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Bulletin of Electrical Engineering and Informatics
Vol. 9, No. 1, February 2020,pp. 94~100
ISSN: 2302-9285,DOI: 10.11591/eei.v9i1.1650  94
Journal homepage: http://beei.org
Adaptive relaying protocol for wireless energy harvesting and
information processing in NOMA systems:
Outage probability analysis
Phu Tran Tin1, Duy-Hung Ha2, Tran Thanh Trang3
1
Faculty of Electronics Technology, Industrial University of Ho Chi Minh City, Vietnam
2
Wireless Communications Research Group, Faculty of Electrical and Electronics Engineering,
Ton Duc Thang University, Vietnam
3
National Key Laboratory of Digital Control and System Engineering, Vietnam
Article Info ABSTRACT
Article history:
Received Jun 3, 2019
Revised Aug 10, 2019
Accepted Sep 26, 2019
In order to satisfy the increasing data rate demands, the research in
the fifth-generation (5G) wireless networks is ongoing, both in academia and
industry. In this research, we propose and investigate adaptive relaying
protocol (ARP) For wireless energy harvesting (EH) and information
processing in NOMA systems. Firstly, we investigate and derive
the closed-form and integral-form expressions of the outage probability (OP)
of the model system. Then, all the results are convinced by the Monte Carlo
simulation. The research results show that all the analytical and simulation
results are the same in connection with the primary system parameters.
This research can provide a recommendation for NOMA system network.
Keywords:
Energy harvesting
Monte Carlo
NOMA
Outage probability
Relaying network This is an open access article under the CC BY-SA license.
Corresponding Author:
Duy-Hung Ha,
Wireless CommunicationsResearch Group,
Faculty of Electrical and Electronics Engineering,
Ton Duc Thang University, Ho Chi Minh City, Vietnam.
Email: haduyhung@tdtu.edu.vn
1. INTRODUCTION
In order to satisfy the increasing data rate demands, the research in the fifth-generation (5G)
wireless networks is ongoing, both in academia and industry. The full-duplex (FD) is a popular technique
in the relaying communication network, which allows the communication node to transmit and receive
signals over the same frequency band at the same time slot. In comparison with the traditional water-filling
power allocation strategy, NOMA allocates more power to the users with worse channel conditions,
which results in a better tradeoff between the system throughput and user fairness [1-6]. From the previous
researches, authors in [7] investigate the impact of user pairing on downlink NOMA systems. [8] has
proposed power allocation with the max-min fairness criterion. An uplink NOMA scheme with joint power
and subcarrier allocations has been considered in [9]. In [10], the authors introduced a cooperation -based
NOMA scheme for coordinated direct and relay transmissions. A diversity-oriented detection mechanism for
the cooperative relaying system using NOMA has been presented in [11]. The performance of transmit
antenna selection for NOMA assisted multiple-input-multiple-output (MIMO) relay networks have been
examined in [12]. Authors in [13] presented and investigated a cooperative NOMA transmission scheme.
Bulletin of Electr Eng & Inf ISSN: 2302-9285 
Adaptive relaying protocol forwireless energy harvesting and information processing… (Phu Tran Tin)
95
In this research, we propose adaptive relaying protocol (ARP) for wireless energy harvesting and
information processing in NOMA Systems. Firstly, we investigate and derive the closed-form and integral
form expression of the outage probability (OP) of the model system. Then, all the results are convinced
by Monte Carlo simulation in connection with all primary system parameters. From the results, we can
convince that all the analytical and simulation results are the same in connection with the primary system
parameters.The research focuseson some contributions as;
- The ARP for wireless energy harvesting and information processing in NOMA systems is proposed.
- The closed-form and integral-form expressions of the system OP is investigated and derived.
- All the results are convinced by Monte Carlo simulation in connection with all primary system
parameters.
2. SYSTEM MODEL
The ARP for wireless energy harvesting and information processing in NOMA systems is drawn in
Figure 1. In this system model, we denote Source is S, D1 and D2 are two destination nodes. The energy
harvesting (EH) and information processing (IT) for this proposed model system are illustrated in Figure 2.
In this protocol, the transmission time T consists of three-time slots. In the first time slot αT (α is the time
switching factor, 0<ρ<1), the energy of the D1 harvest from the source node S. In the second interval
time (1-α)T/2, the source S transfers the energy and information to D1 at the same time.
Finally, the remaining time slot (1-α)T/2 is used for information transferring from the destination node D1 to
the destination node D2.
Energy Harvesting
(EH)
Information transmission
(IT)
S D2
D1
EH at D1
IT
D1àD2
(1-α)T/2
T
(1-α)T/2
S
P

