- Open Access
- Total Downloads : 189
- Authors : Karine B. Carbonaro, Gilberto A. Carrijo
- Paper ID : IJERTV4IS070735
- Volume & Issue : Volume 04, Issue 07 (July 2015)
- Published (First Online): 28-07-2015
- ISSN (Online) : 2278-0181
- Publisher Name : IJERT
- License: This work is licensed under a Creative Commons Attribution 4.0 International License
Analysis of Cross M- QAM OFDM systems under Gaussian and Impulsive Noise
Carbonaro, K. B. and Carrijo, G. A. Faculty of electrical engineering Federal University of Uberlândia
Patos de Minas, Brazil
AbstractPower line communications (PLC) allows establishing a digital communications without adding any new wires. However, the power line channel was not originally meant to be used for communications and it is a difficult channel for several reasons, for example, it has high noise. This paper derives the exact symbol error probability (SEP) for cross quadrature amplitude modulation with orthogonal frequency division multiplexing (M-QAM/OFDM) systems over Gaussian and impulsive noise. Analytical performances are evaluated and compared with computational simulations, which show good agreement.
KeywordsM-QAM, OFDM, Gaussian noise, impulsive noise, SEP.
-
INTRODUCTION
impulsive noise. In Section V, numerical results of the SEP performance of the cross M-QAM/OFDM system are presented. Finally, Section VI gives conclusion.
-
COMBINED NOISE MODEL
Both background noise and impulsive noise are considered when studying the effects of impulsive noise on PLC as their effects differ from that on the OFDM system.
-
Gaussian Noise
Assuming background noise is considered to be additive white Gaussian noise with potential spectral density (PSD) can be expressed as [2]
The power line communication (PLC) provides a high data
S (f) = 2 N0 = kTe [W / Hz]
transmission rate using quadrature amplitude modulation (QAM) presenting high bandwidth efficiency. If there is a requirement for the transmission of an odd number of bits per symbol, the rectangular QAM is not a good choice in terms of
w
where,
w 2 2
power efficiency. The cross-QAM constellation has been found to be useful in adaptive modulation schemes wherein the constellation size is adjusted depending on the channel quality. For the latter, as the channel quality improves, the constellation size should be from 2b to 2b+2 if only the square QAM were used. By using cross QAM, however, the increments can be changed from 2b to 2b+1, which allows for more granularities [1]. Cross-QAM is of current interest for employment in adaptive orthogonal frequency division
multiplexing (OFDM) systems.
k – the Boltzman´s constant (1,38.1023 [J/k]),
Te – the system temperature [k],
w
mw – mean zero 2 2 – variance.
The noise is Gaussian with a probability density function (PDF) defined as follows
1 -(x – m )2
G(x, m , 2 ) = exp w
w
Various research results available in the technical literature evidence that the properties of the noise affecting indoor power line channels. OFDM can perform better than single carrier when the channel is interfered by impulsive noise, because it spreads the effect of impulsive noise over multiple
w w
-
Impulsive Noise
w 2
22
symbols due to discrete Fourier transform (DFT) algorithm.
Therefore, in this paper, we present exact expression for the symbol error probability (SEP) of cross M-QAM and OFDM systems for the channel with Gaussian and impulsive
The impulsive noises have a behavior in time similar to a sinusoidal wave, with peak values declining exponentially. The occurrence is a Bernoulli process while the amplitudes are modeled as a Gaussian process as follows:
noise.
The remaining part of this paper is organized as follows. In Section II, the combined noise model is presented. The formulas for the SEP of cross M-QAM are derived in section
-
-
Section IV presents a generalized performance expression form OFDM system, taking the effects of the Gaussian and
ik = Bk .gk
where, Bk is the Bernoulli process, sequence of zeros and ones
The energy of the individual alphabets is
with
Pr (Bk
1) p
and
gk is complex white Gaussian
m 3 M
m 3 M
4 2 4 2
i
noise with mean zero, variance 2 2 and the PSD is given by
E1
m1
| (2m 1) j(2m 1) |2 2
m1
| (2m 1) |2
2 Ni
2 s(4s2 1) 1
M 9M 1
Si ( f ) i
3 2
2 8
2
2
M
The presence of impulsive noise may lead to severe deterioration in communication performance at PLC receivers.
