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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.

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