IT: SàD1
(1 ) S
P

−
EH at D1
αT
Figure 1. System model Figure 2. The EH and IT
2.1. Energy harvesting phase
The received signal at the relay R in the first time slot αT can be formulated as;
( )
1 1
1
1 1 2 2
D s s D
y h b P x b P x n
= + + (1)
Where Ps is the transmitting power of source S, h is channel gain of S-D1 link and nD1 denoted
the additive white Gaussian noise (AWGN) at D1 which has zero-mean and variance N0. b1 and b2 are power
allocation coefficientsfor data symbols x1 and x2 that is wished to send from;
S toD1 and D2, respectively and satisfied 2 1
1 2
0
1
b b
b b
 


+ =

.
We assume that    
2 2
1 2 1
x x
 =  = which  
 • is the expectation operator. Based on (1),
the harvested energy in the first time slot αT can be calculated as;
( )
2 2
1 2 1
s s
E TP h b b TP h
 
= + = (2)
The received signal at D1 in the second interval time (1-α)T/2 can be expressed as;
( )
1 1
2
1 1 1 2
D s s D
y h b P x b P x n

= + + (3)
 ISSN: 2302-9285
Bulletin of Electr Eng & Inf, Vol. 9, No. 1, February 2020 : 94 – 100
96
Therefore, the harvested energy in the second interval time (1-α)T/2 can be given by;
( )
2 2
2 1 2
1 1
2 2
s s
E TP h b b TP h
 
 
− −
   
= + =
   
   
(4)
From (2) and (4), the total average transmitted power at the relay node R can be calculated
asthe following;
1
1
2
1 2
(1 ) / 2 (1 ) / 2
D
D s
E E E
P P h
T T

 
+
= = =
− −
(5)
Where
2 (1 )
1
  


+ −
=
−
2.2. Information transmission phase
In the second interval time (1-α)T/2, the received signal at the destination node D1 can be
expressed as;
( )
1 1
1 1 2 1
(1 )
D s D
y P h b x b x n

= − + + (6)
After receiving the signal from S, D1 will decode the signal and decode its own signal by using
successive interference cancellation (SIC) [14]. From (6) the received signal to interference plus noise ratio
(SINR) at the destination node D1 to detect of the destination node D2 is given by;
1
2
2
2, 2
1
(1 )
(1 ) 1
D
h b
SINR
h b


− 
=
−  +
(7)
Where
0
s
P
N
 = represents the transmit signal-to-noise ratio (SNR).
After applying SIC, there is no interference remaining in the received signal at the destination node
D1. Therefore, the received SNR at the destination node D1 to detect its own signal 1
x is obtained by;
1
2
1, 1
(1 )
D
SNR h b

= −  (8)
In the third interval time (1-α)T/2, the decoded signal 2
x at D1 is forwarded to D2.
Hence, the received signal at the destination node D2 can be given as;
2 1 2
2
D D D
y P gx n
= + (9)
Where g is channel gain of D1-D2 link and 2
D
n is AWGN at D2 which has zero-mean and variance N0.
Hence, the received SNR at D2 is given by;
1
2
2
2,
0
D
D
P g
SNR
N
= (10)
Substituting (5) into (10), we have:
2
2 2
2 2
2,
0
s
D
P h g
SNR h g
N


= =  (11)
Bulletin of Electr Eng & Inf ISSN: 2302-9285 
Adaptive relaying protocol forwireless energy harvesting and information processing… (Phu Tran Tin)
97
3. SYSTEM PERFORMANCE ANALYSIS
3.1. Outage probability (OP) at D1
In the NOMA protocol, D1 is not in an outage when it can decode both 1
x and 2
x received from S.
So, the OP at D1 can be expressed as;
( )
1 1 1
2 1
2, 1,
1 Pr ,
D D th D th
OP SINR SNR
 
