Ber Calculation
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BER calculation
Vahid Meghdadi
reference: Wireless Communications by Andrea Goldsmith
January 2008
- SER and BER over Gaussian channel
- BER for BPSK modulation
In a BPSK system the received signal can be written as:
y = x + n | (1) |
where x 2 f A; Ag, n CN (0; 2) and 2 = N0. The real part of the above equation is yre = x + nre where nre N (0; 2=2) = N (0; N0=2). In BPSK constellation dmin = 2A and b is de ned as Eb=N0 and sometimes it is called SNR per bit. With this de nition we have:
b := | Eb | = | A2 | = | dmin2 | (2) | |||||||||
4N0 | |||||||||||||||
N0 | N0 | ||||||||||||||
So the bit error probability is: | |||||||||||||||
Pb = P fn > Ag = Z | 1 | 1 | e | x2 | (3) | ||||||||||
2 2=2 | |||||||||||||||
A | 2 2=2 | ||||||||||||||
This equation can be simpli ed using Q- | function as: | ||||||||||||||
p |
0 1
s
d2
Pb = Q @ min A = Q
2N0
where the Q function is de ned as:
Q(x) = p1 2
dmin | |||||||
= Q p | 2 b | ||||||
p | (4) | ||||||
2N0 | |||||||
Zx1 | e | x2 | dx | (5) | |||
2 |
- BER for QPSK
QPSK modulation consists of two BPSK modulation on in-phase and quadrature components of the signal. The corresponding constellation is presented on gure 1. The BER of each branch is the same as BPSK:
p
Pb = Q 2 b (6)
1
[pic 1]
Figure 1: QPSK constellation
The symbol probability of error (SER) is the probability of either branch has a bit error:
p
Ps = 1 [1 Q 2 b ]2 (7)
Since the symbol energy is split between the two in-phase and quadrature com-ponents, s = 2 b and we have:
Ps = 1 [1 Q (p | )]2 | (8) | ||
s |
We can use the union bound to give an upper bound for SER of QPSK. Regard-ing gure 1, condition that the symbol zero is sent, the probability of error is bounded by the sum of probabilities of 0 ! 1, 0 ! 2 and 0 ! 3. We can write:
Ps | Q(d01= 2N0) + Q(d02= | 2N0) + Q(d03= | 2N0) | (9) | |||||||||||
= | 2Q(A= p | ) + Q(p2A=p | ) | p | (10) | ||||||||||
N0 | 2N0 | ||||||||||||||
p | p | ||||||||||||||
Since s = 2 b = A2=N0, we can write: | |||||||||||||||
Ps 2Q(p | ) + Q(p | ) 3Q(p | ) | ||||||||||||
2 s | (11) | ||||||||||||||
s | s |
Using the tight approximation of Q function for z 0:
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