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<strong>Exact</strong> <strong>Per<strong>for</strong>mance</strong> <strong>of</strong> <strong>Wireless</strong> <strong>Multihop</strong><br />

<strong>Transmission</strong> <strong>for</strong> M-<strong>ary</strong> Coherent Modulations<br />

over Generalized Gamma Fading Channels<br />

Ferkan YILMAZ 1-2 and Oğuz KUCUR 1<br />

Electronics Engineering Dept., Gebze Institute <strong>of</strong> Technology, P.K. 141, 41400, Gebze-Kocaeli, Turkey 1<br />

Source<br />

Terminal<br />

Vodafone IT, ITU Teknokent, ARI 2 Binasi, B Blok/1, 34467, Maslak-Istanbul, Turkey 2<br />

Abstract—Closed-<strong>for</strong>m moment generation function (MGF)<br />

expressions <strong>for</strong> the harmonic mean <strong>of</strong> N independent and not<br />

identically distributed generalized gamma random variables<br />

(RVs) are presented and some well known special cases are<br />

accentuated. The statistical results are also applied in order to<br />

obtain exact symbol error rate (SER) per<strong>for</strong>mance <strong>of</strong> wireless<br />

multihop transmission with non-regenerative relays and M-<strong>ary</strong><br />

coherent modulations over generalized gamma flat fading<br />

channels.<br />

Index Terms—Symbol error rate (SER), harmonic mean,<br />

moment generating function (MGF), multihop transmission,<br />

cooperative/collaborative diversity, generalized gamma fading.<br />

M<br />

I. INTRODUCTION<br />

ULTIHOP relaying technology in which two<br />

terminals are communicating with each other via<br />

relaying terminals [1], [2] is an inspiring and expected<br />

solution <strong>for</strong> such quality requirements as throughput, high<br />

data-rate and coverage in bent pipe satellites and microwave<br />

links, as well as ad-hoc wireless, future cellular (4G and<br />

5G), WLAN, hybrid wireless communication systems [3]<br />

without the need to employ large power at the transmitter,<br />

and to reduce deeply fading or shadowing effects through<br />

spatial repetition [4]-[6]. The concept <strong>of</strong> wireless multihop<br />

transmission is also encountered in cooperative and<br />

collaborative wireless communications [7]. In multihop<br />

transmission, when the direct link between source and<br />

destination terminals is deeply faded, the signal from source<br />

terminal to the destination terminal propagates through the<br />

terminals between them, each <strong>of</strong> which relays a signal<br />

received from the previous terminal to the next terminal in<br />

series as shown in Figure 1. Generally, there exist two types<br />

<strong>of</strong> such relays. If each relaying terminal in multihop<br />

transmission just amplifies and re-transmits the in<strong>for</strong>mation<br />

signal recovered from previous relaying terminal, it is called<br />

non-regenerative, while relaying terminals decodes the<br />

E-mail: ferkan.yilmaz@{vodafone, gmail}.com, okucur@gyte.edu.tr<br />

Relaying<br />

Terminal<br />

Relaying<br />

Terminal<br />

signal and then transmits the detected version to the next<br />

node, it is called regenerative.<br />

There exist a few published papers concerning wireless<br />

multihop transmission. An analysis <strong>for</strong> the per<strong>for</strong>mance <strong>of</strong><br />

wireless dual-hop transmission with non-regenerative relays,<br />

operating over independent but not necessarily identically<br />

distributed (i.d.) Nakagami-m fading channels, is presented<br />

in [8] by Zogas et.al. and Hasna and Alouini put <strong>for</strong>ward the<br />

outage and the error per<strong>for</strong>mance <strong>of</strong> wireless dual-hop<br />

transmission with regenerative and non-regenerative relays<br />

over Rayleigh [9] and Nakagami-m [10] fading channels<br />

[11]. In addition, Karagiannidis et. al. employed the<br />

geometric mean approximation <strong>of</strong> harmonic mean in order<br />

to produce upper per<strong>for</strong>mance limit <strong>of</strong> wireless N-hop<br />

transmission with fixed gain relays 2 over<br />

Nakagami-m and Ricean fading channels [8]. To the best <strong>of</strong><br />

our knowledge, the exact per<strong>for</strong>mance <strong>of</strong> wireless multihop<br />

transmission has not been investigated not only <strong>for</strong> the case<br />