= −   (12)
Where 1
2
1
2 1
R
th
 = − and 2
2
2
2 1
R
th
 = − in which R1 and R2 are the source rates to detect 1
x and 2
x at D1,
respectively. Substituting (7) and (8) into (12), the OP at D1 can be rewritten as;
( )
( )
1
2
2
2
2 2 1
1
2
1
2 1
2 2
2
1
2 1
2
(1 )
1 Pr ,(1 )
(1 ) 1
1 Pr ,
(1 )
(1 )
1 Pr
1 ( ) 1 exp
D th th
th th
th
h
h
h b
OP h b
h b
h h
b
b b
h
f x dx

  

 

 



 
− 
 
= −  −  
 
−  +
 
 
 
= −  
− 
−  −
 
 
 
= −  
 
= − = − − 

(13)
Where
( )
2 1
2
1
2 1
max ,
(1 )
(1 )
th th
th
b
b b
 

 
 
 
 =
− 
−  −
 
 
and h
 is mean of the random
variable (RV)
2
h
3.2. Outage probability (OP) at D2
D2 is in an outage when either D1 can not detect 2
x or D2 can not recover the forwarded signal from
D1. Hence,the OP at D2 can be obtained as;
( ) ( )
2 1 2 1
2 2 2
2, 2, 2,
Pr Pr ,
D D th D th D th
OP SINR SNR SINR
  
=  +   (14)
The first term of (14) can be derived as;
( )
( )
( )
1
2
2
2 2
2, 2
1
2
2 2
2 1
2
2 1
2
2 1
2
2
2 1
2
2 1
2
2 1
(1 )
Pr Pr
(1 ) 1
Pr , 0
(1 )
1 , 0
1 exp , 0
(1 )
1 , 0
D th th
th
th
th
th
th h
th
th
th
h b
SINR
h b
h b b
b b
b b
b b
b b
b b

 



 

 

 

 
− 
 = 
 
−  +
 
 
  
  
 − 

= −  −
 
  

− 


  
  
− − − 

= −  −
 
  

− 


(15)
 ISSN: 2302-9285
Bulletin of Electr Eng & Inf, Vol. 9, No. 1, February 2020 : 94 – 100
98
The second term of (14) can be rewritten as;
( )
( )
( )
2 1
2
2
2 2
2
2
2 1
2
2 2 2
2 2 2 2
2, 2, 2
1
2 2
2 2
2 2
2 1
0
(1 )
2
(1 )
Pr , Pr ,
(1 ) 1
Pr ,
(1 )
( ) ( )
1 exp
th
th
th
D th D th th th
th th
th
h
h g
b b
th g
h
h b
SNR SINR h g
h b
g h
b b
h
f x f y dxdy
x



 

    

 
 

 




−  −
 
− 
  =   
 
−  +
 
 
 
 
=  
−  −
 

 
=
 
= − −
 
 
 
 
( )
exp h
x dx



 
−
 

 
 

(16)
Where
( )
2
2
2 1
(1 )
th
th
b b

 
 =
−  −
. Substituting (15), (16) into (14), finally, the OP at D2 can be claimed as;
( ) ( )
2
2
1 exp 1 exp exp
th g
D h h h
OP x dx
x
 
  



 
 
= − −  + − − −
 
 
 

 
 
