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PERFORMANCE ANALYSIS OF MRC-CHIRP SYSTEM OVER INDEPENDENTAND CORRELATED FADING CHANNELS
Muhammad Ajmal Khan, Raveendra K. Rao, Xianbin Wang
Department of Electrical and Computer EngineeringWestern University, London, Ontario, Canada, N6A 5B9.
ABSTRACT
In this paper, chirp modulation is proposed to employ in Max-imal Ratio Combining (MRC) diversity, referred to as MRC-Chirp system. Moment generating function (MGF) approachis used to derive easy-to-compute expressions for average biterror probability (ABEP) for two fading situations. Firstly,independent fadings with Rayleigh and Nakagami-π statis-tics are considered. Next, an exponentially correlated fadingenvironment with Nakagami-π statistics is considered. TheABEP performance of the proposed system is illustrated usinganalytical expressions and using extensive Monte Carlo simu-lations. Numerical results show close agreement of analyticalwork with those of simulations. A discussion of numerical re-sults on the performance of MRC-Chirp system as a functionof diversity order πΏ, chirp modulation parameters, and fadingparameters is presented.
Index Termsβ MRC diversity, chirp modulation, Naka-gami-π fading, independent fading, correlated fading.
1. INTRODUCTION
Chirp signals, also known as linear frequency-modulated sig-nals, have been widely used in radar and sonar applications.These signals are robust to multipath interference and can re-alize higher processing gains and have been used in wirelesscommunications to improve the performance due to its anti-jamming characteristic [1]. Chirp signals have also been usedin various other applications such as combating multipath in-terference [2], spread spectrum techniques [3], multiple-accessschemes [4], equalization [5], and channel estimation [6].
Although the error performance of linear modulation sch-emes such as PSK, QAM, etc. has been extensively analyzedin independent [7] and correlated fading channels with MRCdiversity reception [8], there is hardly any work in the lit-erature devoted to the chirp modulation particularly in cor-related fading channels. In [9], authors mainly focused onchannel estimation using chirp signals and briefly discussedorthogonal chirp signals in multipath diversity using com-puter simulations only. In [10], authors suggested two RAKEreceiver architectures for chirp spread spectrum system and
evaluated performance using computer simulations. It is im-portant to understand the bit error probability performance ofchirp modulation in diversity reception as well as in correlatedfading channels. In this paper, we propose and analyze a wire-less communication system using chirp modulation scheme inconjunction with Maximal Ratio Combining (MRC) diversity.The main contribution of the paper are: (i) derivation of errorprobability performance of MRC-Chirp system using MGFapproach under independent Rayleigh and Nakagami-π sta-tistical channels, (ii) analysis of MRC-Chirp system in ex-ponentially correlated Nakagami-π fading channel, and (iii)validation of the ABEP through Monte Carlo simulations.
The paper is organized as follows: Section 2 describes theproposed MRC-Chirp system, followed by theoretical perfor-mance analysis of the system over fading channels in Section3. Sections 4 and 5 present performance analysis in indepen-dent and correlated fading channels, respectively. Numericalresults are presented in Section 6 and the paper is concludedin Section 7.
2. MRC-CHIRP SYSTEM MODEL
Input
Data
Chirp
Modulator
+
s(t)
+
h1(t)
+
h2(t)
+
hL(t)
+
+
n1(t)
n2(t)
nL(t)
r1(t)
r2(t)
rL(t)
MRC-Chirp
Receiver
Output
DataDecision
Fig. 1: MRC-Chirp Communication System.
The proposed MRC-chirp communication system with πΏfading paths for coherent detection is shown in Fig. 1. The in-put data is assumed to be a sequence of binary digits from anequally likely and statistically independent data source. Thisdata is then passed through the chirp modulator that mapseach π-bit chunk to one of the π = 2π waveforms, i.e. π π(π‘),where π = 1, 2, 3, ...,π . Mathematically, chirp modulated
2013 26th IEEE Canadian Conference Of Electrical And Computer Engineering (CCECE)
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signal is represented by
π π(π‘) =
β2πΈπ
πcos [2ππππ‘+ πππ(π‘) + π0] , 0 β€ π‘ β€ π (1)
where πΈπ is the energy of symbol over the duration of π , ππis the carrier frequency, π0 is the starting phase of the carriersignal at π‘ = 0, and ππ is the information data taking one ofthe values Β±1, Β±3, Β±5, ...,Β±(π β 1) and π = 2, 4, 8, ....The phase function π(π‘) is given by
π(π‘) =
β§β¨β©0 , π‘ β€ 0, π‘ > π
π{β(
π‘π
)β π€(
π‘π
)2}, 0 β€ π‘ β€ π
π(ββ π€) = ππ , π‘ = π
(2)
where the parameters β and π€ represent the peak-to-peak fre-quency deviation divided by the symbol rate, and the fre-quency sweep width divided by the symbol rate, respectively.Since π = ββπ€, the pair π and π€, (π, π€), represents the set ofindependent modulation parameters. The optimized values ofπ and π€ (π = 0.28, π€ = 1.85) [11] are used for binary chirpmodulation throughout this paper for illustration of numericalresults.
