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 101<br />
are computed for <strong>the</strong>se tracks, but no refitt<strong>in</strong>g is performed. The tracks are scored,<br />
resolved for ambiguities, and stored <strong>in</strong> a third track collection.<br />
Once all <strong>the</strong> track reconstruction sequences have run, <strong>the</strong> three separate track<br />
collections are merged. Ambiguity-resolv<strong>in</strong>g is performed once more to select unique<br />
tracks from <strong>the</strong> three collections, and <strong>the</strong> f<strong>in</strong>al tracks stored <strong>in</strong> one collection. At this<br />
po<strong>in</strong>t, post-process<strong>in</strong>g steps such as vertex f<strong>in</strong>d<strong>in</strong>g, photon conversion reconstruction<br />
and beam-spot f<strong>in</strong>d<strong>in</strong>g can be executed.<br />
Vertex reconstruction<br />
At <strong>the</strong> LHC design lum<strong>in</strong>osity <strong>of</strong> 10 34 cm −2 s −1 , each bunch <strong>cross</strong><strong>in</strong>g is expected<br />
to have > 20 events on average, <strong>of</strong> which <strong>in</strong> general only one will be <strong>in</strong>terest<strong>in</strong>g,<br />
<strong>the</strong> o<strong>the</strong>rs be<strong>in</strong>g mostly low-pT events 4 . Hence, <strong>the</strong>re will be a number <strong>of</strong> primary<br />
vertices <strong>in</strong> <strong>the</strong> <strong>in</strong>teraction region, as well as secondary vertices, vertices from photon<br />
conversions, long-lived neutral particles such as KS, and decay cha<strong>in</strong>s. The various<br />
vertex topologies are shown <strong>in</strong> Figure 4.3 [35].<br />
The correct reconstruction <strong>of</strong> vertices is important for many physics studies. Pri-<br />
mary vertices arise from promptly decay<strong>in</strong>g particles, while displaced vertices <strong>in</strong>dicate<br />
<strong>the</strong> decay <strong>of</strong> long-lived particles. Dist<strong>in</strong>guish<strong>in</strong>g between <strong>the</strong> different vertex types is<br />
crucial for discovery channels such as H → 4l, H → γγ, b-tagg<strong>in</strong>g, τ-jet identification,<br />
measurement <strong>of</strong> <strong>the</strong> lifetime <strong>of</strong> long-lived particles, and so on. ATLAS <strong>in</strong>ner detector<br />
reconstruction <strong>in</strong>cludes dedicated vertex f<strong>in</strong>ders for <strong>the</strong> different vertex types, <strong>in</strong>clud-<br />
<strong>in</strong>g full decay cha<strong>in</strong>s. The various reconstruction techniques will be discussed <strong>in</strong> some<br />
4 As <strong>of</strong> <strong>the</strong> writ<strong>in</strong>g <strong>of</strong> this <strong>the</strong>sis, <strong>the</strong> maximum <strong>in</strong>stantaneous lum<strong>in</strong>osity reached is 2.07 × 10 32<br />
cm −2 s −1 , <strong>the</strong> peak number <strong>of</strong> <strong>in</strong>teractions per bunch <strong>cross</strong><strong>in</strong>g be<strong>in</strong>g 3.78.