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

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Chapter 6: Event Selection 166<br />

Entries<br />

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-1<br />

∫L<br />

dt = 331 nb<br />

Data 2010 (<br />

Z → µ µ<br />

bb<br />

cc<br />

W → µ ν<br />

Z → τ<br />

tt<br />

s=7<br />

TeV)<br />

0<br />

0 10 20 30 40 50<br />

MDT hits/track<br />

Figure 6.2: MDT hits per muon track for signal Monte Carlo, background Monte<br />

Carlo and data after event preselection. The total Monte Carlo event number has<br />

been normalized to <strong>the</strong> number <strong>of</strong> events <strong>in</strong> data.<br />

segment must have at least 3 hits on it, <strong>in</strong> pr<strong>in</strong>ciple <strong>the</strong>re should be no track with less<br />

than 6 hits. We see a very small number <strong>of</strong> tracks with 3-5 hits, which are most likely<br />

badly reconstructed tracks with two segments that share one or more MDT hits.<br />

A track can have more than 20 MDT hits ow<strong>in</strong>g to two reasons:<br />

• It traverses <strong>the</strong> overlap region between adjacent φ sectors. Such a track can<br />

have a maximum <strong>of</strong> 40 hits, assum<strong>in</strong>g that it does not have more than one hit<br />

<strong>in</strong> any MDT tube layer.<br />

• It traverses multiple tubes <strong>in</strong> <strong>the</strong> same tube layer. Because <strong>of</strong> <strong>the</strong> geometry <strong>of</strong><br />

<strong>the</strong> multilayers, <strong>the</strong>re should be very few such tracks <strong>in</strong> collision events.<br />

We see that a small number <strong>of</strong> tracks have more than 40 hits, which are tracks

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