In the proposed MRC-Chirp system, the signal π (π‘) istransmitted over πΏ independent channels, where each channelhas an impulse response of βπ(π‘) = πΌππ
βππππΏ(π‘ β ππ). Eachreplica of the signal is perturbed by the additive white Gaus-sian noise (AWGN) π(π‘) with zero-mean and power spectraldensity (PSD) π0/2. We assume AWGN to be statisticallyindependent from channel to channel and independent of thefading amplitude. The received signal at πth branch can bewritten as
ππ(π‘) = πΌππβππππ (π‘β ππ) + ππ(π‘), π = 1, 2, ..., πΏ (3)
where π is the branch index, and πΌ, π and π are the randomchannel amplitude, phase and delay, respectively. In this pa-per, slow fading is assumed, so πΌ, π and π are all constantover a symbol period. The perfect knowledge of the chan-nel state information (CSI) is also assumed to be available atthe receiver but transmitter has no information of the channel.At the receiver, each received replica of the signal is passedthrough the correlators and combined at the MRC and thendecision is made based on the amplitude output of each com-biner branch.
3. ANALYSIS OF MRC-CHIRP SYSTEM
In this paper, we consider binary case (π = 2) for our pro-posed MRC-Chirp system and derive the average bit errorprobability (ABEP) ππ(π) over a generalized fading channelin this section. The instantaneous signal-to-noise ratio (SNR)per bit per path for binary chirp modulation is defined by [11]
πΎπ =πΌ2ππΈπ
ππ(1β πππ) (4)
where πππ is the normalized cross-correlation coefficient be-tween the chirp signals and is given by [11].
πππ =cos(Ξ©)β2ππ€
[C(π₯+)βC(π₯β)]+sin(Ξ©)β2ππ€
[S(π₯+)β S(π₯β)]
where π₯+ =β
π2π€βπβ
π€, π₯β = β
βπ2π€+πβ
π€, Ξ© = π
4 π(π+π€)2
π€ ,
π = β£ππ βππβ£, ππ and ππ are data symbols Β±1,Β±3, ...,Β±(π β1), and C(β ) and S(β ) are the standard Fresnel cosine and sineintegrals respectively and are given by
C(π₯) =
β« π₯
0
cos
(ππ‘2
2
)ππ‘, S(π₯) =
β« π₯
0
sin
(ππ‘2
2
)ππ‘
Now, the total conditional SNR per bit πΎπ‘ at the output ofthe MRC combiner for equally likely transmitted data is ex-pressed as
πΎπ‘ =
πΏβπ=1
πΎπ (5)
The conditional BEP ππ(πβ£{πΎπ}πΏπ=1) (i-e. BEP over AWGNchannel) of binary chirp modulation is given by [11]
ππ(πβ£{πΎπ}πΏπ=1) = π (βπΎπ‘) (6)
where π(β ) is the Gaussian Q-function defined by
π(π₯) =1β2π
β« β
π₯
πβπ‘2/2ππ‘ (7)
For mathematical analysis, the alternate form of π(β ) is moreconvenient and is given by [12]
π(π₯) =1
π
β« π/2
0
exp
(β π₯2
2 sin2 π
)ππ (8)
Using (8) in (6), the conditional BEP (6) can be written as
ππ(πβ£{πΎπ}πΏπ=1) =1
π
β« π/2
0
exp
(β πΎπ‘
2 sin2 π
)ππ (9)
Using (5), the conditional BEP (9) can be expressed as
ππ(πβ£{πΎπ}πΏπ=1) =1
π
β« π/2
0
πΏβπ=1
exp
(β πΎπ
2 sin2 π
)ππ (10)
The ABEP ππ(π) of the proposed MRC-Chirp system is ob-tained by averaging conditional BEP ππ(πβ£{πΎπ}πΏπ=1) over thejoint PDF of the instantaneous SNR sequence ππΎ1,πΎ2,...,πΎπΏ
(alsoequal to
βπΏπ=1 ππΎπ
(πΎπ) for independent identically distributedpaths), hence
ππ(π) =
β« β
0
β« β
0
...