 
 (17)
4. NUMERICAL RESULTS AND DISCUSSION
In this section, we investigate the OP of the model system using Monte Carlo Simulation
in connection with the primary system parameters [15-26]. In Figure 3, the effect of b2 on the system OP
is plotted with the primary system parameters as η=0.8, R1=R2=0.5 bps/Hz, α=ρ=0.5. From the results,
we can see that the system OP of the destination node D1 significantly decreases with the rising of b2.
However, the system OP of the destination node D2 decreases when a2 increases from 0.55 to 0.7 and after
that, has a massive increase with the remaining values of b2. In the same way, the system OP versus α
is drawn in Figure 4. In this simulation, we set η=0.8, ψ=7 dB, ρ=0.5, and b2=0.9, b1=0.1. As shown in
Figure 4, we can state that the OP of the model system has a slight decrease when α varies from 0 to 1.
In both Figure 3 and Figure 4, the simulation and analyticalresults are the same wit hall values of α and b2.
Figure 3. OP versus b2 Figure 4. OP versus α
Bulletin of Electr Eng & Inf ISSN: 2302-9285 
Adaptive relaying protocol forwireless energy harvesting and information processing… (Phu Tran Tin)
99
Furthermore, we investigate the effect of η and ψ on the OP of the model system, as plotted
in Figure 5 and Figure 6. In these Figure, we set the primary parameters as a2=0.7, 0.9, R1=R2=0.5 bps/Hz,
PS/N0=0.5. From Figure 5 and Figure 6, it can be observed that the system OP has a slight decrease when η
varies from 0 to 1, and the system OP crucially decreases with the rising of ψ from 0 to 25. In all two Figure,
the analytical and simulation results agree well with each other. On another hand, the comparison
of the system OP of two destination nodes is demonstrated in all Figure. From the results, we can state that
the system OP of the destination node D2 is better than the destination node D1.
Figure 5. OP versus η Figure 6. OP versus ψ
5. CONCLUSION
In this research, we propose the ARP For wireless energy harvesting and information processing in
NOMA systems. Firstly, we investigate and derive the closed-form and integral form expression
of the outage probability (OP) of the model system. Then, all the results are convinced by Monte Carlo
simulation in connection with all primary system parameters. From the results, we can convince that all
the analyticaland simulation results are the same in connection with the primary system parameters.
ACKNOWLEDGEMENTS
This research was supported by National Key Laboratory of Digital Control and System
Engineering (DCSELAB), HCMUT, VNU-HCM, Vietnam.
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Adaptive relaying protocol for wireless energy harvesting and information processing in NOMA systems: Outage probability analysis