<strong>of</strong> more than one relaying terminals but also <strong>for</strong> generalized<br />

gamma fading channels.<br />

In this paper, we focus on N-hops 2 transmission<br />

with non-regenerative relays and obtain end-to-end<br />

per<strong>for</strong>mance <strong>for</strong> coherent M-<strong>ary</strong> modulation schemes over<br />

independent, not necessarily identical, generalized gamma<br />

fading channels. The main contribution <strong>of</strong> this paper is to<br />

derive closed <strong>for</strong>m expressions <strong>for</strong> moment generating<br />

function (MGF) <strong>of</strong> normalized harmonic mean <strong>of</strong> N<br />

generalized gamma (GG3) random variables (RVs) since<br />

end-to-end per<strong>for</strong>mance in multihop transmission is<br />

connected with the normalized harmonic mean <strong>of</strong> signal-tonoise<br />

ratios (SNR) <strong>of</strong> relaying / hop links (as it is explained<br />

in Section II). Besides, other such statistical measures as<br />

probability density function (PDF), cumulative distribution<br />

function (CDF) can be obtained easily through the medium<br />

<strong>of</strong> employing the linear trans<strong>for</strong>mations, derivations and<br />

linear algebraic manipulations <strong>of</strong> MGF. Eventually, the endto-end<br />

exact per<strong>for</strong>mance <strong>of</strong> wireless multihop transmission<br />

Relaying<br />

Terminal<br />

Figure 1. <strong>Wireless</strong> multihop communication where S communicates with the destination terminal D<br />

through 1 relaying terminals, , ,…, .<br />

978-1-4244-2644-7/08/$25.00 © 2008 IEEE<br />

Destination<br />

Terminal


over generalized gamma fading channels is obtained.<br />

The remainder <strong>of</strong> this paper is organized as follows:<br />

Section II introduces wireless multihop transmission and the<br />

fading channel models. Section III presents MGF <strong>of</strong><br />

normalized harmonic mean <strong>of</strong> N independent GG3 RVs and<br />

the obtained results are accentuated <strong>for</strong> such well known<br />

special cases as single-hop and dual-hop transmissions in<br />

literature. Upon applying the obtained results, the end-toend<br />

per<strong>for</strong>mance <strong>of</strong> wireless multihop transmission with<br />

nonregenerative relays is evaluated in Section IV. Finally,<br />

Section V summarizes the main results <strong>of</strong> the paper.<br />

II. MULTIHOP TRANSMISSION<br />

Consider a multihop (N-hop) wireless transmission as<br />

shown in Figure 1, which operates over independent and not<br />

identically distributed GG3 fading channels, the source<br />

terminal S and destination terminal D are too far apart <strong>for</strong> a<br />

single link within the sight <strong>of</strong> power constraints and channel<br />

fading effects. However, they can be connected using<br />

multiple wireless links arranged in an end-to-end<br />

configuration such that the source terminal S communicates<br />

with the destination terminal D through 1 relaying<br />

terminals ,,…,. Clearly, these terminals relay the<br />

in<strong>for</strong>mation signal only from one hop to the next, acting as<br />

nonregenerative relays. All relaying terminals concurrently<br />

receive and transmit in the same frequency band, and no<br />

latency is incurred in the whole chain <strong>of</strong> relaying<br />

transmissions and there is no wireless multihop diversity.<br />

Assume that the source terminal S transmits a signal ,<br />

which has an average power normalized to one, to the<br />

destination terminal D through relaying terminals. The<br />

received signal at the first terminal can be written as<br />

, (1)<br />

where is the fading amplitude <strong>of</strong> the channel between<br />

source terminal S and the first relaying terminal and<br />

, is an additive white Gaussian noise (AWGN) signal<br />

with one sided power spectral density, ,. After the<br />

received signal at the first terminal is multiplied with which is the gain, it is retransmitted to the next relaying<br />

terminal (the second relaying terminal) . The received<br />

signal at the second relaying terminal can be written as<br />

, , (2)<br />

where is the fading amplitude <strong>of</strong> the channel between the<br />

first relaying terminal and the second relaying terminal<br />

and , is an AWGN signal with one sided power<br />

spectral density, ,. In the same manner, the received<br />

signal at the second terminal is multiplied with and<br />

retransmitted to the next terminal (the third relaying<br />

terminal) . The received signal at the third relaying<br />

terminal can be written as<br />

<br />

(3)<br />

, , , where is the fading amplitude <strong>of</strong> the channel between the<br />

