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Bulletin of Electrical Engineering and Informatics
Vol. 10, No. 5, October 2021, pp. 2686∼2695
ISSN: 2302-9285, DOI: 10.11591/eei.v10i5.3015 ❒ 2686
Outage performance of downlink NOMA-aided small cell
network with wireless power transfer
Anh-Tu Le1
, Dinh-Thuan Do2
, Munyaradzi Munochiveyi3
1,2
Faculty of Electronics Technology, Industrial University of Ho Chi Minh City, Vietnam
3
Department of Computer Science and Information Engineering, College of Information and Electrical Engineering, Asia
University, Taiwan
Article Info
Article history:
Received Mar 30, 2021
Revised May 30, 2021
Accepted Jul 28, 2021
Keywords:
Non-orthogonal multiple
access
Outage probability
Power beacon
Small cell network
ABSTRACT
This article considers the outage performance of the downlink transmission for a small
cell network in a heterogeneous network. Due to mobility and distribution of users, it
is necessary to study massive connections and high energy efficiency for such kind of
systems. To be an enabler of energy harvesting, a power beacon is helpful to support
the base station to send signals to distant users, and wireless power transfer (WPT) is
exploited to guarantee the data packets transmission from the power beacon to the base
station. To provide massive connections, we propose a novel non-orthogonal multiple
access (NOMA) technique combined with WPT to enhance outage performance and
latency reduction. Furthermore, we derive outage probability (OP) to characterize the
system performance. Simulation results are verified to match well between theoretical
and analytical methods, and main parameters are determined to understand how they
affect the proposed scheme.
This is an open access article under the CC BY-SA license.
Corresponding Author:
Dinh-Thuan Do
Faculty of Electronics Technology
Industrial University of Ho Chi Minh City
12 Nguyen Van Bao, Go Vap Dist., Ho Chi Minh City, Vietnam
Email: dodinhthuan@iuh.edu.vn
1. INTRODUCTION
To power the enormous number of internet of things (IoT), energy harvesting (EH) of radio frequency
(RF) signals is billed as a promising solution [1]–[3]. In particular, the IoT receivers divide the received signal
into two parts (EH and information processing (IP)). Power splitting (PS) or time switching (TS) are two
commonly used EH architectures [4], [5]. Studies have shown that PS outperforms TS although it is difficult
and inefficient to implement in practice. Recently in [4], [6] and [7], the authors demonstrated how harvested
energy contributes to prolonging the lifetime of IoT systems. Reference [6] considered how to secure harvested
residual energy after every forwarding and receiving cycle. As such, EH is essential for green and sustainable
operation. Also, the authors examined the trade-off between residual harvested energy and the achievable
rate. Differently, we go further in this paper to investigate the rate-energy (R-E) region for achievable rate
and harvested residual energy in a two-way decode-and-forward (DF) relay system with a PS based energy
harvesting relay.
Nowadays, power domain non-orthogonal multiple access (PD-NOMA) has been widely studied by
researchers [8]-[14]. The basic principle of PD-NOMA is that the users can transmit power via non-orthogonal
transmission while the successive interference cancellation (SIC) receiver is employed at the receiver to miti-
Journal homepage: http://beei.org
Bulletin of Electr Eng & Inf ISSN: 2302-9285 ❒ 2687
gate interference [15]-[18]. Further, combining NOMA and cognitive radio (CR) is proposed to offer uninter-
rupted, reliable, and massive connectivity [16]. Do et al. in [16], the problem of relay selection in CR-NOMA
networks when spectrum sharing is operational is considered. As such, the number of accessible secondary
users (SUs) sharing the limited and dynamic spectrum resources is boosted due to the opportunistic access of
the licensed spectrum resources. Zaidi et al. in [17] studied the use of EH to maintain distinguishable levels
of power when the users perform uplink NOMA transmissions. They derived an exact system ergodic average
rate to determine the proposed network performance.
The authors Gong and Chen in [19] considered various energy harvesting methods deployed in NOMA
systems. They studied several protocols such as conventional TS, PS, and hybrid time-switching/power-
splitting (TS/PS) by exploiting a single antenna base station and a single user pair setup. The study in [20]
considered WPT via PS and information transmission in a NOMA system consisting of a single antenna base
station. A full-duplex information transmitter subject to energy-constraints is studied in [21] to enable energy
harvesting from a dedicated energy transmitter while NOMA is employed at the transmitter to communicate
with the receivers. Reference [22] examined the performance of a CR-NOMA enabled wireless information
and power transfer network (WIPT). Motivated by the above analysis, we deploy a power beacon (PB) to a
small cell network in the downlink.
Specifically, to implement IoT relay systems in practice, we analyze TS relaying protocol to facilitate
energy harvesting in NOMA systems with the help of a nearby power beacon. This is beneficial for powering
IoT devices and sensors such as indicators, alarms, and detectors which are used in underground trains, coal
mines, and tunnels. Concerning the large number of IoT nodes in such environments, battery replacement
of the sensor nodes or IoT devices is a staggeringly difficult task since connecting all of them through wired