  • 1. Bulletin of Electrical Engineering and Informatics Vol. 9, No. 1, February 2020,pp. 94~100 ISSN: 2302-9285,DOI: 10.11591/eei.v9i1.1650  94 Journal homepage: http://beei.org Adaptive relaying protocol for wireless energy harvesting and information processing in NOMA systems: Outage probability analysis Phu Tran Tin1, Duy-Hung Ha2, Tran Thanh Trang3 1 Faculty of Electronics Technology, Industrial University of Ho Chi Minh City, Vietnam 2 Wireless Communications Research Group, Faculty of Electrical and Electronics Engineering, Ton Duc Thang University, Vietnam 3 National Key Laboratory of Digital Control and System Engineering, Vietnam Article Info ABSTRACT Article history: Received Jun 3, 2019 Revised Aug 10, 2019 Accepted Sep 26, 2019 In order to satisfy the increasing data rate demands, the research in the fifth-generation (5G) wireless networks is ongoing, both in academia and industry. In this research, we propose and investigate adaptive relaying protocol (ARP) For wireless energy harvesting (EH) and information processing in NOMA systems. Firstly, we investigate and derive the closed-form and integral-form expressions of the outage probability (OP) of the model system. Then, all the results are convinced by the Monte Carlo simulation. The research results show that all the analytical and simulation results are the same in connection with the primary system parameters. This research can provide a recommendation for NOMA system network. Keywords: Energy harvesting Monte Carlo NOMA Outage probability Relaying network This is an open access article under the CC BY-SA license. Corresponding Author: Duy-Hung Ha, Wireless CommunicationsResearch Group, Faculty of Electrical and Electronics Engineering, Ton Duc Thang University, Ho Chi Minh City, Vietnam. Email: haduyhung@tdtu.edu.vn 1. INTRODUCTION In order to satisfy the increasing data rate demands, the research in the fifth-generation (5G) wireless networks is ongoing, both in academia and industry. The full-duplex (FD) is a popular technique in the relaying communication network, which allows the communication node to transmit and receive signals over the same frequency band at the same time slot. In comparison with the traditional water-filling power allocation strategy, NOMA allocates more power to the users with worse channel conditions, which results in a better tradeoff between the system throughput and user fairness [1-6]. From the previous researches, authors in [7] investigate the impact of user pairing on downlink NOMA systems. [8] has proposed power allocation with the max-min fairness criterion. An uplink NOMA scheme with joint power and subcarrier allocations has been considered in [9]. In [10], the authors introduced a cooperation -based NOMA scheme for coordinated direct and relay transmissions. A diversity-oriented detection mechanism for the cooperative relaying system using NOMA has been presented in [11]. The performance of transmit antenna selection for NOMA assisted multiple-input-multiple-output (MIMO) relay networks have been examined in [12]. Authors in [13] presented and investigated a cooperative NOMA transmission scheme.
  • 2. Bulletin of Electr Eng & Inf ISSN: 2302-9285  Adaptive relaying protocol forwireless energy harvesting and information processing… (Phu Tran Tin) 95 In this research, we propose adaptive relaying protocol (ARP) for wireless energy harvesting and information processing in NOMA Systems. Firstly, we investigate and derive the closed-form and integral form expression of the outage probability (OP) of the model system. Then, all the results are convinced by Monte Carlo simulation in connection with all primary system parameters. From the results, we can convince that all the analytical and simulation results are the same in connection with the primary system parameters.The research focuseson some contributions as; - The ARP for wireless energy harvesting and information processing in NOMA systems is proposed. - The closed-form and integral-form expressions of the system OP is investigated and derived. - All the results are convinced by Monte Carlo simulation in connection with all primary system parameters. 