Measurement of the Z boson cross-section in - Harvard University ...
Measurement of the Z boson cross-section in - Harvard University ...
Measurement of the Z boson cross-section in - Harvard University ...
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Chapter 4: Data Collection and Event Reconstruction 135<br />
tracks have been formed, an attempt is <strong>the</strong>refore made to match <strong>the</strong>m with corre-<br />
spond<strong>in</strong>g <strong>in</strong>ner detector tracks. The Moore family algorithm that does <strong>the</strong> match<strong>in</strong>g<br />
is MuIDComb<strong>in</strong>ed; <strong>the</strong> correspond<strong>in</strong>g Muonboy family algorithm is Staco.<br />
Comb<strong>in</strong>ed reconstruction by MuIDComb<strong>in</strong>ed<br />
MuIDComb<strong>in</strong>ed starts with a spectrometer track and attempts to match it with<br />
an <strong>in</strong>ner detector track us<strong>in</strong>g a χ 2 quantity compris<strong>in</strong>g <strong>the</strong> five track parameters and<br />
<strong>the</strong>ir covariances from each system:<br />
χ 2 match =(TMS − TID) T (CMS + CID) −1 (TMS − TID) (4.6)<br />
where T is a vector <strong>of</strong> <strong>the</strong> five track parameters expressed at <strong>the</strong> perigee, C is <strong>the</strong><br />
covariance matrix, and ID and MS denote <strong>the</strong> <strong>in</strong>ner detector and <strong>the</strong> muon spec-<br />
trometer respectively. For matches with χ 2 probability greater than 0.001, a partial<br />
refit is performed start<strong>in</strong>g with <strong>the</strong> <strong>in</strong>ner detector track vector and add<strong>in</strong>g hits from<br />
<strong>the</strong> spectrometer track, tak<strong>in</strong>g <strong>in</strong>to account material effects and <strong>the</strong> magnetic field [7].<br />
If no matches are found, a comb<strong>in</strong>ed fit is attempted with a road about <strong>the</strong> spectrom-<br />
eter track, and all measurements from <strong>the</strong> <strong>in</strong>ner detector and spectrometer are used<br />
<strong>in</strong> a global χ 2 fit.<br />
Comb<strong>in</strong>ed reconstruction by Staco<br />
Staco (STAtistical COmb<strong>in</strong>ation) attempts to statistically merge <strong>the</strong> ID and MS<br />
tracks to obta<strong>in</strong> a comb<strong>in</strong>ed track vector:<br />
T=(CMS + CID) −1 (CMSTMS + CIDTID) (4.7)<br />
where <strong>the</strong> Cs and <strong>the</strong> Ts are def<strong>in</strong>ed as before. A comb<strong>in</strong>ation is accepted if it is below<br />
an upper limit on <strong>the</strong> χ 2 , as def<strong>in</strong>ed <strong>in</strong> Eq. 4.6 above. If more than one comb<strong>in</strong>ation<br />
satisfies this criterion, <strong>the</strong> one with <strong>the</strong> lowest χ 2 is kept. The correspond<strong>in</strong>g tracks