connections is difficult. Therefore, it is easy to recharge the IoT sensor nodes by deploying NOMA to transmit
data to multiple IoT users. The main benefits of such a proposal is the enhancement of the power consumption,
spectral efficiency and capacity demands in hard to reach environments [23]-[32]. Moreover, power beacons
can be deployed everywhere to enable wireless power charging of the numerous IoT devices and sensors in
these environments. In addition, it is important to provide the performance evaluation of a downlink system
using NOMA when the impact of a power beacon is considered in such environments. It is expected that our
proposed system model can be implemented in several scenarios as discussed to address existing difficulties.
For the proposed model, we consider first the WPT scenario, and then we present the performance
when PB-NOMA is exploited. For such a scenario, we detail comprehensively the outage performances and
derive the exact outage probability expressions. Next, we determine which parameter affects the system per-
formance under the constraints of the base station transmit signal-to-noise ratio (SNR) and harvested energy.
Our contributions are listed is being as:
− We study PB-NOMA by exploiting the TS scheme to determine the downlink performance under the
scheme of linear energy harvesting. NOMA enables the small cell networks to continue their operations
if they can accurately capture enough energy in the phase of the energy harvesting process. To facilitate
any placement of the base station, the design of the PB benefits nearby base stations to serve their users
in the downlink in limited conditions related to power provided by another source.
− We formulate exact outage probability (OP) formulas subject to the constraint of the transmit SNR. We
evaluate outage in some cases to show how PB-NOMA guarantees operation in the downlink.
− Simulation results demonstrate that the performance of the proposed scheme in terms of the OP, can be
improved if the channel parameters, transmit SNR, and power allocation factors are reasonably selected.
The rest of this paper is organized is being as. Section 2 describes the PB-NOMA small cell networks.
In section 3, we consider the scenario of PB-NOMA in terms of outage performance. We provide extensive
numerical simulations in section 4 and section 5 concludes the paper.
2. SIGNAL ANALYSIS AND SYSTEM MODEL
2.1. System model
As can be seen in Figure 1, we consider a small cell network containing an access point (S) which
needs the help of a power beacon (PB) to serve two users (Ui, i ∈ {1, 2}). In this model, the main nodes (S,
PB, and two user Ui) are equipped with single antennas. Further, all channel are assumed to be identically and
independently distributed (i.i.d.) and following Nakagami-m distribution. The signal frame T includes two
time slots, shown in Figure 2. The access point S harvests energy from the beacon in the first time slot (αT/2)
Outage performance of downlink NOMA-aided small cell network with wireless power transfer (Anh-Tu Le)
2688 ❒ ISSN: 2302-9285
while signal processing in the link of S-Ui is conducted in the second time slot ((1 − α)T/2). Table 1 contains
details of the main system parameters.
PB
U1
U2
Energy harvesting
Information Transmission
hS
h1
h2
S
Figure 1. NOMA-aided WPT downlink small cell network
EH at S S to Ui
T
Figure 2. Frame representing energy harvesting and information processing
Table 1. Main parameters
Symbol Description
hS The power beacon to base station channel coefficients
h1 The base station to U1 channel coefficients
h2 The base station to U2 channel coefficients
PB The power beacon transmit power
PS The base station transmit power
ϑ The energy conversion efficiency at the power beacon with 0 < ϑ < 1
xi The information symbol of the user Ui with i ∈ {1, 2}
ϕi The power allocation factors with ϕ2
1 > ϕ2 and ϕ2
1 + ϕ1
2 = 1
ni The additive white Gaussian noise with CN(0, σ2
i )
Moreover, the harvested energy at the small cell access point S is formulated by
ES =
ϑαPB |hS|
2
T
2
, (1)
Then, the average transmit power at S after the first time slot is obtained as
PS =
ES
(1 − α) T/2
=
ϑαPB |hS|
2
(1 − α)
. (2)
During the second phase, S transmits the information
√
PSϕ1x1 +
√
PSϕ2x2 to two users Ui. The Ui
received signal is computed by
yUi
=
p
PS (ϕ1x1 + ϕ2x2) hi + ni (3)
Bulletin of Electr Eng & Inf, Vol. 10, No. 5, October 2021 : 2686 – 2695
Bulletin of Electr Eng & Inf ISSN: 2302-9285 ❒ 2689
Then, the signal-to-interference- plus-noise ratio (SINR) to detect x2 at U1 is written as
Γ1,2 =
PSϕ2
1 |h1|
2
PSϕ2
2 |h1|
2
+ σ2
1
(4)
Putting (2) into (4), we can rewrite SINR as
Γ1,2 =
ϑαρ |hS|
2
|h1|
2
ϕ2
1
ϑαρ |hS|
2
|h1|
2
ϕ2
2 + (1 − α)
, (5)
where ρ = PB
σ2
i
is the transmit SNR at the access point S.
After applying SIC, the SINR required to detect x1 at U1 is formulated by
Γ1 =
ϑαρ |hS|
2
|h1|
2
ϕ2
2
(1 − α)
. (6)
Similarly, the SINR to detect x2 at U2 is formulated as
Γ2 =
PSϕ2
1 |h2|
2
PSϕ2
2 |h2|
2
+ σ2
2
=
ϑαρ |hS|
2
|h2|
2
ϕ2
1
ϑαρ |hS|
2
|h2|
2
ϕ2
2 + (1 − α)
.
(7)
These computations of SINR are the important step to further evaluate OP. It is noted that such outage perfor-
mance depends on distribution of wireless channels. We then examine such metric along with related impacts
in next the section.
3. OUTAGE PROBABILITY ANALYSIS
3.1. Channel distribution
In this section, hS and hi are followed by the Nakagami-m fading distribution. In particular, the
probability density function (PDF) is given as
f|hQ|2 (x) =
1
Γ (mQ)