-
Model
each alphabet is used 3 times in the cross M-QAM constellation and total energy { E1T } is given by
All of the above random sequences are assumed to be
1
M 9M
M 3M 9M
independent of each other. This model can be physically
E1T 2
2 8
1 .3
2 4 8
1
thought of as each transmitted data symbol being hit independently by an impulsive with probability p and with random amplitude. Hence, the combined noise seen by the receiver is [3].
The 128-QAM constellation is shown in the Fig. 1.
where,
nk nkR jnkI wk ik
nk – noise with real and imaginary part,
wk – Gaussiano noise,
ik – impulsive noise.
The ratio between the noises is
Ni
N0
and the total noise is a random variable with variance described as follows
2 2 2 N0 Ni N0 1
m w i
2 2 2
Fig. 1 Cross 128-QAM constellation modified [4].
-
SEP OF CROSS-M-QAM
QAM is extensively used modulation scheme in which
There are non-constellation individual alphabets {±11±j11,
±11±j9, ±9±j11, ±9±j9} and the energy is
both amplitude and phase will carry information. The 3 M
constellation has M = 2b symbols, where the number of bits in each constellation symbol is b [4]. In the cross M-QAM
m
4 2
E 2
(2m 1)2
13 M 4 2 M
constellation, b is an odd integer. The alphabet was created in the range m
2
m 1
M 1 4 2
(2m 1)
j(2m 1)
m
3 M
2 2
M
M QAM
1,…, 4 2
and each alphabet is used
times in the cross M-
2
±11±j11
±11±j9
±11±j7
±11±j5
±11±j3
±11±j1
±9±j11
±9±j9
±9±j7
±9±j5
±9±j3
±9±j1
±7±j11
±7±j9
±7±j7
±7±j5
±7±j3
±7±j1
±5±j11
±5±j9
±5±j7
±5±j5
±5±j3
±5±j1
±3±j11
±3±j9
±3±j7
±3±j5
±3±j3
±3±j1
±1±j11
±1±j9
±1±j7
±1±j5
±1±j3
±1±j1
QAM constellation and total energy { E2T } is given by
13 M M
E2T 4 M 4 2 2 . 2
M 26M 32 M
128
128 M
The average energy from M constellation symbols
Região de integração
{ EM QAM (Cross) } is the sum of (10) and (12) divided by M. The aveage energy can be evaluated by
The symbol in the inside is decoded correctly with the region's integration within the limits, Fig. 3.
E E 1
128
region of integration
EM QAM (Cross) 1T 2T
M
128 82M M
128
M
k Es nkR k Es
k Es nkI k Es
The average energy and scaling factor {k} are tabulated in Table I.
TABLE I. SCALING FACTOR.
M-QAM
EM-QAM(Cross)
Scaling factor (k)
32-QAM
20
1/20
128-QAM
82
1/82
512-QAM
330
1/330
Fig. 3 – The limits of integration to the symbols with four neighbors.
The limits of integration are applied in (15) and the probability of error of symbol in the inside is given by
There are three types of constellation symbols in a non-
p (N )
Es
2 Es
square M-QAM constellations as depicted in Fig. 1.
Constellation points in the corner: has two neighboring symbols. The number of constellation points in the corner in any cross M-QAM constellation is always 8.
e 4 2erfc k erfc k
N N
0 0
Constellation points neither at the corner, nor at the center: has three neighboring symbols. The number of constellation points in the neither at the corner, nor at the center in any
N2 8
cross M-QAM constellation is
The symbol in the corner is decoded correctly with the region's integration within the limits, Fig. 2.
