27.09.2014 Views

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

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

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

SHOW MORE
SHOW LESS

You also want an ePaper? Increase the reach of your titles

YUMPU automatically turns print PDFs into web optimized ePapers that Google loves.

11.2.3 Statistical Analysis<br />

For the final value <strong>of</strong> S to carry meaning, it needs to be supplemented with an<br />

estimate <strong>of</strong> its standard deviation σ S . To come up with a meaningfull estimate<br />

<strong>of</strong> this standard deviation turns out to be somewhat involved. A simple-minded<br />

approach is to break up an experiment consisting <strong>of</strong> N runs into n sections <strong>of</strong> N n<br />

runs each. For each section i, an S-value S i can be calculated and the resulting<br />

sample set can be statistically analyzed to obtain an estimator for the sample<br />

mean S, the sample standard deviation σ Si , and the resulting standard error <strong>of</strong><br />

the sample mean σ S :<br />

S = 1 n<br />

σ Si = √ 1<br />

n − 1<br />

n∑<br />

S i (11.1)<br />

i=1<br />

n∑ (<br />

Si − S ) 2<br />

i=1<br />

(11.2)<br />

σ S = σ S<br />

√ i<br />

(11.3)<br />

n<br />

The problem with this analysis is that it assumes the errors <strong>of</strong> S i to be uncorrelated,<br />

an assumption that does not hold in the presence <strong>of</strong> systematic errors in<br />

the experiment like drift and 1/f noise. This leads to different estimates <strong>of</strong> σ S<br />

for different choices for the number <strong>of</strong> sections n. In reality, the overall standard<br />

error in S as a function <strong>of</strong> sampling-time is the result <strong>of</strong> two competing effects:<br />

• S is calculated from a linear combination <strong>of</strong> 16 probabilities (P | 00 〉 (ab), . . . ,<br />

248

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!