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

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Bell inequality. To make this claim, the number needs to be supplemented with an<br />

estimate <strong>of</strong> its standard error as described in Section 11.2.3. Since the experiment<br />

was run over roughly 8 hours to collect around 34.1 million statistical samples<br />

for each <strong>of</strong> the involved probabilities, the standard error is most likely dominated<br />

by 1/f noise and drifts in the experiment. Thus, one would need to model these<br />

error mechanisms in order to obtain a meaningful estimate for the standard error.<br />

This can be avoided by breaking the dataset into sections for which the standard<br />

error is known to be dominated by statistical sampling noise.<br />

11.5 Analysis and Verification<br />

11.5.1 Standard Error <strong>of</strong> the S-Value<br />

To find the right section size, the dataset is tentatively split into n sections.<br />

Each section is then divided into two halves that each yield an S-value S i,1 and<br />

S i,2 . The difference between these can be used as a drift-sensitive estimate <strong>of</strong> the<br />

internal variance for each section:<br />

v i = (S i,2 − S i,1 ) 2 (11.5)<br />

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