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Secrecy Capacity for Full-Duplex Massive MIMO Relaying Systems With Low-Resolution

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Secrecy Capacity for Full-Duplex Massive MIMO Relaying Systems With Low-Resolution

ADCs

Bridget Durowaa Antwi-Boasiako and Kyoung-Jae Lee

Department of Electronics and Control Engineering, Hanbat National University, 125 Dongseo-daero, Yuseong-gu, Daejeon, Korea

Emails: [email protected], [email protected]

Abstract—In this paper, we consider an amplify-and- forward (AF) full duplex (FD) massive-antenna relay (or base station) aiding communication between K single-antenna source and destination pairs whose transmissions are over- heard by one single-antenna eavesdropper. Maximum ratio combining (MRC) and maximum ratio transmission (MRT) processing is employed at the relay. The secrecy performance of the system is then derived with both relay and destination being equipped with low resolution analog-to-digital convert- ers (ADCs). The results show the detrimental effect of the eavesdropper’s presence on the sum rate of the system.

I. INTRODUCTION

Fifth generation (5G) communication systems are gain- ing lots of traction in recent years. 5G promises very high data rate, low latency and provides support for many devices. 5G will incorporate full duplex (FD) systems, where transmission and reception of data is done simulta- neously to theoretically double the spectral efficiency. Also technologies like massive MIMO, where many antennas are deployed at the base station to serve users, will be used to further enhance the 5G system performance. The issue of high hardware cost and power consumption could be curbed by using analog-to-digital converters (ADCs) with low resolution. The peformance loss due to quantization in low ADCs can be compensated for by the large number of antennas employed [1].

Wireless communication requires secured links to pre- vent interception of signals. FD systems could help im- prove secrecy and also the use of large scale antennas in massive MIMO systems allows simple beamforming techniques to be applied to enhance secrecy [2]. It has also been shown that the amplify-and-forward (AF) relaying scheme could achieve better security performance [3].

The main contribution of this paper is to derive the closed-form ergodic secrecy rate by employing MRC/MRT beamforming technique at the AF massive antenna relay in order to study the effect of the eavesdropper presence on the system rate.

II. SYSTEMMODEL

Figure 1 considers a massive MIMO AF relaying sys- tem, where a FD relay (R) with M -massive receive and transmit antennas helps K single antenna-pair users (Sk, Dk) communicate, while an eavesdropper (E) tries to intercept the transmission between R and the destination (D).

Signal

psxs,k[i] is transmitted from each source Sk

to R in thei-th time slot. The previously received signal

Fig. 1. FD massive MIMO AF relaying model with eavesdropper

˜

yR at R is processed with a linear processing matrix F and amplified to give signal xR. The relay then forwards xR to D. E tries to eavesdrop on transmission between R and D. The signals received at R (after some form of self-interference mitigation), D and E are respectively expressed as

yR[i] =

PsGSRxS[i] + GRRˆxR[i] + nR[i], (1) yD[i] = GTRDxR[i] + nD[i], (2) yE[i] = gRET xR[i] + nE[i], (3) where GSR ∈ CM×K with kth column gSR,k CN (0, βSR,kIM) and GRD ∈ CM×K withk-th column gRD,k∼ CN (0, βRD,kIM) are channels from S to R and from R to D respectively.

g,k= ˆg,k+ e,k, (4)

ˆ

g,k has variance σ,k = ατpppβ2,k

1 + τpppβ,k and e,k has variance ˜σ,k = β,k+ (1 − α)τpppβ,k2

1 + τpppβ,k , and  ∈ (SR, RD). The eavesdropper channel is given by gRE CM×1 ∼ CN (0, βREIM). ¯GRR ∈ CM×M is the loop interference channel, nR[i], nD[i] and nE[i] denote the noise at R, D, and E respectively and are i.i.d.CN (0, 1).

xR[i] = γF˜yR[i − d] with γ being the amplification con- stant and MRC/MRT processing matrix F = ˆGRDHSR. E{ˆxR[i]ˆxHR[i]} = P RMIM.

