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Practical Implementation of PN Scrambler for PAPR Reduction

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The probability that the power W > L occurs at least m=1<br />

time out <strong>of</strong> N samples is<br />

Pr{A occurs at least 1 time in N samples} =<br />

N ⎛ N ⎞ i N −i<br />

∑= ⎜ ⎟ ⋅ p q<br />

i 1 ⎝ i ⎠<br />

(19)<br />

In order to simplify the equation, note that the probability<br />

W > L occurs at least m=1 time out <strong>of</strong> N samples is the<br />

same as the complementary probability that exactly no<br />

samples (m=0) have W > L, which can be written as<br />

1-Pr{A occurs exactly 0 times out <strong>of</strong> N samples} =<br />

⎛ N ⎞ N<br />

N<br />

N<br />

1−<br />

g N ( 0)<br />

= 1−<br />

⎜ ⎟ ⋅ p q = 1−<br />

q = 1−<br />

( 1−<br />

p)<br />

= 1−<br />

F<br />

⎝ 0 ⎠<br />

0 N<br />

W ( L)<br />

(20)<br />

Thus, we now define the CCDF <strong>of</strong> the peak power per<br />

OFDM symbol as the probability that the peak power <strong>of</strong><br />

one sample out <strong>of</strong> N samples exceeds threshold L<br />

N<br />

⎛ ⎛ L ⎞⎞<br />

Fsym = Pr{<br />

PeakPowerOFDM<br />

_ Symbol > L}<br />

= 1−<br />

⎜1<br />

− exp⎜<br />

− ⎟⎟<br />

2<br />

⎝ ⎝ 2 ⋅σ<br />

⎠⎠<br />

(21)<br />

Using the <strong>PN</strong> scrambler to generate k OFDM symbols and<br />

then selecting the OFDM symbol with the lowest <strong>PAPR</strong><br />

<strong>for</strong> transmission reduces the peak power probability to p k .<br />

For example, if an OFDM symbol has the probability <strong>of</strong><br />

p=0.1 <strong>of</strong> exceeding threshold L, then the probability <strong>of</strong> k=2<br />

OFDM symbols exceeding threshold L is (0.1) 2 =0.01.<br />

This is true because <strong>of</strong> the statistical independence <strong>of</strong> the<br />

peak power between OFDM symbols generated by the <strong>PN</strong>-<br />

<strong>Scrambler</strong> (i.e. uncorrelated data sets). That is, if the<br />

probability <strong>of</strong> event S1 does not depend upon the outcome<br />

<strong>of</strong> S2 and visa versa, such events are said to be statistically<br />

independent and<br />

Pr(S , S )<br />

=<br />

1<br />

2<br />

2<br />

= Pr(S1)<br />

⋅ Pr(S2)<br />

= p ⋅ p p (22)<br />

For k statistically independent events, this becomes<br />

Pr(S , S ,..., S )<br />

=<br />

1<br />

2<br />

k<br />

k<br />

= Pr(S1)<br />

⋅Pr(S2<br />

) ⋅⋅⋅<br />

Pr(Sk<br />

) = p⋅<br />

p⋅<br />

⋅⋅<br />

p p (23)<br />

For k scrambling sequences, the new <strong>PAPR</strong> CCDF per<br />

OFDM symbol can now be <strong>for</strong>mally written as<br />

Pr<br />

{ <strong>PAPR</strong> k > L}<br />

OFDM _ Symbol sequences<br />

N<br />

⎛<br />

⎞<br />

⎜ ⎛ ⎛ L ⎞⎞<br />

= 1−<br />

⎜1−<br />

exp⎜<br />

− ⎟⎟<br />

⎟<br />

⎜<br />

2<br />

2 ⎟<br />

⎝ ⎝ ⎝ ⋅σ<br />

⎠⎠<br />

⎠<br />

k<br />

2 1<br />

σ =<br />

2<br />

(24)<br />

Substituting equation (13) into (21) yields<br />

F = 1 − F<br />

N<br />

(25)<br />

sym<br />

W<br />

4 <strong>of</strong> 7<br />

Rearranging, the sample-based power distribution is<br />

related to the OFDM symbol-based peak power<br />

distribution by<br />

( ) N<br />

1<br />

FW<br />

= 1− F<br />

(26)<br />

sym<br />

Next, we define the new <strong>PAPR</strong> distribution Fsym ˆ as the<br />

OFDM symbol-based peak-power distribution after k<br />

scrambling sequences<br />

k<br />

N k<br />

F ˆ<br />

sym = Fsym<br />

= ( 1 − FW<br />

)<br />

(27)<br />

Finally, in order to determine FW ˆ , which is the new <strong>PAPR</strong><br />