second relaying terminal and the third relaying terminal<br />

and , is an AWGN signal with one sided power<br />

spectral density, ,. Finally, at the end <strong>of</strong> whole chain <strong>of</strong><br />

relaying transmissions, the received signal at the destination<br />

terminal D can be given as [3]<br />

<br />

, <br />

<br />

<br />

<br />

<br />

with 1. Then, it is straight<strong>for</strong>ward that the end-to-end<br />

signal-to-noise ratio (SNR), i.e., the SNR at destination<br />

terminal D, can be written as [4]<br />

<br />

(4)<br />

<br />

<br />

, <br />

(5)<br />

<br />

<br />

<br />

<br />

<br />

It is clear from (5) that the choice <strong>of</strong> the relay gain<br />

determines the equivalent SNR between source and<br />

destination terminals. One choice <strong>for</strong> the gain is [4]<br />

1⁄ <br />

(6)<br />

where the relay just amplifies the incoming signal with the<br />

inverse <strong>of</strong> the channel fading amplitude <strong>of</strong> the previous hop,<br />

regardless <strong>of</strong> the noise <strong>of</strong> that hop. As mentioned in [4],<br />

such a relaying technique serves as a benchmark <strong>for</strong> all<br />

practical multihop systems employing non-regenerative<br />

relays. By applying (6) into (5), the end-to-end<br />

instantaneous SNR (the instantaneous SNR at destination<br />

terminal D) becomes<br />

1<br />

<br />

1<br />

<br />

1<br />

<br />

<br />

1<br />

(7)<br />

where the instantaneous SNRs , 1,2,…, are given as<br />

,<br />

(8)<br />

Here, the amplitude fading , 1,2,…, <strong>of</strong> relays in<br />

wireless multihop transmission are modeled as GG3 fading<br />

[12]. Consequently, the PDF <strong>of</strong> instantaneous SNRs <strong>of</strong> hops,<br />

, can be expressed as follows<br />

Γ <br />

<br />

Ω exp <br />

<br />

Ω (9)<br />

over 0 ∞, where Γ 1⁄ ⁄ Γ and<br />

1⁄ 2,<br />

0 are such two parameters as the fading<br />

parameter, the shape parameter, respectively, related to<br />

fading severity. Ω is the power-scaling parameter <strong>of</strong> the<br />

random variable, defined as Ω , with . <br />

denoting expectation operator. Additionally, GG3 fading<br />

model covers a wide range <strong>of</strong> fading conditions <strong>for</strong> different<br />

shape parameter and fading figure values. Such commonly<br />

employed fading models in literature as the Rayleigh <br />

ξ1, Nakagami-m ξ 1, Weibull 1, lognormal<br />

∞,ξ0, and AWGN ∞,ξ1 are special<br />

or limiting cases <strong>of</strong> the generalized gamma distribution.<br />

Ricean fading can also be closely approximated by<br />

generalized gamma fading if the shape parameter ξ1 and<br />

the relationship 21⁄ 2 1 between the


Ricean factor κ and the fading figure, m exists. As a step<br />

<strong>for</strong>ward, using definition <strong>of</strong> MGF / (one-sided) Laplace<br />

trans<strong>for</strong>m given as<br />

|,,Ω <br />

| , ,Ω <br />

<br />

(10)<br />

where · | is the Laplace trans<strong>for</strong>mation operator<br />

with respect to x and exploiting Mellin-Barnes integral, we<br />

can easily derive Moment Generating Function (MGF) as<br />

follows<br />

, Ω H, <br />

1 , 1<br />

<br />

,0<br />

(11)<br />

0,1<br />

,<br />

where H, ·, ,,, is Fox’s H function defined<br />

in [13], [14].<br />

III. STATISTICAL BACKGROUND<br />

In order to study important statistical metrics <strong>of</strong> the end-toend<br />

SNR, MGF <strong>of</strong> the normalized harmonic mean <strong>of</strong> the<br />

