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signal processing from power amplifier operation control point of view

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74 LINEAR EQUALIZATION<br />

What if we could use r-.ι, as well? There is a copy of s 2 that would be helpful.<br />

However, there is an even larger copy of s,¡. With the zero-forcing strategy, we<br />

found it best not to use r,-¡ because of the larger copy of s;j. However, with the<br />

MMSE strategy, it turns out that r :i is useful. We will explore this more in the<br />

next chapter.<br />

4.2 MORE DETAILS<br />

So far we have explored partial zero-forcing and MMSE. For partial zero-forcing, a<br />

better approach would be to minimize ISI, accounting for ISI not canceled. This<br />

approach is explored in the Problems section. As for the MMSE solution, here we<br />

provide more details. Then a maximum SINR solution is developed. It is shown<br />

that the MMSE solution also maximizes SINR. Results are then generalized for the<br />

dispersive and MIMO scenarios.<br />

4.2.1 Minimum mean-square error solution<br />

Consider the MMSE solution. In (4.16), we found that the MSE for the dispersive<br />

channel example is given by<br />

E 2 = (w 2 (-10) - l) 2 + (w 2 (9) + wi(-10)) 2 + ( Wl 9) 2 + {w\ + w|)100. (4.17)<br />

We used trial-and-error plots to find the weights that minimized MSE.<br />

There is another way to find such weights. In the plots, we were looking for the<br />

minimum of the MSE. At the minimum, the instantaneous slope of the curve is<br />

zero. From differential calculus, we know that the instantaneous slope is given by<br />

the derivative. Thus, we can take the derivative of E 2 with respect to each weight<br />

and set the derivatives to zero.<br />

For this particular example, it will help to recall the following facts from differential<br />

calculus.<br />

1. The derivative of ax 2 + bx + c with respect to (w.r.t.) x is 2ax + b.<br />

2. The derivative of (ax + d) 2 w.r.t. x is 2a(ax + d).<br />

3. When we take the derivative w.r.t. one variable, we treat the other variable<br />

as a constant.<br />

Using these facts, we can take the derivative of E 2 w.r.t. w\ and ω 2 and set the<br />

results to zero. This gives<br />

0 = 0 + 2(-10)(u) 2 (9)+wi(-10)) + 2(u> 1 9)+2(w 1 )100 (4.18)<br />

0 = 2(-10)(w 2 (-10) - 1) + 2(9)(w 2 (9) + wi(-10)) + 0 + 2(w 2 )100. (4.19)<br />

Solving these two equations gives w\ = —0.0127 and w 2 = —0.0397. Substituting<br />

these results into the MSE equations gives an MSE of 0.603.<br />

As for computing SINR, substituting (4.13) into (4.14) gives<br />

2 2 = W 2 (-10)S2 + (Wl(—10) + W 2 9)si + Wl9S() + Wim + W2H2- (4.20)

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