Because low ADCs are used at both R and D, the quantized versions of the signals at the receivers of R and Dk with linear gainα and distortion factor θ are given by

˜

yR[i] = αyR[i] + ˜nR[i], (5) y˜D,k[i] = θyD,k[i] + ˜nD,k[i], (6)

286

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where ˜nR[i] and ˜nD,k[i] denote quantized versions of the noise at R and Dkrespectively with covariance given by

Rn˜R[i]= α(1 − α)diag E

yR[i]yR[i]H

, (7) R˜nD,k[i]= θ(1 − θ)diagE

|yD,k[i]|2

. (8)

III. SECRECYRATEANALYSIS

Assuming Dk only has statistical knowledge of the channel, the received signal is expressed as in [1].

y˜D,k[i] = αθγ√

pSEgTRD,kFgSR,k

xS,k[i − d]

+ n  effk [i]

effective noise

(9)

neffk [i] = αθγ√ pS

gTRD,kFgSR,k− E

gTRD,kFgSR,k

xS,k[i − d] + αθγ√ pS

j=k

gTRD,kFgSR,jxS,j[i − d]

 

interpair interference

+ αθγgRD,kT FGRRˆxR[i − d]

 

loop interference

+ αθγgRD,kT FnR[i − d]

 

noise at the relay

+ θγgTRD,kF˜nR[i − d]

 

quantization noise at at Rk

+ θn  D,k[i]

noise at Dk

+   ˜nD,k[i]

quantization noise at Dk

.

(10) Assuming E has perfect knowledge of its own channel, the received signal at E is given by

y˜E[i] = αθγ√

pSgTREFgSR,kxS,k[i − d]

+ αθγ√ pS

j=k

gTREFgSR,jxS,j[i − d]

+ αθγgTREFGRRˆxR[i − d] + αθγgRET FnR[i − d]

+ θγgRET F˜nR[i − d] + nE[i], (11) where the first terms of (9) and (11) are the desired signals and the remaining terms are effective noise components.

The secrecy rate of the k-th user in AF FD massive MIMO relaying with low ADCs can be expressed as

secRk= [Rk− RE]+, (12) where [x]+= max(x, 0), Rkis the rate at the destination Dk whose solution is given in [1] andRE is the rate at the eavesdropper E.

RE = τc− 2τp

τc log(1 + SINRE), (13) where we define

SIN RE= Aeve

Ceve+ Deve+ Feve+ Geve, (14) Aeve= psM3βREσ2RDkσ4SRk

+ psM2βREσ2RDkσ2SRkβSRk, Ceve= M2βREk K

j=kβSRj K

n=k,jσRDn2 σ2SRn, + M2βREkσRDk2 σSRk2 K

j=kβSRj

+ M3βREk K

j=kσ2RDjσ4SRj + M2βREk K

j=kσ2RDjσ2SRjβSRj, Deve= pRM2LI2 + 1)βRE K

j=1σRDj2 σSRj2 , Feve=1−αα (M2βRE K

n=1σRDn2 σ2SRn,

× [σ2SRn+ K i=1βSR,i] + M2βRE(pRσ2LI+ 1) K

n=1σ2RDnσSRn2 ).

Fig. 2. Simulation vs analytic secrecy rate

Fig. 3. Sumrate vs power

IV. NUMERICALRESULTS

In this section, we confirm the results derived above by setting the coherence interval τc = 196 symbols, K = 5, τp = K, βSR,k = βRD,k = βRE = 1, and σn2R = σn2D = 1, σ2LI = 0dB, and ps = pR = pp = 10dB, θ = α = 0.8825. Figure 2 compares the result in (12) with the Monte-Carlo simulation result. Both results match tightly as the number of antennas increase, thus confirming our results.

The secrecy sum rate is then plotted against the sum rate in [1]. Figure 3 shows that the presence of the eavesdropper caused a decrease in sum rate as expected which has to be investigated and be further improved.

REFERENCES

[1] C. Kong, C. Zhong, S. Jin, S. Yang, H. Lin, and Z. Zhang, “Full- duplex massive MIMO relaying systems with low-resolution adcs,”

IEEE Transactions on Wireless Communications, vol. 16, pp. 5033–

5047, Aug. 2017.

[2] J. Chen, X. Chen, W. H. Gerstacker, and D. W. K. Ng, “Resource allocation for a massive MIMO relay aided secure communication,”

IEEE Transactions on Information Forensics and Security, vol. 11, pp. 1700–1711, Aug. 2016.

[3] X. Chen, L. Lei, H. Zhang, and C. Yuen, “Large-scale MIMO relaying techniques for physical layer security: Af or df?,”IEEE Transactions on Wireless Communications, vol. 14, pp. 5135–5146, Sept. 2015.

한국정보통신학회 2019년 춘계 종합학술대회 논문집

287

수치

Figure 1 considers a massive MIMO AF relaying sys- sys-tem, where a FD relay (R) with M -massive receive and transmit antennas helps K single antenna-pair users (S k , D k ) communicate, while an eavesdropper (E) tries to intercept the transmission between
Fig. 2. Simulation vs analytic secrecy rate

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