GG3 RVs given in (7) can be given as follows<br />

<br />

<br />

<br />

<br />

1⁄ 1⁄ 1⁄ <br />

<br />

|,, Ω … <br />

(12)<br />

After algebraic manipulations based Mellin-Barnes integrals<br />

and Fox’s H functions [14], we have obtained exact MGF <strong>of</strong><br />

the end-to-end SNR <strong>for</strong> wireless multihop transmission as<br />

follows<br />

<br />

2√H ,<br />

where H is defined as<br />

<br />

<br />

, Δ,∞ H, H, <br />

Δ1,1, Δ, <br />

<br />

<br />

Ω <br />

, Δ,∞ H, <br />

Δ0,1, Δ, <br />

<br />

<br />

Ω <br />

(13)<br />

(14)<br />

where Δ, and are the parameters <strong>of</strong> Fox’s H<br />

function defined as<br />

1<br />

Δ, ,<br />

<br />

1<br />

(15)<br />

<br />

<br />

<br />

<br />

Ω <br />

<br />

(16)<br />

Finally, let us consider some special cases in order to check<br />

analytical simplicity and accuracy:<br />

A. Special Case I (Single-hop special case): Most <strong>of</strong> the<br />

investigated communications systems in literature are based<br />

on single-hop, which is the special case <strong>of</strong> wireless multihop<br />

transmission such that there is no relaying terminal in the<br />

transmission (total number <strong>of</strong> hops 1). Besides, most <strong>of</strong><br />

the results <strong>for</strong> single-hop communications systems are given<br />

<strong>for</strong> Nakagami-m fading channels. Then, we can simplify<br />

MGF given in (13) <strong>for</strong> single-hop Nakagami-m <br />

0.5, 1 fading channels as follows<br />

<br />

ΩΓ <br />

, <br />

2√H, <br />

Ω <br />

<br />

0,1, 1,1 <br />

<br />

(17)<br />

<br />

Using Fox’s H function equality [13, eq. (2.9.19)],<br />

, <br />

H, <br />

4 <br />

<br />

<br />

2<br />

,1 , <br />

2<br />

,1 2<br />

2 <br />

<br />

, (18)<br />

where , and is the nth-order modified Bessel<br />

function <strong>of</strong> second kind, we simplify the MGF as<br />

2<br />

Γ <br />

Ω <br />

<br />

<br />

<br />

<br />

2√ 2 <br />

Ω <br />

<br />

(19)<br />

<br />

Then, substituting the integral equality [15, eq. (3.16.11.7)]<br />

into (19) gives MGF <strong>for</strong> Nakagami-m fading channels as<br />

follows<br />

1 Ω<br />

<br />

<br />

(20)<br />

which is well-known in literature [16, eq. (5.15)], [17].<br />

B. Special Case II (Balanced double-hop special case): For<br />

the case in which there is one relaying terminal in the<br />

transmission 2, we can simplify MGF given in (13)<br />

<strong>for</strong> Nakagami-m 0.5, 1<br />

fading channels as follows<br />

2<br />

ΩΓ 2√ <br />

<br />

<br />

, <br />

H, <br />

Ω <br />

<br />

1<br />

2 ,1,1<br />

2 ,1<br />

, <br />

H, <br />

Ω <br />

<br />

1<br />

2 ,1,1<br />

2 ,1<br />

(21)<br />

in which replacing Fox’s H equality given in (18) gives<br />

<br />

<br />

<br />

<br />

8<br />

Γ <br />

Ω <br />

2√<br />

<br />

<br />

2 <br />

Ω 2 <br />

Ω <br />

(22)<br />

Finally, upon employing [15, eq. (8.4.23.29)], MGF <strong>for</strong><br />

Nakagami-m fading channels is obtained as follows<br />

, 2; 1 Ω<br />

;<br />

2 4 <br />

(23)<br />

which has been already proposed in [10, eq. (5)], where<br />

·,·;·;· is the Gauss’ hypergeometric function defined in<br />

[18, eq.(15.1.1)]. If the fading figure 1 (i.e. it is the<br />

balanced double-hop transmission over Rayleigh fading<br />

channels), then (23) reduces into [9, eq. (21)].