mQ
λQ
mQ
xmQ−1
e
−
mQ
λQ
x
, (8)
where Q ∈ {S, 1, 2}, mS and λQ denote the fading severity factor and mean, respectively.
3.2. Outage probability
Similar metrics considered in the literature [10]-[16], utilize outage performance as a tool to decide if
an emerging technique can be implemented in practice or not. In particular, the OP of U1 is defined as [23]
Pout,1 = 1 − Pr (Γ1  γ1) , (9)
where γi = 22Ri/(1−α)
− 1 and Ri are the threshold SINR and the target rate, respectively. Substituting (6)
into (9), it can be written such that OP for user U1 is
Pout,1 =1 − Pr
ϑαρϕ2
2 |h1|
2
|hS|
2
(1 − α)
 γ1
!
= 1 − Pr |h1|
2

γ1 (1 − α)
ϑαρϕ2
2 |hS|
2
!
= 1 −
∞
Z
0
f|hS |2 (y)
∞
Z
γ1(1−α)
ϑαρϕ2
2y
f|h1|2 (x)dxdy
(10)
Outage performance of downlink NOMA-aided small cell network with wireless power transfer (Anh-Tu Le)
2690 ❒ ISSN: 2302-9285
With the help of (8), we can express OP as
Pout,1 =1 −
1
Γ (m1) Γ (mS)

m1
λ1
m1

mS
λS
mS
×
∞
Z
0
xmS −1
e
−
mS
λS
x
∞
Z
γ1(1−α)
ϑαρϕ2
2y
xm1−1
e−
m1
λ1
x
dxdy
(11)
Based on [33] in (12), we obtain
Pout,1 =1 −
m1−1
X
k=0
(mS/λS)
mS
Γ (mS) k!

m1γ1 (1 − α)
λ1ϑαρϕ2
2
k
×
∞
Z
0
ymS −k−1
e
−
mS
λS
y−
m1γ1(1−α)
λ1ϑαρϕ2
2y
dy
(12)
Moreover, by applying [33] in (13) and (14) the closed-form OP of U1 is obtained by
Pout,1 =1 −
m1−1
X
k=0
2
Γ (mS) k!

m1mSγ1 (1 − α)
λ1λSϑαρϕ2
2
mS +k
2
× KmS −k 2
s
m1mSγ1 (1 − α)
λ1λSϑαρϕ2
2
! (13)
Next, the OP of U2 is given as [23]
Pout,2 = 1 − Pr (Γ1,2  γ2, Γ2  γ2) (14)
Using (5) and (7), OP for user U2 as seen in (15) can be expressed as
Pout,2 = 1 − Pr
ϑαρ |hS|
2
|h1|
2
ϕ2
1
ϑαρ |hS|
2
|h1|
2
ϕ2
2 + (1 − α)
 γ2,
ϑαρ |hS|
2
|h2|
2
ϕ2
1
ϑαρ |hS|
2
|h2|
2
ϕ2
2 + (1 − α)
 γ2
!
= 1 − Pr |h1|
2

γ2 (1 − α)
ϑαρ (ϕ2
1 − γ2ϕ2
2) |hS|
2 , |h2|
2

γ2 (1 − α)
ϑαρ (ϕ2
1 − γ2ϕ2
2) |hS|
2
!
= 1 −
∞
Z
0
f|hS |2 (x)
∞
Z
γ2(1−α)
ϑαρ(ϕ2
1−γ2ϕ2
2)x
f|h1|2 (y)
∞
Z
γ2(1−α)
ϑαρ(ϕ2
1−γ2ϕ2
2)x
f|h2|2 (z)dzdydx
(15)
Thus, with the help of (8), Pout,2 is expressed as
Pout,2 = 1 −
(mS/ΩS)
mS
(m1/Ω1)
m1
(m2/Ω2)
m2
Γ (mS) Γ (m1) Γ (m2)
×
∞
Z
0
xmS −1
e
−
mS
ΩS
x
∞
Z
γ2(1−α)
ϑαρ(φ2
1−γ2φ2
2)x
ym1−1
e−
m1
Ω1
y
×
∞
Z
γ2(1−α)
ϑαρ(φ2
1−γ2φ2
2)x
zm2−1
e−
m2
Ω2
z
dzdydx.
(16)
Bulletin of Electr Eng  Inf, Vol. 10, No. 5, October 2021 : 2686 – 2695
Bulletin of Electr Eng  Inf ISSN: 2302-9285 ❒ 2691
Following similar steps as before, we can write Pout,2 as (17). Moreover, (17) is express as
Pout,2 = 1 −
1
Γ (mS)

mS
λS
mS m1−1
X
k1=0
m2−1
X
k2=0
1
k1!k2!

