional PDF and conditional LT, conditioned on K = k, where K is a RV representing the shape parameter. Focusing on 2), we write L β s) = E e sβ] = E E { e sβ K = k }] = E 1 + sω) K] = E e log1+sω)k] = L K log 1 + sω)). 3) Note that 3) is valid when the RV K is continuous or discrete. The expected value of β can be obtained from 3) as Eβ] = d ds L βs) s= Ω = Ke 1 + sω E log1+sω)k] s= = ΩEK]. 4) Note that 4) can alternatively be obtained as Eβ] = E E {β K = k}] = EΩk] = ΩEK]. Since α = log 1 + sω) >, making use of Jensen s inequality implies that Ee αk ] e αek]. That is, a lower bound on 3) is obtained as follows L β s) 1 + sω) EK]. 5) Note that 5) becomes an equality when K = k with probability one. We now extend 3) and 5) to the case of multiple Gamma RVs with arbitrarily correlated shape parameters. We consider N RVs β 1,..., β N. Let K n denote the shape parameter RV associated with β n. We assume that conditioned on K 1,..., K N β 1,..., β N are independent. That is f β1,...,β N K 1,...,K N x 1,..., x N ) = N f βn K n x n ). 6) The joint LT of β 1,...,β N is obtained as L β1,...,β N s 1,..., s N ) = E e ] N snβn = E E e ]] N snβn K1,..., K N N = E E ] ] e snβn K n N ] = E 1 + s n Ω n ) Kn = L K1,...,K N log 1 + s 1 Ω 1 ),...,log 1 + s N Ω N ))7) whereas Jensen s inequality yields L K1,...,K N log 1 + s 1 Ω 1 ),...,log 1 + s N Ω N )) N 1 + s n Ω n ) EKn]. 8) As will be shown in Section III, expressions in 3) and 5), as well as their multivariate counterparts in 7) and 8), have direct applications to the performance analysis of linear modulation schemes over wireless fading channels. III. APPLICATIONS The fading severity index also known as the scintillating index or coefficient of variation CV) 4] 1 of the single-variate Gamma distribution with random shape parameter is computed as CV = Eβ 2 ] E 2 β] 1 = Var K) + K K, 9) where Var K) denotes the variance of K. Here, it is worthwhile noticing that the CV depends on the first two moments of the shape factor distribution rather than its actual value. Now, consider communication over a single-input singleoutput SISO) flat fading channel. With E s the average symbol energy and N the one-sided power-spectral density of the additive white Gaussian random process, the instantaneous received signal-to-noise ratio SNR) is γ = E s /N )β, where β denotes the instantaneous fading power. When β is a Gamma RV with random shape parameter, the average received SNR is γ = Eγ] = E s /N )Eβ] = E s /N )ΩK, where K = EK] is the average fading severity. That is, we can express the scale parameter Ω as Ω = γ N E s K. 1) Assuming -PSK modulation, the average SEP is 5] P s, PSK = 1 π = 1 π = 1 π L β E s L K log ) sin 2 π L γ sin 2 θ ) N sin 2 θ 1 + γ K Upon using 5) in 11), we have P s, PSK π 1 + γ K 1 )) K. 11), 12) proving that the average SEP induced by the random shape parameter is in fact lower bounded by the one obtained with a deterministic fading severity index whose value equals the expected value of the random fading severity index. This is not only an intuitive result but also one that is valid for a wide range of fading severity index distributions. We can also consider the case with L antennas at the receiver with maximal ratio combining RC). Here, the instantaneous received SNR on the lth branch is denoted by γ l, whereas the SNR at the output of the RC receiver is γ = L l=1 γ l. We denote the scale and shape parameters on the lth branch by Ω l and K l, respectively. Similar to 1), we have N Ω l = γ l, 13) E s K l 1 Note that the CV is related to another fading severity measure which is the amount of fading AF) defined as AF := CV 2.

