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

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Chapter 9: Discussion and Outlook 240<br />

Entries/2.5 GeV<br />

400<br />

350<br />

300<br />

250<br />

200<br />

150<br />

100<br />

50<br />

Data 2010 ( s = 7 TeV)<br />

Z → µ µ<br />

Fit<br />

ATLAS Prelim<strong>in</strong>ary<br />

-1<br />

L dt = 3.37 pb<br />

0<br />

60 70 80 90 100 110 120<br />

[GeV]<br />

∫<br />

mµ<br />

µ<br />

Figure 9.3: Unb<strong>in</strong>ned fit to <strong>the</strong> Z <strong>boson</strong> mass peak us<strong>in</strong>g a <strong>the</strong>oretical l<strong>in</strong>eshape<br />

function convolved with a Gaussian function. The Monte Carlo prediction, normalized<br />

to <strong>the</strong> total number <strong>of</strong> data events, is also shown.<br />

Carlo.<br />

Fit parameter Value from data [GeV] Value from MC [GeV]<br />

Mean 90.85 ± 0.14 91.30 ± 0.01<br />

Width 2.83 ± 0.17 1.52 ± 0.01<br />

Table 9.3: Mean and width <strong>of</strong> <strong>the</strong> Gaussian component <strong>of</strong> Z l<strong>in</strong>eshape fits. The fit is<br />

made on unb<strong>in</strong>ned data events from a 3.37 pb −1 dataset and on b<strong>in</strong>ned Monte Carlo.<br />

Figure 9.4 shows muon k<strong>in</strong>ematic distributions (pT , η and φ) for muons from <strong>the</strong><br />

decay <strong>of</strong> <strong>the</strong> Z <strong>boson</strong>s. Figure 9.5 shows <strong>the</strong> muon pT versus dimuon <strong>in</strong>variant mass<br />

at two different stages <strong>of</strong> <strong>the</strong> Z selection cuts: after <strong>the</strong> muon pT cut (left) and after<br />

<strong>the</strong> isolation cut (right) on <strong>the</strong> decay muons. As with <strong>the</strong> lower-statistics dataset,

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