m1
λ1
k1

m2
λ2
k2

γ2 (1 − α)
ϑαρ (ϕ2
1 − γ2ϕ2
2)
k1+k2
×
∞
Z
0
xmS −k1−k2−1
e
−
mS
λS
x−
γ2(1−α)(m1λ2−λ1m2)
λ1λ2ϑαρ(ϕ2
1−γ2ϕ2
2)x
(17)
Finally, the expression of OP in closed-form at user U2 is formulated as (18), it is shown as
Pout,2 =1 −
m1−1
X
k1=0
m2−1
X
k2=0
2 (Ω1Ω2)
k1+k2
(m1/Ω1)
k1
(m2/Ω2)
k2
k1!k2!Γ (mS) (m1Ω2 + Ω1m2)
k1+k2
×

mSγ2 (1 − α) (m1Ω2 + Ω1m2)
ΩSΩ1Ω2ϑαρ (φ2
1 − γ2φ2
2)
mS +k1+k2
2
× KmS −k1−k2
2
s
mSγ2 (1 − α) (m1Ω2 + Ω1m2)
ΩSΩ1Ω2ϑαρ (φ2
1 − γ2φ2
2)
!
(18)
3.3. Throughput
Relying on OP computed in the previous section, throughput in delay-limited transmission mode is
further investigated. At fixed rates R1, R2, the throughput can be examined by [30]
T = (1 − Pout,1)R1 + (1 − Pout,2)R2 (19)
4. NUMERICAL RESULT AND EVALUATIONS
In this section, we present the numerical analysis of our PB-NOMA system along with corroboration
of analytical results. The parameters can be seen in Table 2. Figure 3 depicts OP for two users U1, U2 versus
transmit SNR at the access point. Such outage performance can be improved when the system achieves high
SNR. The reason is that high transmit power at the access point leads to high SNR, then outage performance is
enhanced significantly, especially in high SNR region. At different target rates, the system shows two different
curves of outage probability. It can be seen that at lower target rates, the better the OP can be achieved.
Figure 4 examines how the factor m influences to OP for two users U1, U2. The similar trends of OP
can be seen in this figure when compared with Figure 3. It is concluded that m affects performance, m = 3
exhibits the best case. The performance gap of the two users exists due to different power allocation factors. It
can be seen that the system continues its operation as normal if OP is kept low.
Figure 5 provides outage performance at the range of percentage time for energy harvesting. It is
obvious that the more time is allocated to energy harvesting leads to higher transmit power at the access point,
then such outage performance can be improved. We have similar trends of OP as in previous figures. Similar
performance can be seen in Figure 6 as varying ϑ. The main reason is that ϑ contributes to how much energy
can be harvested at the access point and the OP will be changed as well.
Table 2. Numerical result parameters
Target rates R1 = R2 = 0.4
Power allocation coefficients φ2
1 = 0.8, φ2
1 = 0.2
The fading severity factor mean mS = m1 = m2 = m = 2
and λS = λ2 = 1, λ1 = 2
The energy conversion efficiency ϑ = 0.9
Monte Carlo simulation 106
Outage performance of downlink NOMA-aided small cell network with wireless power transfer (Anh-Tu Le)
2692 ❒ ISSN: 2302-9285
0 5 10 15 20 25 30
10-3
10-2
10-1
100
Figure 3. The outage probability versus SNR varying R1 = R2 with α = 0.1
0 5 10 15 20 25 30
10-3
10-2
10-1
100
Figure 4. The outage probability versus SNR varying m with α = 0.1
0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9
10-4
10-3
10-2
10-1
100
= 10dB
= 20dB
= 30dB
Figure 5. The outage probability versus α varying ρ with α = 0.1
Bulletin of Electr Eng  Inf, Vol. 10, No. 5, October 2021 : 2686 – 2695
Bulletin of Electr Eng  Inf ISSN: 2302-9285 ❒ 2693
0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1
10-4
10-3
10-2
10-1
100
= 0.1
= 0.5
Figure 6. The outage probability versus ϑ varying α with ρ = 30dB
Figure 7 indicates that high throughput occurs in the high SNR region. It can be explained by the fact
that OP influences throughput. This result is definitely consistent with outage performance reported in previous
figures. Similarly to Figure 7 and Figure 8 illustrates how energy harvesting impacts throughput in the whole
SNR range. It can be explained by the fact that OP depends on how much energy is harvested and throughput
is affected as well. This result provides guidelines to implement energy harvesting in PB-NOMA.
0 5 10 15 20 25 30
0
0.1
0.2
0.3
0.4
0.5
0.6
0.7
0.8
0.9
1
m = 1,2,3
Figure 7. System throughput versus SNR varying m with α = 0.1
0 5 10 15 20 25 30
0
0.1
0.2
0.3
0.4
0.5
0.6
0.7
0.8
0.9
1
m = 1,2,3
Figure 8. System throughput versus ϑ varying α with ρ = 20dB
Outage performance of downlink NOMA-aided small cell network with wireless power transfer (Anh-Tu Le)
2694 ❒ ISSN: 2302-9285
5. CONCLUSION
Taking into account the linear characteristics of the actual circuit providing energy harvesting, this
paper has presented a mathematical framework to analyze system performance. Taking into account the outage
characteristics of the system. Based on the model, since the Nakagami-m channel is adopted, this paper derived
the exact expression of the outage probability downlink of PB-NOMA system based on the TS protocol and
calculated the throughput of the system. To find parameters affecting to system, this paper provided simulations
that verified the outage probability as derived in the theory. The simulation results verified the exactness of the
theoretical derivation and showed the influence of the different system parameters on the outage and throughput
performance. When the transmission rate are small and the harvested power is high at the access point, the PB-
NOMA system had better outage throughput. The simulations also showed that there is a gap between two
users which is caused by allocated power levels to each user. This study benefits the design of IoT with the
ability harvest energy. We can extend the two-user PB-NOMA approach to multiple users in future work.
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Outage performance of downlink NOMA-aided small cell network with wireless power transfer (Anh-Tu Le)