N3 3 2M 16
k Es *
region of integration
Região de integração
k Es nkR
k Es nkI
The symbol in the neither at the corner, nor at the center is
decoded correctly with the region's integration within the limits, Fig. 4.
Região de integração
region of integration
* k Es * *
k Es nkR
k Es
* k Es nkI k Es
*
Fig. 2 – The limits of integration to the symbols with two neighbors.
The limits of integration are applied in the probability distribution function
k Es
Fig. 4 – The limits of integration to the symbols with three neighbors.
e
k E
k E
n R I R I
P 1 k Es k Es p (n
, n )dn dn
The probability of error of symbol in the neither at the
corner, nor at the center is defined as
s s
and the probability of error of symbol in the corner is given
3 E 1 2
E
by pe (N3 )
erfc k
2
s
N0
erfc k s
N
2 0
p (N )
Es 1 2
Es
The Symbol Error Probability (SEP) of cross M-QAM
e 2 erfc k N 4 erfc k N
follow the logic:
0 0
Constellation points in the inside: has four neighboring symbols. The number of constellation points in the insider in any cross M-QAM constellation is
Pe(M QAMcruz )
eq.(14) (16) (17) (18) (19) (20)
M
N4 M 3 2M 8
combining results leads the exact SEP due to additive white Gaussian noise (AWGN).
P 2 3 2
Es
-
SEP OF CROSS M-QAM
In OFDM multiple sinusoidals with frequency separation
e( M QAMcruz )
2 M erfc k N
1
0 is used and can be defined as [4]
1 2 3 2 2
Es T
M 2
M erfc k N
1 Nc 1
j2 nk
0
sk an exp
The proposed equation will be validated using other published equations. An exact expression to determine the SEP of 32-QAM cross on a channel with Gaussian noise is proposed in [5].
where,
Nc n0 Nc
k 0,1,…, Nc 1
4
E
104
E
sk – transmitted signal,
P Q
A Q A
a – nth symbol in the message,
e 32 10 2 32 20 2 n
w w
N – number of carriers.
92
E
Q2 A
2
c
The signal received {rk} with influence of noise is solved
32
20 w
as follows
N
1 Nc 1
j2 nk
where,
rk
an exp N
w i
A
E 20d 2 – average energy,
-
n0
c
-
– minimum distance between two adjacent points in the constellation.
where,
k 0,1,…, Nc 1
The equations (23) e (24) is an exact intuitive geometric infinite double series for the average symbol error probability of 128-cross-QAM and 512-cross-QAM in additive white
w – Gaussian noise,
i – impulsive noise.
The characteristic function is formulated as
Gaussian noise is derived in [6].
Nc N
c
2 2 2
m 1 2
1
Nk
(1,2 )
m
pm (1 p)Nc m exp
2
e
P 468Q
s 440Q2
s
m0
128
41
41
where, the variance of the combined noise is developed considering the noise and the number of OFDM subcarriers
1
[5].P 1956Q
s 1880Q2
s 2
e 512
165
165
2 2 mi
N0 mNi N0 1 m
m w N
c 2 2Nc 2
Nc
where,
2
Applying (30) into (21) leads to the symbol error probability of cross M-QAM
N
s
Es
0
82d
w
2 2
P 1 N Nc pm
e m
m0
(1 p)Nc m
Applying (6) and (7) into (21) leads to the symbol error
3 2 3 2 2
2
probability of cross M-QAM due to AWGN and impulsive
2 2 M erfc(a) 1 2
M M erfc (a)
noise.
P
2 3 2
k
erfc
Es
-
-
NUMERICAL RESULTS
e( M QAMcross )
2 M
1 N
0
1 2 3 2 erfc2 k Es
In the first stage of simulations, we have verified our exact SEP expressions. The Figs. 5, 6 and 7 presents the results obtained by simulation of cross M-QAM modulations due to
M 2
M
1
N0
AWGN.
