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

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Chapter 6: Event Selection 165<br />

Figure 6.1: Background versus signal efficiency for three different cone sizes used to<br />

def<strong>in</strong>e <strong>the</strong> relative track isolation. Monte Carlo samples are used for both background<br />

and signal.<br />

6.1.1 Properties <strong>of</strong> <strong>the</strong> preselected sample<br />

In this <strong>section</strong>, we present some properties <strong>of</strong> <strong>the</strong> data events, Monte Carlo signal<br />

and Monte Carlo background events after <strong>the</strong> preselection criteria have been applied.<br />

The backgrounds we consider <strong>in</strong>clude t¯t, QCD (b ¯ b and c¯c), Z → ττ and W → µν.<br />

These channels will be discussed <strong>in</strong> some detail <strong>in</strong> Chapter 7.<br />

Hit distributions<br />

We show below <strong>the</strong> distribution <strong>of</strong> hits on muon tracks <strong>in</strong> <strong>the</strong> various subsystems<br />

<strong>of</strong> <strong>the</strong> muon spectrometer and <strong>the</strong> <strong>in</strong>ner detector. Figure 6.2 shows <strong>the</strong> number <strong>of</strong><br />

MDT hits per track. The distribution peaks at 20 hits, which is expected for tracks<br />

that traverse all layers <strong>of</strong> all three MDT stations (Section 2.2.4). However, we see a<br />

significant number <strong>of</strong> tracks with 12 hits, i.e. , tracks that go through two stations.<br />

S<strong>in</strong>ce at least 2 segments are required for a track to be reconstructed, and each

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