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Outage performance of downlink NOMA-aided small cell network with wireless power transfer

  • 1. Bulletin of Electrical Engineering and Informatics Vol. 10, No. 5, October 2021, pp. 2686∼2695 ISSN: 2302-9285, DOI: 10.11591/eei.v10i5.3015 ❒ 2686 Outage performance of downlink NOMA-aided small cell network with wireless power transfer Anh-Tu Le1 , Dinh-Thuan Do2 , Munyaradzi Munochiveyi3 1,2 Faculty of Electronics Technology, Industrial University of Ho Chi Minh City, Vietnam 3 Department of Computer Science and Information Engineering, College of Information and Electrical Engineering, Asia University, Taiwan Article Info Article history: Received Mar 30, 2021 Revised May 30, 2021 Accepted Jul 28, 2021 Keywords: Non-orthogonal multiple access Outage probability Power beacon Small cell network ABSTRACT This article considers the outage performance of the downlink transmission for a small cell network in a heterogeneous network. Due to mobility and distribution of users, it is necessary to study massive connections and high energy efficiency for such kind of systems. To be an enabler of energy harvesting, a power beacon is helpful to support the base station to send signals to distant users, and wireless power transfer (WPT) is exploited to guarantee the data packets transmission from the power beacon to the base station. To provide massive connections, we propose a novel non-orthogonal multiple access (NOMA) technique combined with WPT to enhance outage performance and latency reduction. Furthermore, we derive outage probability (OP) to characterize the system performance. Simulation results are verified to match well between theoretical and analytical methods, and main parameters are determined to understand how they affect the proposed scheme. This is an open access article under the CC BY-SA license. Corresponding Author: Dinh-Thuan Do Faculty of Electronics Technology Industrial University of Ho Chi Minh City 12 Nguyen Van Bao, Go Vap Dist., Ho Chi Minh City, Vietnam Email: dodinhthuan@iuh.edu.vn 1. INTRODUCTION To power the enormous number of internet of things (IoT), energy harvesting (EH) of radio frequency (RF) signals is billed as a promising solution [1]–[3]. In particular, the IoT receivers divide the received signal into two parts (EH and information processing (IP)). Power splitting (PS) or time switching (TS) are two commonly used EH architectures [4], [5]. Studies have shown that PS outperforms TS although it is difficult and inefficient to implement in practice. Recently in [4], [6] and [7], the authors demonstrated how harvested energy contributes to prolonging the lifetime of IoT systems. Reference [6] considered how to secure harvested residual energy after every forwarding and receiving cycle. As such, EH is essential for green and sustainable operation. Also, the authors examined the trade-off between residual harvested energy and the achievable rate. Differently, we go further in this paper to investigate the rate-energy (R-E) region for achievable rate and harvested residual energy in a two-way decode-and-forward (DF) relay system with a PS based energy harvesting relay. Nowadays, power domain non-orthogonal multiple access (PD-NOMA) has been widely studied by researchers [8]-[14]. The basic principle of PD-NOMA is that the users can transmit power via non-orthogonal transmission while the successive interference cancellation (SIC) receiver is employed at the receiver to miti- Journal homepage: http://beei.org
  • 2. Bulletin of Electr Eng & Inf ISSN: 2302-9285 ❒ 2687 gate interference [15]-[18]. Further, combining NOMA and cognitive radio (CR) is proposed to offer uninter- rupted, reliable, and massive connectivity [16]. Do et al. in [16], the problem of relay selection in CR-NOMA networks when spectrum sharing is operational is considered. As such, the number of accessible secondary users (SUs) sharing the limited and dynamic spectrum resources is boosted due to the opportunistic access of the licensed spectrum resources. Zaidi et al. in [17] studied the use of EH to maintain distinguishable levels of power when the users perform uplink NOMA transmissions. They derived an exact system ergodic average rate to determine the proposed network performance. The authors Gong and Chen in [19] considered various energy harvesting methods deployed in NOMA systems. They studied several protocols such as conventional TS, PS, and hybrid time-switching/power- splitting (TS/PS) by exploiting a single antenna base station and a single user pair setup. The study in [20] considered WPT via PS and information transmission in a NOMA system consisting of a single antenna base station. A full-duplex