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signal processing from power amplifier operation control point of view

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MORE MATH 89<br />

values of h k m (f) from all symbol periods, though practically the values in a window<br />

around mo would be the most influential. Thus, the weights may depend on mo,<br />

the symbol period, and fco, the PMC. For CDM, this means that there will be a<br />

different weight solution for each symbol being detected. For OFDM, the values of<br />

c k m(") are * ne same for different values of m and i. Thus, there will be a weight<br />

vector for each subcarrier fc. This set of weight vectors can be reused for different<br />

symbol periods m.<br />

The MMSE weight solution is obtained by solving (4.77), which can be written<br />

as<br />

C(mo)w = (7£< io) (fco)) hltL- (4.114)<br />

where<br />

h (in)<br />

fco."ID<br />

[^:L(^T S )] T ... [h^rao (A J _ 1 T.)] T ] T . (4.115)<br />

4.4.3 ML solution<br />

The ML formulation for the general case is similar to the ML formulation for the<br />

TDM case. As before, the end result is that C„ is replace with C„ in the weight<br />

solution. Specifically, the ML weights are given by<br />

C u (m n )w = (ν^'(mo) = p^R-V (4.118)<br />

where<br />

= E l Ä J ' W ^ ' W j ^ C - ^ , (4.119)<br />

71=0<br />

Î^\nT c ) = \A# 0) (M i[h ( ' r,) (AoT s - nT c )] T ... [h^(Aj^T s - nT c )] T ~\<br />

(4.120)<br />

and Ec ' (fco) = E¡¡ (ko)/N c is the energy per chip for code fco. Observe that<br />

there is despreading being performed in (4.119). Also, there appears to be multiple<br />

weight vectors, one for each chip period.<br />

We can rewrite these equations as<br />

^"»(mo) = y/Ep\ko) ¿ [c^J'W^W, (4-121)

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