C. Special Case III (Balanced triple-hop special case): For<br />

the case in which there exists two relaying terminals in<br />

transmission (total number <strong>of</strong> hops is 3), we can easily<br />

simplify MGF given in (13) <strong>for</strong> Nakagami-m <br />

0.5, 1 fading channels as<br />

follows<br />

<br />

<br />

24<br />

Γ <br />

Ω <br />

<br />

<br />

2√ 2<br />

<br />

<br />

Ω 2 <br />

Ω <br />

(24)<br />

This integral can be easily taken by means <strong>of</strong> substituting<br />

power series <strong>of</strong> Bessel functions into (24). Then, the MGF,<br />

having not proposed in literature yet, is obtained as follows<br />

3√<br />

<br />

2 <br />

Γ 1<br />

<br />

<br />

Ω<br />

<br />

<br />

∞<br />

<br />

! !<br />

<br />

<br />

,<br />

G, 4 <br />

23<br />

,<br />

3<br />

133<br />

3<br />

, 6 1<br />

6<br />

2 3 2<br />

3<br />

,<br />

3<br />

, 6 2<br />

(25)<br />

<br />

3<br />

,<br />

where G, ·, ,,, is the MeijerG function<br />

defined in [19, eq. (9.301)]. However, this obtained MGF<br />

has singularity while expressing per<strong>for</strong>mance expression <strong>for</strong><br />

M-PSK modulation schemes. In order to avoid this problem,<br />

we can apply Laguerre Trans<strong>for</strong>mation [20] onto MGF.<br />

Consequently, we obtain the MGF as follows<br />

3√<br />

<br />

2 <br />

Γ <br />

<br />

Ω Ω<br />

<br />

<br />

∞<br />

L (26)<br />

!<br />

<br />

where L is defined as<br />

L 1 <br />

<br />

,<br />

G, 4 <br />

!<br />

23<br />

,<br />

3<br />

133<br />

3<br />

, 6 1<br />

6<br />

2 3 2<br />

3<br />

,<br />

3<br />

, 6 2<br />

<br />

(27)<br />

<br />

3<br />

D. Special Case IV (Balanced N-hop special case): For the<br />

case that there are 1 relaying terminals in the system,<br />

(the total number <strong>of</strong> hops is ), we can simplify MGF <strong>for</strong><br />

Nakagami-m 0.5, 1 fading channels, which has not<br />

proposed in literature yet, as follows<br />

2<br />

Γ <br />

Ω <br />

∞<br />

<br />

2√ <br />

<br />

2 <br />

Ω 2 <br />

Ω <br />

(28)<br />

MGF <strong>for</strong> different hop counts is depicted in Figure 2 by<br />

means <strong>of</strong> using (28). If the total number <strong>of</strong> relaying<br />

terminals in transmission goes to infinity ∞, the<br />

MGF becomes<br />

lim<br />

∞ 1, 0<br />

0, (29)<br />

which means that the per<strong>for</strong>mance <strong>of</strong> wireless multihop (Nhop)<br />

transmission deteriorates when increases, i.e., lower<br />

limit symbol error rate (SER) per<strong>for</strong>mance <strong>of</strong> wireless<br />

multihop transmission <strong>for</strong> M-PSK signaling is ⁄ 1<br />

error/symbol, where is the modulation level, <strong>for</strong> DPSK /<br />

BPSK is 0.5 error/symbol. As a result, total number <strong>of</strong> hops<br />

is limited with respect to the desired per<strong>for</strong>mance and<br />

coverage.<br />

Figure 2. The variation <strong>of</strong> MGF <strong>for</strong> different hop counts (fading figures<br />

, 2, shaping parameters , 1 and average powers , Ω <br />

1 , 1,2, … , )<br />

IV. PERFORMANCE EVALUATION<br />

Having the MGF <strong>of</strong> the end-to-end instantaneous SNR, and employing the MGF-based approach <strong>for</strong> the<br />

per<strong>for</strong>mance evaluation <strong>of</strong> digital modulations over fading<br />

channels [16], the obtained MGF result in (13) enables us to<br />

obtain SER per<strong>for</strong>mance <strong>for</strong> various M-<strong>ary</strong> modulations<br />

[such as M-<strong>ary</strong> phase shift keying (MPSK), M-<strong>ary</strong><br />

differential phase shift keying (MDPSK), and M-<strong>ary</strong><br />

quadrature amplitude modulation (MQAM)] as follows<br />

<br />

<br />

<br />

V 2Λ (30)<br />

<br />

where , , , V, Λ and are the per<strong>for</strong>mance<br />

parameters <strong>for</strong> M-<strong>ary</strong> modulation which are given in Table<br />