β« β
0
ππ({πΎπ}πΏπ=1)πΏβ
π=1
ππΎπ(πΎπ)ππΎ1ππΎ2...ππΎπΏ
ππ(π) =
β« β
0
β« β
0
...
β« β
0
1
π
β« π/2
0
πΏβπ=1
exp(β πΎπ2 sin2 π
)
β ππΎπ(πΎπ)ππΎ1ππΎ2...ππΎπΏ
(11)
The moment generating function (MGF) β³πΎ of SNR per bitfor πth path is defined by [7]
β³πΎπββ« β
0
ππΎπ(πΎπ)π
π πΎπππΎπ (12)
Therefore, ABEP of binary chirp modulation with MRC di-versity of πΏ-paths over a generalized fading channel can bewritten as
ππ(π) =1
π
β« π/2
0
πΏβπ=1
β³πΎπ
(β 1
2 sin2 π
)ππ (13)
The MGF of Rayleigh fading channel is given by [7]
β³πΎπ(π ) = (1β π πΎπ)
β1 (14)
The MGF of Nakagami-π fading channel is given by [7]
β³πΎπ(π ) =
(1β π πΎπ
π
)βπ
(15)
4. ANALYSIS IN INDEPENDENT FADING
In this section, we consider the case of independent identi-cally distributed fading with the same average SNR per bit πΎfor all πΏ channels, hence (13) can be written as
ππ(π) =1
π
β« π/2
0
(β³πΎ
(β 1
2 sin2 π
))πΏ
ππ (16)
Using (14), ABEP (16) over Rayleigh fading channel is givenby
ππ(π) =1
π
β« π/2
0
(sin2 π
sin2 π + πΎ/2
)πΏ
ππ (17)
Integrating using [13], ABEP of binary chirp modulation inMRC diversity of πΏ-paths over Rayleigh fading channel isexpressed as
ππ(π) = (ππΎ)πΏ
πΏβ1βπ=0
(πΏβ 1 + π
π
)[1βππΎ ]
π (18)
where
ππΎ =1
2
(1β
βπΎ
2 + πΎ
)(19)
Similarly, using (15) and integrating using [13], we can haveABEP of binary chirp modulation in MRC diversity of πΏ-paths over Nakagami-π fading channel as
ππ(π) = (β¬πΎ)ππΏ
ππΏβ1βπ=0
(ππΏβ 1 + π
π
)[1β β¬πΎ ]
π (20)
where
β¬πΎ =1
2
(1β
βπΎ
2π+ πΎ
)(21)
When π = 1, (20) becomes (18), it is evident that ABEPunder Nakagami-π is identical to under Rayleigh fading.
5. ANALYSIS IN CORRELATED FADING
Generally, diversity branches are assumed to be independentof one another, but it is not the case in real-world situationsdue to antenna spacing particularly [14]. Thus, correlationalways exists among diversity branches and various channelcorrelation models have been proposed in the literature. Oneof the commonly used model is Exponential correlation model,which is proposed by Aalo [14] for identically distributedNakagami-π channels and is represented by the followingMGF [7]
β³(π ) =
(1β π ππ πΎ
ππΏ
)βππΏ2/ππ
(22)
where [14]
ππ = πΏ+2βπ
1ββπ
(πΏβ 1β ππΏ/2
1ββπ
)(23)
πππ =cov
(π2π , π
2π
)β
var(π2π )var(π2π ), π, π = 1, 2, ..., πΏ (24)
Using (22) in (13), we obtain ABEP of binary chirp modula-tion in MRC diversity over exponentially correlated Nakagami-π fading channel as
ππ(π) =1
π
β« π/2
0
πΏβπ=1
(sin2 π
sin2 π +πππΎ2ππΏ
)ππΏ2/ππ
ππ (25)
6. NUMERICAL RESULTS
Numerical results of average bit error probability (ABEP) wereobtained using simulations and using analytical expressionsderived in Sections 4 and 5 as a function of average SNR perbit. In both cases, binary chirp modulation in conjunctionwith MRC diversity were considered over Rayleigh/Nakagami-π fading channels for different diversity order πΏ and channelcorrelation parameter π. Numerical results were obtained byMonte Carlo simulation using over 107 samples for informa-tion bits and the generation of the fading envelopes at eachSNR. Coherent detection is assumed in all results as well aschannel state information (CSI) was assumed to be availableat the receiver.