2. SYSTEM MODEL The ARP for wireless energy harvesting and information processing in NOMA systems is drawn in Figure 1. In this system model, we denote Source is S, D1 and D2 are two destination nodes. The energy harvesting (EH) and information processing (IT) for this proposed model system are illustrated in Figure 2. In this protocol, the transmission time T consists of three-time slots. In the first time slot αT (α is the time switching factor, 0<ρ<1), the energy of the D1 harvest from the source node S. In the second interval time (1-α)T/2, the source S transfers the energy and information to D1 at the same time. Finally, the remaining time slot (1-α)T/2 is used for information transferring from the destination node D1 to the destination node D2. Energy Harvesting (EH) Information transmission (IT) S D2 D1 EH at D1 IT D1àD2 (1-α)T/2 T (1-α)T/2 S P  IT: SàD1 (1 ) S P  − EH at D1 αT Figure 1. System model Figure 2. The EH and IT 2.1. Energy harvesting phase The received signal at the relay R in the first time slot αT can be formulated as; ( ) 1 1 1 1 1 2 2 D s s D y h b P x b P x n = + + (1) Where Ps is the transmitting power of source S, h is channel gain of S-D1 link and nD1 denoted the additive white Gaussian noise (AWGN) at D1 which has zero-mean and variance N0. b1 and b2 are power allocation coefficientsfor data symbols x1 and x2 that is wished to send from; S toD1 and D2, respectively and satisfied 2 1 1 2 0 1 b b b b     + =  . We assume that     2 2 1 2 1 x x  =  = which    • is the expectation operator. Based on (1), the harvested energy in the first time slot αT can be calculated as; ( ) 2 2 1 2 1 s s E TP h b b TP h   = + = (2) The received signal at D1 in the second interval time (1-α)T/2 can be expressed as; ( ) 1 1 2 1 1 1 2 D s s D y h b P x b P x n  = + + (3)
  • 3.  ISSN: 2302-9285 Bulletin of Electr Eng & Inf, Vol. 9, No. 1, February 2020 : 94 – 100 96 Therefore, the harvested energy in the second interval time (1-α)T/2 can be given by; ( ) 2 2 2 1 2 1 1 2 2 s s E TP h b b TP h     − −     = + =         (4) From (2) and (4), the total average transmitted power at the relay node R can be calculated asthe following; 1 1 2 1 2 (1 ) / 2 (1 ) / 2 D D s E E E P P h T T    + = = = − − (5) Where 2 (1 ) 1      + − = − 2.2. Information transmission phase In the second interval time (1-α)T/2, the received signal at the destination node D1 can be expressed as; ( ) 1 1 1 1 2 1 (1 ) D s D y P h b x b x n  = − + + (6) After receiving the signal from S, D1 will decode the signal and decode its own signal by using successive interference cancellation (SIC) [14]. From (6) the received signal to interference plus noise ratio (SINR) at the destination node D1 to detect of the destination node D2 is given by; 1 2 2 2, 2 1 (1 ) (1 ) 1 D h b SINR h b   −  = −  + (7) Where 0 s P N  = represents the transmit signal-to-noise ratio (SNR). After applying SIC, there is no interference remaining in the received signal at the destination node D1. Therefore, the received SNR at the destination node D1 to detect its own signal 1 x is obtained by; 1 2 1, 1 (1 ) D SNR h b  = −  (8) In the third interval time (1-α)T/2, the decoded signal 2 x at D1 is forwarded to D2. Hence, the received signal at the destination node D2 can be given as; 2 1 2 2 D D D y P gx n = + (9) Where g is channel gain of D1-D2 link and 2 D n is AWGN at D2 which has zero-mean and variance N0. Hence, the received SNR at D2 is given by; 1 2 2 2, 0 D D P g SNR N = (10) Substituting (5) into (10), we have: 2 2 2 2 2 2, 0 s D P h g SNR h g N   = =  (11)
  • 4. Bulletin of Electr Eng & Inf ISSN: 2302-9285  Adaptive relaying protocol forwireless energy harvesting and information processing… (Phu Tran Tin) 97 3. SYSTEM PERFORMANCE ANALYSIS 3.1. Outage probability (OP) at D1 In the NOMA protocol, D1 is not in an outage when it can decode both 1 x and 2 x received from S. So, the OP at D1 can be expressed as; ( ) 1 1 1 2 1 2, 1, 1 Pr , D D th D th OP SINR SNR   = −   (12) Where 1 2 1 2 1 R th  = − and 2 2 2 2 1 R th  = − in which R1 and R2 are the source rates to detect 1 x and 2 x at D1, respectively. Substituting (7) and (8) into (12), the OP at D1 can be rewritten as; ( ) ( ) 1 2 2 2 2 2 1 1 2 1 2 1 2 2 2 1 2 1 2 (1 ) 1 Pr ,(1 ) (1 ) 1 1 Pr , (1 ) (1 ) 1 Pr 1 ( ) 1 exp D th th th th th h h h b OP h b h b h h b b b h f x dx                −    = −  −     −  +       = −   −  −  −       = −     = − = − −   (13) Where ( ) 2 1 2 1 2 1 max , (1 ) (1 ) th th th b b b           = −  −  −     and h  is mean of the random variable (RV) 2 h 3.2. Outage probability (OP) at D2 D2 is in an outage when either D1 can not detect 2 x or D2 can not recover the forwarded signal from D1. Hence,the OP at D2 can be obtained as; ( ) ( ) 2 1 2 1 2 2 2 2, 2, 2, Pr Pr , D D th D th D th OP SINR SNR SINR    =  +   (14) The first term of (14) can be derived as; ( ) ( ) ( ) 1 2 2 2 2 2, 2 1 2 2 2 2 1 2 2 1 2 2 1 2 2 2 1 2 2 1 2 2 1 (1 ) Pr Pr (1 ) 1 Pr , 0 (1 ) 1 , 0 1 exp , 0 (1 ) 1 , 0 D th th th th th th th h th th th h b SINR h b h b b b b b b b b b b b b                  −   =    −  +            −   = −  −       −          − − −   = −  −       −    (15)
