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PDF (double-sided) - Physics Department, UCSB - University of ...

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P | 11 〉 (a ′ b ′ )) estimated by sampling four multinomial distributions. As the<br />

number <strong>of</strong> samples increases, the statistical sampling noise goes down and<br />

√<br />

p(1−p)<br />

the estimates <strong>of</strong> the probabilities becomes better following σ p = .<br />

n<br />

• Since the experiment is subject to 1/f noise, the drift in the “true” value<br />

<strong>of</strong> S over the course <strong>of</strong> the experiment becomes worse and worse as the<br />

sampling time is increased.<br />

For small sample sizes, the standard error on S is therefore limited by statistical<br />

sampling noise, while for large sample sizes, the error will be limited by drift <strong>of</strong> S.<br />

Thus, there will exist a certain sample size n ∗ for which the two effects become<br />

equal and the error switches from being dominated by sampling noise to being<br />

dominated by experimental drifts. For sample sizes smaller than n ∗ , the above<br />

described simple-minded analysis approach is valid, while for sample sizes larger<br />

than n ∗ , this approach can severely underestimate the standard error σ S .<br />

To avoid having to model the statistical effects <strong>of</strong> 1/f noise on S, the data<br />

in this thesis will be presented as a collection <strong>of</strong> several measurements <strong>of</strong> S with<br />

individual estimates <strong>of</strong> σ S , each <strong>of</strong> which is based on data taken over short enough<br />

periods to guarantee sample sizes smaller than n ∗ .<br />

249

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