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Measurement of the Z boson cross-section in - Harvard University ...

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Chapter 7: Background Estimation 217<br />

Measured bb fraction (%)<br />

10<br />

8<br />

6<br />

4<br />

2<br />

0<br />

0 2 4 6 8 10<br />

Input bb fraction (%)<br />

Figure 7.6: The measured QCD fraction as a function <strong>the</strong> <strong>in</strong>put fraction from 8<br />

ensemble tests. The slope <strong>of</strong> <strong>the</strong> first-degree polynomial fit gives <strong>the</strong> correction factor<br />

for <strong>the</strong> QCD fraction obta<strong>in</strong>ed from a template fit to data.<br />

<strong>section</strong>s <strong>of</strong> <strong>the</strong>se samples, and use it as a systematic on <strong>the</strong> Monte Carlo prediction<br />

<strong>of</strong> <strong>the</strong> QCD background.<br />

In 331 nb −1 <strong>of</strong> data, we predict 0.038±0.015(stat)±0.038(sys)±0.04(lum) events<br />

us<strong>in</strong>g simulated b ¯ b and c¯c samples.<br />

7.2 Electroweak backgrounds<br />

7.2.1 t¯t background<br />

t¯t decays can fake <strong>the</strong> signal <strong>in</strong> two ways. One W can decay <strong>in</strong>to a muon, which<br />

can comb<strong>in</strong>e with a muon <strong>in</strong> a jet to give a Z → µµ decay topology, or both W ’s<br />

can decay <strong>in</strong>to muons which, be<strong>in</strong>g high-pT and isolated, toge<strong>the</strong>r resemble <strong>the</strong> signal<br />

channel. In <strong>the</strong> former case, <strong>the</strong> muon from <strong>the</strong> jet will generally be non-isolated, and

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