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signal processing from power amplifier operation control point of view

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THE MATH 137<br />

sometimes inaccurate when approximations are made. Only in special cases is performance<br />

accurately predicted by a relatively simple analysis. An example is linear<br />

equalization of CDM signals with large spreading factors, in which SINR expressions<br />

are easy to compute, and performance is related directly to SINR because ISI<br />

can be accurately modeled as Gaussian, similar to the noise.<br />

A second approach is to measure performance at the output of the equalizer and<br />

map the result to an effective SINR. Here we will measure symbol error rate. Using<br />

the relations in (A.6) and (A.7), we can determine an effective E s /Nn, which we<br />

will define as output SINR. In practice, these equations are used to generate a table<br />

of SINR and SER values. Interpolation of table values is then used to determine<br />

an effective SINR from a measured SER.<br />

This second approach also has limitations. One limitation is that enough symbols<br />

must be simulated at each fading realization to obtain an accurate estimate of SER.<br />

This can be challenging when the instantaneous SINR is high, so that few, if any,<br />

symbols are in error. This also gives rise to a granularity issue, as we can only<br />

measure error rates of the form 0, 1/N S , 2/N s , etc., where N s is the number of<br />

symbols simulated. These limitations can be overcome by ensuring that N s is large<br />

so that the range of interesting SINR. values corresponds to many error events (recall<br />

the 100 error events rule).<br />

Effective SINR. results were obtained for the TwoTSfade channel by generating<br />

1000 symbols (plus edge symbols not counted) for each of 2000 fading realizations.<br />

In Fig. 6.15, cumulative distribution functions (CDFs) are provided for various<br />

receivers for a 6 dB average received Eb/Na level (9 dB E s /No). Recall that the<br />

CDF value (y-axis) is the probability that the effective SINR is less than or equal<br />

to a particular SINR value (z-axis). Thus, smaller is better. For the MFB, output<br />

SINR was determined via measurement rather than semi-analytically.<br />

Observe that equalization provides a rightward shift in the CDF, making smaller<br />

SINR values less likely (larger SINR values more likely). As expected, the MMSE<br />

DFE provides higher SINR values than the MMSE LE. While difficult to see, the<br />

CDFs cross at low SINR, so that the MMSE DFE has more lower SINR values due<br />

to error propagation. The MFB acts as a lower bound CDF.<br />

Results with power control are given in Fig. 6.16. Relative to the previous<br />

results, there is less variation in effective SINR (quicker transition from 0 to 1) as<br />

expected. For the MFB, power control ensures that the effective SINR is the same<br />

for each fading realization (9 dB). However, because we used measured results, we<br />

see a slight variation. Similar to the previous results, the MMSE DFE provides<br />

more higher SINR values than MMSE LE. At low SINR, there is no crossover, as<br />

power control and the high target value ensure few decision errors.<br />

Sometimes certain receivers work well under certain fading conditions, whereas<br />

other receivers work well under other conditions. Such behavior can be identified<br />

using a scatter plot, plotting the effective SINR of one receiver against the effective<br />

SINR of the other receiver. Scatter plots can also be useful in determining behaviors<br />

under different fading scenarios.<br />

In Fig. 6.17, a scatter plot of MMSE DFE effective SINR vs. MMSE LE effective<br />

SINR is given. While the simulation was run for 2000 fading realizations, only the<br />

first 1000 realizations are used to generate the scatter plot (making the individual

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