information transmitter subject to energy-constraints is studied in [21] to enable energy harvesting from a dedicated energy transmitter while NOMA is employed at the transmitter to communicate with the receivers. Reference [22] examined the performance of a CR-NOMA enabled wireless information and power transfer network (WIPT). Motivated by the above analysis, we deploy a power beacon (PB) to a small cell network in the downlink. Specifically, to implement IoT relay systems in practice, we analyze TS relaying protocol to facilitate energy harvesting in NOMA systems with the help of a nearby power beacon. This is beneficial for powering IoT devices and sensors such as indicators, alarms, and detectors which are used in underground trains, coal mines, and tunnels. Concerning the large number of IoT nodes in such environments, battery replacement of the sensor nodes or IoT devices is a staggeringly difficult task since connecting all of them through wired connections is difficult. Therefore, it is easy to recharge the IoT sensor nodes by deploying NOMA to transmit data to multiple IoT users. The main benefits of such a proposal is the enhancement of the power consumption, spectral efficiency and capacity demands in hard to reach environments [23]-[32]. Moreover, power beacons can be deployed everywhere to enable wireless power charging of the numerous IoT devices and sensors in these environments. In addition, it is important to provide the performance evaluation of a downlink system using NOMA when the impact of a power beacon is considered in such environments. It is expected that our proposed system model can be implemented in several scenarios as discussed to address existing difficulties. For the proposed model, we consider first the WPT scenario, and then we present the performance when PB-NOMA is exploited. For such a scenario, we detail comprehensively the outage performances and derive the exact outage probability expressions. Next, we determine which parameter affects the system per- formance under the constraints of the base station transmit signal-to-noise ratio (SNR) and harvested energy. Our contributions are listed is being as: − We study PB-NOMA by exploiting the TS scheme to determine the downlink performance under the scheme of linear energy harvesting. NOMA enables the small cell networks to continue their operations if they can accurately capture enough energy in the phase of the energy harvesting process. To facilitate any placement of the base station, the design of the PB benefits nearby base stations to serve their users in the downlink in limited conditions related to power provided by another source. − We formulate exact outage probability (OP) formulas subject to the constraint of the transmit SNR. We evaluate outage in some cases to show how PB-NOMA guarantees operation in the downlink. − Simulation results demonstrate that the performance of the proposed scheme in terms of the OP, can be improved if the channel parameters, transmit SNR, and power allocation factors are reasonably selected. The rest of this paper is organized is being as. Section 2 describes the PB-NOMA small cell networks. In section 3, we consider the scenario of PB-NOMA in terms of outage performance. We provide extensive numerical simulations in section 4 and section 5 concludes the paper. 2. SIGNAL ANALYSIS AND SYSTEM MODEL 2.1. System model As can be seen in Figure 1, we consider a small cell network containing an access point (S) which needs the help of a power beacon (PB) to serve two users (Ui, i ∈ {1, 2}). In this model, the main nodes (S, PB, and two user Ui) are equipped with single antennas. Further, all channel are assumed to be identically and independently distributed (i.i.d.) and following Nakagami-m distribution. The signal frame T includes two time slots, shown in Figure 2. The access point S harvests energy from the beacon in the first time slot (αT/2) Outage performance of downlink NOMA-aided small cell network with wireless power transfer (Anh-Tu Le)
  • 3. 2688 ❒ ISSN: 2302-9285 while signal processing in the link of S-Ui is conducted in the second time slot ((1 − α)T/2). Table 1 contains details of the main system parameters. PB U1 U2 Energy harvesting Information Transmission hS h1 h2 S Figure 1. NOMA-aided WPT downlink small cell network EH at S S to Ui T Figure 2. Frame representing energy harvesting and information processing Table 1. Main parameters Symbol Description hS The power beacon to base station channel coefficients h1 The base station to U1 channel coefficients h2 The base station to U2 channel coefficients PB The power beacon transmit power PS The base station transmit power ϑ The energy conversion efficiency at the power beacon with 0 < ϑ < 1 xi The information symbol of the user Ui with i ∈ {1, 2} ϕi The power allocation factors with ϕ2 1 > ϕ2 and ϕ2 1 + ϕ1 2 = 1 ni The additive white Gaussian noise with CN(0, σ2 i ) Moreover, the harvested energy at the small cell access point S is formulated by ES = ϑαPB |hS| 2 T 2 , (1) Then, the average transmit power at S after the first time slot is obtained as PS = ES (1 − α) T/2 = ϑαPB |hS| 2 (1 − α) . (2) During the second phase, S transmits the information √ PSϕ1x1 + √ PSϕ2x2 to two users Ui. The Ui received signal is computed by yUi = p PS (ϕ1x1 + ϕ2x2) hi + ni (3) Bulletin of Electr Eng & Inf, Vol. 10, No. 5, October 2021 : 2686 – 2695