1 Cross 32-QAM
10
0
10
-1
10
SEP
-2
10
-3
10
The analysis was made considering SEP {10-5}. The ratio
N0
M=32 equation (21)
M=32 equation (22)
/td> Es was 23,1dB, 29,2dB and 35,3dB in the Figs. 5, 6 and 7,
respectively.
The Figs. 8 and 9 presents the results obtained by simulation of cross M-QAM due to Gaussian and impulsive noises. In the article [7], the authors used the ratio between the Gaussian noise and the impulsive with the value of
w i
{ 2 102 2 }. The results presented in the Fig. 8.
1
10
M=32 M=128 M=512
-4
10 0
10
-5
10 -1
0 5 10 15 20 25 30 35 40 10
Es/N0 [dB]
SEP
Fig. 5 32-cross-QAM. -2
10
1 Cross 128-QAM
M=128 equation (21)
M=128 equation (23)
10
-3
10
0
10
-4
10
-1
10
-5
10
SEP
0 10 20 30 40 50 60
10
-2 Es/N0 [dB]
-3
10
-4
10
-5
10
0 5 10 15 20 25 30 35 40
Es/N0 [dB]
Fig. 6 128-cross-QAM.
The figures shows excellent agreement between our results with other published results for cross 32-QAM [5], 128-QAM and 512-QAM in [6].
1 Cross 512-QAM
M=512 equation (21)
M=512 equation (24)
10
0
10
-1
10
SEP
-2
10
-3
10
-4
10
-5
10
Fig. 8 SEP performances of 32/128/512-QAM with µ=100.
i w
In [3] specify the ratio between the variance of Gaussian noise and impulse { 2 10 2 }. From Fig. 9, it can be seen that the addition of the impulsive noise increased the
N0
ratio Es . The new values are about 33,5dB, 39,6dB and
45,7dB.
To improve the ratio, we add OFDM with 52 subcarriers. The results obtained by simulation of cross M-QAM/OFDM due to Gaussian and impulsive noises are presents in the Figs. 10, 11 and 12. The impulsive noise occurrence probability
ranged from {0.01; 0.1; 1.0}.
1
M=32 M=128 M=512
10
0
10
-1
10
SEP
-2
10
-3
10
-4
10
05 10 15 20 25 30 35 40
Es/N0 [dB]
Fig. 7 512-cross-QAM.
-5
10
0 10 20 30 40 50 60
Es/N0 [dB]
Fig. 9 SEP performances of 32/128/512-QAM with µ=10.
1 1
p=1 p=.1 p=.01
10 10
0 0
10 10
-1 -1
10 10
SEP
SEP
-2 -2
10 10
-3 -3
10 10
p=1 p=.1 p=.01
-4 -4
10 10
-5
10
0 5 10 15 20 25 30 35 40 45 50
Es/N0 [dB]
-5
10
0 5 10 15 20 25 30 35 40 45 50
Es/N0 [dB]
Fig. 10 SEP performances of 32-QAM/OFDM.
From Fig. 10, it can be seen that the new value is about 24 to 34dB. Fig. 11 shows a variation of 30dB to 40dB.
1
10
0
10
-1
10
SEP
-2
10
-3
10
p=1 p=.1 p=.01
-4
10
-5
10
Fig. 12 SEP performances of 512-QAM/OFDM.
-
CONCLUSION
-
In this paper, we have developed form expression for the SEP of cross M-QAM constellations in the presence of Gaussian noise. We have compared the exact SEP expression with other expressions published literature. Then we evaluate the performance of cross M-QAM in the presence of impulsive and AWGN noise. The addition of impulse noise increased a SEP of cross M-QAM. To control the SEP, we use OFDM.
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L. Izzo; L. Panico; L. Paura. Character error probabilities of M-ary noncoherent systems due to additive combinations of Gaussian and impulsive noise. Alta Frequenza, vol. LI, julho Agosto, 1982.
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Es/N0 [dB]
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N0
As has been verified in Fig. 12, the ratio Es
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