I. For instance, the per<strong>for</strong>mance expression <strong>for</strong> coherent<br />

MDPSK modulations is easily reduced to [16]<br />

<br />

<br />

2<br />

<br />

2 <br />

<br />

1 <br />

<br />

2 <br />

<br />

(31)<br />

<br />

In literature, the most <strong>of</strong> the per<strong>for</strong>mance results<br />

concerning wireless multihop transmission are given <strong>for</strong><br />

bin<strong>ary</strong> DPSK (BDPSK). On account <strong>of</strong> that, Figure 3<br />

compares the bit error rate (BER) per<strong>for</strong>mances <strong>of</strong> wireless<br />

multihop transmission with non-regenerative relays and<br />

DPSK modulation <strong>for</strong> different hop counts. Similar to the<br />

MGF results obtained from Figure 2, it is clear that the<br />

number <strong>of</strong> hops increases then the per<strong>for</strong>mance deteriorates.<br />

There<strong>for</strong>e, total number <strong>of</strong> hops in transmission is limited<br />

with respect to the desired per<strong>for</strong>mance and coverage under


TABLE I<br />

PARAMETERS FOR SPECIFIC MODULATIONS<br />

M-<strong>ary</strong><br />

Modulation<br />

Schemes<br />

V Λ MPSK 1<br />

MDPSK 1<br />

MQAM 2<br />

MPAM 1<br />

1<br />

<br />

2<br />

<br />

4√ 4<br />

√<br />

44√<br />

√<br />

2 2<br />

<br />

1<br />

0 <br />

2<br />

<br />

<br />

1 <br />

<br />

0 1<br />

2<br />

0 1<br />

2<br />

0 1<br />

2<br />

the assumption that there is no multihop diversity in the<br />

transmission. Besides, if the fading figure increases (i.e.<br />

the channel fading conditions improve), the per<strong>for</strong>mance <strong>of</strong><br />

wireless multihop transmission with nonregenerative relays<br />

will converge to the per<strong>for</strong>mance <strong>of</strong> BDPSK over AWGN<br />

channels.<br />

Figure 3. BER per<strong>for</strong>mance <strong>of</strong> wireless multihop transmission with nonregenerative<br />

relays (fading figures , 1,2, shaping parameters<br />

, 1, 1,2, … , ).<br />

V. CONCLUSION<br />

<br />

<br />

<br />

<br />

<br />

<br />

3⁄ 2<br />

1<br />

3⁄ 2<br />

1<br />

3<br />

1<br />

The parameters <strong>for</strong> such common coherent modulations as M-<strong>ary</strong> phase shift<br />

keying (MPSK), M-<strong>ary</strong> differential phase shift keying (MDPSK), M-<strong>ary</strong> square<br />

quadrature amplitude modulation (MQAM) with and even, M-<strong>ary</strong> pulse amplitude<br />

modulation (MPAM).<br />

In this paper, we presented not only the exact and<br />

generalized per<strong>for</strong>mance <strong>of</strong> wireless multihop (N-hop)<br />

transmission 2 with nonregenerative relays <strong>for</strong> M-<strong>ary</strong><br />

modulations over generalized gamma (GG3) fading<br />

channels but also the MGF <strong>of</strong> the normalized harmonic<br />

mean <strong>of</strong> N GG3 random variables by means <strong>of</strong> Mellin-<br />

Barnes integrals and Fox’s H functions. Such special cases<br />

<strong>of</strong> multihop transmission as single-hop, balanced doublehop,<br />

balanced triple-hop and balanced N-hop are<br />

accentuated <strong>for</strong> Nakagami-m and Rayleigh fading channels.<br />

<br />

2<br />

<br />

4<br />

<br />

2<br />

Furthermore, the exact generalized per<strong>for</strong>mance expression<br />

is presented <strong>for</strong> M-<strong>ary</strong> modulation schemes and the<br />

per<strong>for</strong>mance <strong>for</strong> BDPSK modulation is depicted on the<br />

purpose <strong>of</strong> comparing the obtained results <strong>for</strong> wireless<br />

double-hop transmission with the literature. Besides, it is<br />

shown that there is a threshold between number <strong>of</strong> hops and<br />

the desired per<strong>for</strong>mance and coverage when there is no<br />

multihop diversity in the transmission.<br />

[1]<br />

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