  • 5.  ISSN: 2302-9285 Bulletin of Electr Eng & Inf, Vol. 9, No. 1, February 2020 : 94 – 100 98 The second term of (14) can be rewritten as; ( ) ( ) ( ) 2 1 2 2 2 2 2 2 2 1 2 2 2 2 2 2 2 2 2, 2, 2 1 2 2 2 2 2 2 2 1 0 (1 ) 2 (1 ) Pr , Pr , (1 ) 1 Pr , (1 ) ( ) ( ) 1 exp th th th D th D th th th th th th h h g b b th g h h b SNR SINR h g h b g h b b h f x f y dxdy x                        −  −   −    =      −  +         =   −  −      =   = − −         ( ) exp h x dx      −         (16) Where ( ) 2 2 2 1 (1 ) th th b b     = −  − . Substituting (15), (16) into (14), finally, the OP at D2 can be claimed as; ( ) ( ) 2 2 1 exp 1 exp exp th g D h h h OP x dx x             = − −  + − − −               (17) 4. NUMERICAL RESULTS AND DISCUSSION In this section, we investigate the OP of the model system using Monte Carlo Simulation in connection with the primary system parameters [15-26]. In Figure 3, the effect of b2 on the system OP is plotted with the primary system parameters as η=0.8, R1=R2=0.5 bps/Hz, α=ρ=0.5. From the results, we can see that the system OP of the destination node D1 significantly decreases with the rising of b2. However, the system OP of the destination node D2 decreases when a2 increases from 0.55 to 0.7 and after that, has a massive increase with the remaining values of b2. In the same way, the system OP versus α is drawn in Figure 4. In this simulation, we set η=0.8, ψ=7 dB, ρ=0.5, and b2=0.9, b1=0.1. As shown in Figure 4, we can state that the OP of the model system has a slight decrease when α varies from 0 to 1. In both Figure 3 and Figure 4, the simulation and analyticalresults are the same wit hall values of α and b2. Figure 3. OP versus b2 Figure 4. OP versus α
  • 6. Bulletin of Electr Eng & Inf ISSN: 2302-9285  Adaptive relaying protocol forwireless energy harvesting and information processing… (Phu Tran Tin) 99 Furthermore, we investigate the effect of η and ψ on the OP of the model system, as plotted in Figure 5 and Figure 6. In these Figure, we set the primary parameters as a2=0.7, 0.9, R1=R2=0.5 bps/Hz, PS/N0=0.5. From Figure 5 and Figure 6, it can be observed that the system OP has a slight decrease when η varies from 0 to 1, and the system OP crucially decreases with the rising of ψ from 0 to 25. In all two Figure, the analytical and simulation results agree well with each other. On another hand, the comparison of the system OP of two destination nodes is demonstrated in all Figure. From the results, we can state that the system OP of the destination node D2 is better than the destination node D1. Figure 5. OP versus η Figure 6. OP versus ψ 5. CONCLUSION In this research, we propose the ARP For wireless energy harvesting and information processing in NOMA systems. Firstly, we investigate and derive the closed-form and integral form expression of the outage probability (OP) of the model system. Then, all the results are convinced by Monte Carlo simulation in connection with all primary system parameters. From the results, we can convince that all the analyticaland simulation results are the same in connection with the primary system parameters. ACKNOWLEDGEMENTS This research was supported by National Key Laboratory of Digital Control and System Engineering (DCSELAB), HCMUT, VNU-HCM, Vietnam. REFERENCES [1] S. Bi, C. K. Ho, and R. Zhang, "Wireless powered communication: opportunities and challenges," in IEEE Communications Magazine, vol. 53, no. 4, pp. 117-125, April 2015. [2] D. Niyato, D. I. Kim, M. Maso, and Z. Han, "Wireless powered communication networks: research directions and technological approaches," in IEEE Wireless Communications, vol. 24, no. 6, pp. 88-97, Dec 2017. [3] H. Yu, H. Lee, and H. Jeon, "What is 5G? Emerging 5G mobile services and network requirements," Sustainability, vol. 9, no. 1848, pp. 1-22, 2017. [4] M. Duarte, C. Dick, and A. Sabharwal, "Experiment-driven characterization of full-duplex wireless systems," in IEEE Transactions on Wireless Communications, vol. 11, no. 12, pp. 4296-4307, Dec 2012. [5] W. C. Y. Lee, "The most spectrum-efficient duplexing system: CDD," in IEEE Communications Magazine, vol. 40, no. 3, pp. 163-166, March 2002. [6] C. Wang et al., "Cellular architecture and key technologies for 5G wireless communication networks," in IEEE Communications Magazine, vol. 52, no. 2, pp. 122-130, Feb 2014. [7] Z. Ding, P. Fan, and H. V. Poor, "Impact of user pairing on 5G nonorthogonal multiple-access downlink transmissions," in IEEE Transactions on Vehicular Technology, vol. 65, no. 8, pp. 6010-6023, Aug 2016. [8] S. Timotheou and I. Krikidis, "Fairness for non-orthogonal multiple access in 5G systems," in IEEE Signal Processing Letters, vol. 22, no. 10, pp. 1647-1651, Oct 2015.
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