reduced sample-based power distribution after application<br />

<strong>of</strong> k scrambling sequences, we simply substitute Fsym ˆ into<br />

equation (26) relating the sample-based power distribution<br />

to the OFDM symbol-based peak power distribution,<br />

Fˆ<br />

W<br />

=<br />

1<br />

N<br />

N k<br />

( 1 − Fˆ<br />

) = ( 1 − ( 1 − F ) )<br />

sym<br />

W<br />

1<br />

N<br />

1<br />

N<br />

k N<br />

⎛<br />

⎞<br />

⎜ ⎛<br />

L ⎞<br />

1 ⎜ ⎛ ⎛ ⎞⎞<br />

⎟<br />

= ⎜ − 1 − ⎜1<br />

− exp⎜<br />

− ⎟ ⎟<br />

2 ⎟<br />

2<br />

⎟<br />

⎜ ⎜<br />

⎟ ⎟<br />

⎝ ⎝ ⎝ ⎝ ⋅σ<br />

⎠⎠<br />

⎠ ⎠<br />

(28)<br />

In the above equation, FW ˆ is the CDF <strong>of</strong> the <strong>PAPR</strong><br />

reduced sample-based distribution using k-scrambling<br />

sequences, which is the probability that each individual<br />

sample’s peak power is less than or equal to threshold<br />

level L using an IFFT size <strong>of</strong> N. It is more useful to<br />

evaluate the probability that each individual sample’s peak<br />

power is greater than threshold level L, which is the<br />

complementary CDF, CCDF=1-CDF.<br />

1<br />

k<br />

N<br />

N<br />

⎛<br />

⎞<br />

⎜ ⎛<br />

L ⎞<br />

CCDF(<br />

L,<br />

N,<br />

k)<br />

1 1 ⎜ ⎛ ⎛ ⎞⎞<br />

⎟<br />

= − ⎜ − 1−<br />

⎜1−<br />

exp⎜<br />

− ⎟ ⎟<br />

2 ⎟<br />

2<br />

⎟<br />

⎜ ⎜<br />

⎟ ⎟<br />

⎝ ⎝ ⎝ ⎝ ⋅σ<br />

⎠⎠<br />

⎠ ⎠<br />

(29)<br />

After normalization <strong>of</strong> the complex time-domain signal’s<br />

average power<br />

<strong>PAPR</strong><br />

CCDF<br />

1<br />

N k N<br />

= 1−<br />

⎜<br />

⎛1− ( 1−<br />

( 1−<br />

exp(<br />

− L)<br />

) ) ⎞ (30)<br />

( L,<br />

N,<br />

k)<br />

⎟<br />

⎝<br />

⎠<br />

It is important to note that due to the equivalence<br />

theorem, the analysis and linear signal processing <strong>of</strong><br />

baseband wave<strong>for</strong>m presented herein will be identical to<br />

the analysis <strong>of</strong> the bandpass wave<strong>for</strong>m with the exception<br />

<strong>of</strong> oversampling error. A rigorous discussion <strong>of</strong> the <strong>PAPR</strong><br />

measurement error due to Nyquist sampling versus<br />

continuous sampling can be found in [10]. Because most<br />

applications are typically concerned with the probability<br />

that a signal’s power exceeds a certain level L, instead <strong>of</strong><br />

using the CDF, the CCDF is typically plotted and is shown<br />

in Fig. 3 <strong>for</strong> FFT sizes N=64, N=128, N=256 and number<br />

<strong>of</strong> scrambling sequences k=1 (i.e. no <strong>PAPR</strong> reduction),<br />

k=8, and k=256. The plot shows both the theoretical<br />

curves obtained using equation (30) and the empirical<br />

curves obtained through computer simulations.

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