Fig. 2 depicts the error performance of binary chirp mod-ulation in conjunction with MRC diversity for different or-ders πΏ operating over independent and identically distributed(i.i.d.) Rayleigh fading channel. The performance over AWGNchannel is also shown for comparison. From this figure, it isnoted that ABEP decreases with the increase in diversity or-der πΏ.
For example, a fixed ABEP of ππ = 10β5 can be achievedat SNR=45 dB with πΏ = 1, or SNR=25.4 dB with πΏ = 2, orSNR=19.6 dB with πΏ = 3 or SNR=14.6 dB with πΏ = 4. Thus
0 5 10 15 20 25 30 35 40 4510
β6
10β5
10β4
10β3
10β2
10β1
100
Average SNR per bit [dB]
Ave
rag
e B
it E
rro
r P
rob
abili
ty
SimulationAnalytical
L=1
L=2
L=3L=4
AWGN
Fig. 2: Binary MRC-Chirpover Rayleigh Fading Chan-nel.
β10 β5 0 5 10 15 20 25 3010
β6
10β5
10β4
10β3
10β2
10β1
100
Average SNR per Bit [dB]
Ave
rag
e B
it E
rro
r P
rob
abili
ty
SimulationAnalytical
L=1
L=2
L=3
L=4
AWGN
Fig. 3: Binary MRC-Chirpover Nakagami-π FadingChannel (π = 2).
comparing to single antenna system, MRC-Chirp system al-lows an SNR gain of more than 19.6 dB, 25.4 dB and 30.4dB using two, three and four receive antennas, respectively.Also, it is observed from the figure that both simulation andanalytical results are in close agreement.
Error performance over Nakagami-π channel with fadingparameter π = 2 for different πΏ is illustrated in Fig. 3. Itis apparent from this figure that diversity order πΏ providesimprovement in ABEP and the figure also verifies the derivedanalytical results.
The effects of channel correlation in MRC-Chirp systemare shown in Figs. 4 and 5, where ABEP of binary chirpmodulation with diversity orders, πΏ = 3 and πΏ = 5, overan exponential correlation profile across Nakagami-π fadingchannel (π = 1) is represented. From Fig. 5, for a fixedABEP of ππ = 10β5, an SNR loss of 3.6 dB with correla-tion π = 0.5 is noticed as compared to uncorrelated fading.Both figures depict that channel correlation degrades the errorperformance of MRC-Chirp system.
β10 β5 0 5 10 15 20 25 3010
β6
10β5
10β4
10β3
10β2
10β1
100
Average SNR per Bit [dB]
Ave
rag
e B
it E
rro
r P
rob
abili
ty
UncorrelatedΟ = 0.2Ο = 0.5Ο = 0.9
Fig. 4: Binary MRC-Chirpwith πΏ = 3 over CorrelatedNakagami-π Fading Chan-nel (π = 1).
β10 β5 0 5 10 15 20 25 3010
β6
10β5
10β4
10β3
10β2
10β1
100
Average SNR per Bit [dB]
Ave
rag
e B
it E
rro
r P
rob
abili
ty
UncorrelatedΟ = 0.2Ο = 0.5Ο = 0.9
Fig. 5: Binary MRC-Chirpwith πΏ = 5 over CorrelatedNakagami-π Fading Chan-nel (π = 1).
7. CONCLUSIONS
This paper investigated the error performance of MRC-Chirpsystem in independent and correlated fading channels. Theanalysis included both Rayleigh and Nakagami-π fading chan-nels. MGF based approach was employed and error probabil-ity expressions were derived, one of our major contribution
in this paper. Moreover, an SNR gain of more than 30.4 dBwas noticed with the aid of diversity order πΏ = 4 as com-pared to without diversity. Furthermore, exponential channelcorrelation model was employed to examine the error perfor-mance of the MRC-Chirp system in correlated fading and anSNR loss of 3.6 dB with correlation π = 0.5 was observedfor binary chirp modulation with πΏ = 5. It was found that thechannel correlation degrades the performance of MRC-Chirpsystem. Finally, Monte Carlo simulation was carried out andthe simulation results were compared with the obtained ana-lytical results. It is observed that both analytical and simula-tion results compare very well thereby validating the former.This work can be further extended for π -ary chirp modula-tion and the challenge may be in deriving accurate symbolerror probability, one of our future goal.
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