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 98<br />
Inside-out track reconstruction<br />
Inside-out track<strong>in</strong>g starts with <strong>the</strong> silicon detectors, namely <strong>the</strong> Pixel and <strong>the</strong><br />
SCT (see Chapter 2). This technique takes advantage <strong>of</strong> <strong>the</strong> very high granularity<br />
<strong>of</strong> <strong>the</strong> silicon detectors, which is especially useful at high track multiplicities. In<br />
<strong>the</strong> first stage, <strong>the</strong> raw data from <strong>the</strong> silicon layers is converted <strong>in</strong>to clusters, and<br />
<strong>the</strong> TDC output from <strong>the</strong> TRT <strong>in</strong>to calibrated drift circles. The silicon clusters are<br />
transformed <strong>in</strong>to 3-dimensional space-po<strong>in</strong>ts. In <strong>the</strong> SCT, cluster <strong>in</strong>formation from<br />
opposite sides <strong>of</strong> a module is comb<strong>in</strong>ed to form a 3D space-po<strong>in</strong>t.Pixel clusters are<br />
obviously 3-dimensional.<br />
The second stage <strong>in</strong>volves track-f<strong>in</strong>d<strong>in</strong>g, <strong>in</strong> which <strong>the</strong> algorithm searches for prompt<br />
tracks com<strong>in</strong>g from <strong>the</strong> <strong>in</strong>teraction region. First, track seeds are formed by comb<strong>in</strong><strong>in</strong>g<br />
three space-po<strong>in</strong>ts, each space-po<strong>in</strong>t orig<strong>in</strong>at<strong>in</strong>g <strong>in</strong> a unique Pixel or SCT layer. Fig-<br />
ure 4.2 shows <strong>the</strong> number <strong>of</strong> track seeds per event <strong>in</strong> data and <strong>in</strong> Monte Carlo. The<br />
seeds are extended to <strong>the</strong> rema<strong>in</strong><strong>in</strong>g silicon layers to form track candidates, which<br />
are fitted us<strong>in</strong>g a comb<strong>in</strong>atorial Kalman fitter/smooth<strong>in</strong>g technique [90]. Outly<strong>in</strong>g<br />
clusters are removed based on <strong>the</strong>ir large contribution to <strong>the</strong> fit χ 2 .<br />
The third stage is termed ambiguity-resolv<strong>in</strong>g. Some track candidates share clus-<br />
ters, or are fakes result<strong>in</strong>g from random cluster comb<strong>in</strong>ations. In order to resolve<br />
cluster-to-track association ambiguities and reject fake tracks, each candidate track<br />
is scored, <strong>the</strong> score <strong>in</strong>dicat<strong>in</strong>g <strong>the</strong> likelihood that <strong>the</strong> track reproduces <strong>the</strong> path <strong>of</strong><br />
an actual charged particle 2 . The highest scor<strong>in</strong>g track candidates are refitted, shared<br />
2 Track scor<strong>in</strong>g takes <strong>in</strong>to account <strong>the</strong> number <strong>of</strong> silicon clusters associated with a track candidate,<br />
<strong>the</strong> number <strong>of</strong> shared clusters and <strong>the</strong> number <strong>of</strong> holes, i.e. , layers where a cluster is expected but<br />
none is found.