  • 4. Bulletin of Electr Eng & Inf ISSN: 2302-9285 ❒ 2689 Then, the signal-to-interference- plus-noise ratio (SINR) to detect x2 at U1 is written as Γ1,2 = PSϕ2 1 |h1| 2 PSϕ2 2 |h1| 2 + σ2 1 (4) Putting (2) into (4), we can rewrite SINR as Γ1,2 = ϑαρ |hS| 2 |h1| 2 ϕ2 1 ϑαρ |hS| 2 |h1| 2 ϕ2 2 + (1 − α) , (5) where ρ = PB σ2 i is the transmit SNR at the access point S. After applying SIC, the SINR required to detect x1 at U1 is formulated by Γ1 = ϑαρ |hS| 2 |h1| 2 ϕ2 2 (1 − α) . (6) Similarly, the SINR to detect x2 at U2 is formulated as Γ2 = PSϕ2 1 |h2| 2 PSϕ2 2 |h2| 2 + σ2 2 = ϑαρ |hS| 2 |h2| 2 ϕ2 1 ϑαρ |hS| 2 |h2| 2 ϕ2 2 + (1 − α) . (7) These computations of SINR are the important step to further evaluate OP. It is noted that such outage perfor- mance depends on distribution of wireless channels. We then examine such metric along with related impacts in next the section. 3. OUTAGE PROBABILITY ANALYSIS 3.1. Channel distribution In this section, hS and hi are followed by the Nakagami-m fading distribution. In particular, the probability density function (PDF) is given as f|hQ|2 (x) = 1 Γ (mQ) mQ λQ mQ xmQ−1 e − mQ λQ x , (8) where Q ∈ {S, 1, 2}, mS and λQ denote the fading severity factor and mean, respectively. 3.2. Outage probability Similar metrics considered in the literature [10]-[16], utilize outage performance as a tool to decide if an emerging technique can be implemented in practice or not. In particular, the OP of U1 is defined as [23] Pout,1 = 1 − Pr (Γ1 γ1) , (9) where γi = 22Ri/(1−α) − 1 and Ri are the threshold SINR and the target rate, respectively. Substituting (6) into (9), it can be written such that OP for user U1 is Pout,1 =1 − Pr ϑαρϕ2 2 |h1| 2 |hS| 2 (1 − α) γ1 ! = 1 − Pr |h1| 2 γ1 (1 − α) ϑαρϕ2 2 |hS| 2 ! = 1 − ∞ Z 0 f|hS |2 (y) ∞ Z γ1(1−α) ϑαρϕ2 2y f|h1|2 (x)dxdy (10) Outage performance of downlink NOMA-aided small cell network with wireless power transfer (Anh-Tu Le)
  • 5. 2690 ❒ ISSN: 2302-9285 With the help of (8), we can express OP as Pout,1 =1 − 1 Γ (m1) Γ (mS) m1 λ1 m1 mS λS mS × ∞ Z 0 xmS −1 e − mS λS x ∞ Z γ1(1−α) ϑαρϕ2 2y xm1−1 e− m1 λ1 x dxdy (11) Based on [33] in (12), we obtain Pout,1 =1 − m1−1 X k=0 (mS/λS) mS Γ (mS) k! m1γ1 (1 − α) λ1ϑαρϕ2 2 k × ∞ Z 0 ymS −k−1 e − mS λS y− m1γ1(1−α) λ1ϑαρϕ2 2y dy (12) Moreover, by applying [33] in (13) and (14) the closed-form OP of U1 is obtained by Pout,1 =1 − m1−1 X k=0 2 Γ (mS) k! m1mSγ1 (1 − α) λ1λSϑαρϕ2 2 mS +k 2 × KmS −k 2 s m1mSγ1 (1 − α) λ1λSϑαρϕ2 2 ! (13) Next, the OP of U2 is given as [23] Pout,2 = 1 − Pr (Γ1,2 γ2, Γ2 γ2) (14) Using (5) and (7), OP for user U2 as seen in (15) can be expressed as Pout,2 = 1 − Pr ϑαρ |hS| 2 |h1| 2 ϕ2 1 ϑαρ |hS| 2 |h1| 2 ϕ2 2 + (1 − α) γ2, ϑαρ |hS| 2 |h2| 2 ϕ2 1 ϑαρ |hS| 2 |h2| 2 ϕ2 2 + (1 − α) γ2 ! = 1 − Pr |h1| 2 γ2 (1 − α) ϑαρ (ϕ2 1 − γ2ϕ2 2) |hS| 2 , |h2| 2 γ2 (1 − α) ϑαρ (ϕ2 1 − γ2ϕ2 2) |hS| 2 ! = 1 − ∞ Z 0 f|hS |2 (x) ∞ Z γ2(1−α) ϑαρ(ϕ2 1−γ2ϕ2 2)x f|h1|2 (y) ∞ Z γ2(1−α) ϑαρ(ϕ2 1−γ2ϕ2 2)x f|h2|2 (z)dzdydx (15) Thus, with the help of (8), Pout,2 is expressed as Pout,2 = 1 − (mS/ΩS) mS (m1/Ω1) m1 (m2/Ω2) m2 Γ (mS) Γ (m1) Γ (m2) × ∞ Z 0 xmS −1 e − mS ΩS x ∞ Z γ2(1−α) ϑαρ(φ2 1−γ2φ2 2)x ym1−1 e− m1 Ω1 y × ∞ Z γ2(1−α) ϑαρ(φ2 1−γ2φ2 2)x zm2−1 e− m2 Ω2 z dzdydx. (16) Bulletin of Electr Eng Inf, Vol. 10, No. 5, October 2021 : 2686 – 2695
  • 6. Bulletin of Electr Eng Inf ISSN: 2302-9285 ❒ 2691 Following similar steps as before, we can write Pout,2 as (17). Moreover, (17) is express as Pout,2 = 1 − 1 Γ (mS) mS λS mS m1−1 X k1=0 m2−1 X k2=0 1 k1!k2! m1 λ1 k1 m2 λ2 k2 γ2 (1 − α) ϑαρ (ϕ2 1 − γ2ϕ2 2) k1+k2 × ∞ Z 0 xmS −k1−k2−1 e − mS λS x− γ2(1−α)(m1λ2−λ1m2) λ1λ2ϑαρ(ϕ2 1−γ2ϕ2 2)x (17) Finally, the expression of OP in closed-form at user U2 is formulated as (18), it is shown as Pout,2 =1 − m1−1 X k1=0 m2−1 X k2=0 2 (Ω1Ω2) k1+k2 (m1/Ω1) k1 (m2/Ω2) k2 k1!k2!