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signal processing from power amplifier operation control point of view

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14 INTRODUCTION<br />

is the "channel" response, which includes the symbol waveform at the transmitter<br />

as well as the medium response.<br />

1.3.2.1 Noise and interference models The term n(t) models noise. Here we will<br />

assume this noise is additive, white Gaussian noise (AWGN). Such noise is implicitly<br />

assumed to have zero mean, i.e.,<br />

m n (i) = E{n(i)}=0. (1.25)<br />

The term "white" noise means two things. First, it means that different samples<br />

of the noise are uncorrelated. It also means that its moments are not a function of<br />

time. That is, the covariance function is given by<br />

C n (h,h) â Ε{[η(ίι) - m n {h)\[n*{t 2 ) - m* n {t 2 )\) = N a 6 D (U - h), (1.26)<br />

where 5r>{r) denotes the Dirac delta function (a unity-area impulse at τ = 0).<br />

Another implicit assumption with AWGN is that it is proper, also referred to<br />

as circular. This has to do with the relation between the real and imaginary<br />

parts of an arbitrary noise sample n(i () ) = n = n r + jn,. With circular noise,<br />

the real and imaginary components of n(io) are uncorrelated and have the same<br />

distribution. With AWGN, this distribution is assumed to be Gaussian, which is a<br />

good model for thermal noise. A circular, complex Gaussian random variable (r.v.)<br />

has probability density function (PDF)<br />

where m n is the mean, assumed to be zero, and TVo is the one-sided power spectral<br />

density of the original radio signal (noise on the I and Q components has variance<br />

σ 2 = 7V()/2). If we write n — n r + jrii, where n r and n¿ are real random variables,<br />

then n r is Gaussian with PDF<br />

1 J-(x m, 12<br />

/„„ (x) = -== exp<br />

V7r7V 0 L Λ/ 0 J<br />

and has cumulative distribution function (CDF)<br />

v<br />

Tl<br />

(1.28)<br />

F nr (x)àp T {n r

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