where γ l = E s /N )Eβ l ] is the average received SNR and K l = EK l ] is the average fading severity on the lth branch, respectively. Assuming arbitrarily correlated β 1,..., β L, as in 6), we have L γ s) = L γ1,...,γ L s,..., s), and an expression similar to 11) and 12) can be obtained as P s, PSK = log 1 + γ 1 K 1 π L K 1,...,K L ),..., log 1 + γ L π L l=1 1 1+ γ l K l K L ) ) 14) ) Kl. 15) Expressions similar to 11), 12), 14) and 15) can also be obtained for other modulation formats such as -QA. We note that 11) and 14) are valid for arbitrary distributions of the fading severity index K, and we only need the LT of K to compute the average error rates. IV. NUERICAL RESULTS In this section, we provide numerical results to illustrate the analytical ones obtained in the previous two sections. Fig. 1 shows the average SEP of -PSK modulation with {2, 8} on Gamma fading channels. Both deterministic and random fading severity indexes are considered. With deterministic fading severity index, we consider k = 1 and k = 5, whereas with random fading severity index we assume that K is uniformly distributed over the interval 1, 5]. From Fig. 1, we conclude that k = 1 leads to a first-order diversity performance, whereas k = 5 predicts a fifth-order diversity performance. On the other hand, with a uniformly distributed random fading severity index, the diversity order of average SEP is conservatively estimated to be within that induced by the deterministic fading severity indexes. Fig. 1 further upholds the lower bound obtained using a deterministic fading severity whose value equals the expected value of the random shape parameter. Fig. 2 illustrates the average bit error rate BER) performance of 16-QA on measured Nakagamim fading channels 3] where a discrete approximation for the distribution of the Nakagami parameter m is shown in the upper part of Fig. 2. In addition to the middle curve representing the BER of 16-QA averaged over both the fading distribution as well as the measured distribution of the m parameter, a lower and upper bounds on the average BER performance are also depicted pertaining to the average BER results of 16-QA with deterministic m values corresponding to m =.625 and m = 3.375, respectively. V. CONCLUSION In this letter, we introduce the Gamma distribution with random shape factor as a new model for analyzing the performance of digital communications over fading channels. It is noteworthy to mention that the random shape factor idea investigated in this letter can easily be exported to a Average Symbol Error Probability 1 1 1 1 2 1 3 1 4 1 5 1 6 1 7 BPSK: k = 1 BPSK: k = 5 BPSK: K ~ U1, 5] Uniformly Distributed Fading Severity Index BPSK: Lower Bound 8 PSK: k = 1 8 PSK: k = 5 8 PSK: K ~ U1, 5] 8 PSK: Lower Bound 1 8 2 4 6 8 1 12 14 16 18 2 Average Received SNR db] Fig. 1. Average SEP of BPSK and 8-PSK modulations on Gamma fading channels with uniform fading severity index. Probability Average BER.4.3.2.1 Discrete Distribution Approximation of easured Nakagami Parameter.5 1 1.5 2 m value bin average) 2.5 3 3.5 1 5 16 QA on easured Nakagami Fading Channels Lower Bound Average Upper Bound 1 15 2 25 3 35 Average Received SNR per bit db] Fig. 2. Average BER of 16-QA on measured Nakagami-m fading channels. Rician fading channel model with random line-of-sight LOS) component, in which case analog results for the CV, the average SEP and its lower bound can also be derived. ACKNOWLEDGENT The authors would like to thank Dr. L. Rubio for providing us with the data traces of the measurement campaign reported in 3]. REFERENCES 1]. Nakagami, The m-distribution a general formula of intensity distribution of rapid fading, in Statistical ethods in Radio Wave Propagation. Oxford, U.K.: Pergamon Press, 196, pp. 3 36. 2] S. K. N. L. Johnson and N. Balakrishnan, Continuous Univariate Distributions: Volume 1, 2nd ed. Wiley Series in Probability and athematical Statistics, 24. 3] L. Rubio, J. Reig, and N. Cardona, Evaluation of Nakagami fading behavior based on measurements in urban scenarios, AEU Int. J. Electron. Commun., vol. 61, no. 2, pp. 135 138, Feb. 27. 4] R. U. Nabar, Signaling for general IO channels, Ph.D. dissertation, Stanford University, 23. 5]. K. Simon and. S. Alouini, Digital Communications over Generalized Fading Channels: A Unified Approach to the Performance Analysis. Wiley & Sons, Inc., 2.