Γ (mS) (m1Ω2 + Ω1m2) k1+k2 × mSγ2 (1 − α) (m1Ω2 + Ω1m2) ΩSΩ1Ω2ϑαρ (φ2 1 − γ2φ2 2) mS +k1+k2 2 × KmS −k1−k2 2 s mSγ2 (1 − α) (m1Ω2 + Ω1m2) ΩSΩ1Ω2ϑαρ (φ2 1 − γ2φ2 2) ! (18) 3.3. Throughput Relying on OP computed in the previous section, throughput in delay-limited transmission mode is further investigated. At fixed rates R1, R2, the throughput can be examined by [30] T = (1 − Pout,1)R1 + (1 − Pout,2)R2 (19) 4. NUMERICAL RESULT AND EVALUATIONS In this section, we present the numerical analysis of our PB-NOMA system along with corroboration of analytical results. The parameters can be seen in Table 2. Figure 3 depicts OP for two users U1, U2 versus transmit SNR at the access point. Such outage performance can be improved when the system achieves high SNR. The reason is that high transmit power at the access point leads to high SNR, then outage performance is enhanced significantly, especially in high SNR region. At different target rates, the system shows two different curves of outage probability. It can be seen that at lower target rates, the better the OP can be achieved. Figure 4 examines how the factor m influences to OP for two users U1, U2. The similar trends of OP can be seen in this figure when compared with Figure 3. It is concluded that m affects performance, m = 3 exhibits the best case. The performance gap of the two users exists due to different power allocation factors. It can be seen that the system continues its operation as normal if OP is kept low. Figure 5 provides outage performance at the range of percentage time for energy harvesting. It is obvious that the more time is allocated to energy harvesting leads to higher transmit power at the access point, then such outage performance can be improved. We have similar trends of OP as in previous figures. Similar performance can be seen in Figure 6 as varying ϑ. The main reason is that ϑ contributes to how much energy can be harvested at the access point and the OP will be changed as well. Table 2. Numerical result parameters Target rates R1 = R2 = 0.4 Power allocation coefficients φ2 1 = 0.8, φ2 1 = 0.2 The fading severity factor mean mS = m1 = m2 = m = 2 and λS = λ2 = 1, λ1 = 2 The energy conversion efficiency ϑ = 0.9 Monte Carlo simulation 106 Outage performance of downlink NOMA-aided small cell network with wireless power transfer (Anh-Tu Le)
  • 7. 2692 ❒ ISSN: 2302-9285 0 5 10 15 20 25 30 10-3 10-2 10-1 100 Figure 3. The outage probability versus SNR varying R1 = R2 with α = 0.1 0 5 10 15 20 25 30 10-3 10-2 10-1 100 Figure 4. The outage probability versus SNR varying m with α = 0.1 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 10-4 10-3 10-2 10-1 100 = 10dB = 20dB = 30dB Figure 5. The outage probability versus α varying ρ with α = 0.1 Bulletin of Electr Eng Inf, Vol. 10, No. 5, October 2021 : 2686 – 2695
  • 8. Bulletin of Electr Eng Inf ISSN: 2302-9285 ❒ 2693 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1 10-4 10-3 10-2 10-1 100 = 0.1 = 0.5 Figure 6. The outage probability versus ϑ varying α with ρ = 30dB Figure 7 indicates that high throughput occurs in the high SNR region. It can be explained by the fact that OP influences throughput. This result is definitely consistent with outage performance reported in previous figures. Similarly to Figure 7 and Figure 8 illustrates how energy harvesting impacts throughput in the whole SNR range. It can be explained by the fact that OP depends on how much energy is harvested and throughput is affected as well. This result provides guidelines to implement energy harvesting in PB-NOMA. 0 5 10 15 20 25 30 0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1 m = 1,2,3 Figure 7. System throughput versus SNR varying m with α = 0.1 0 5 10 15 20 25 30 0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1 m = 1,2,3 Figure 8. System throughput versus ϑ varying α with ρ = 20dB Outage performance of downlink NOMA-aided small cell network with wireless power transfer (Anh-Tu Le)
  • 9. 2694 ❒ ISSN: 2302-9285 5. CONCLUSION Taking into account the linear characteristics of the actual circuit providing energy harvesting, this paper has presented a mathematical framework to analyze system performance. Taking into account the outage characteristics of the system. Based on the model, since the Nakagami-m channel is adopted, this paper derived the exact expression of the outage probability downlink of PB-NOMA system based on the TS protocol and calculated the throughput of the system. To find parameters affecting to system, this paper provided simulations that verified the outage probability as derived in the theory. The simulation results verified the exactness of the theoretical derivation and showed the influence of the different system parameters on the outage and throughput performance. When the transmission rate are small and the harvested power is high at the access point, the PB- NOMA system had better outage throughput. 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