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 138<br />
TileMuId was orig<strong>in</strong>ally designed to run as a Level-2 trigger algorithm, but has<br />
been adapted to run <strong>of</strong>fl<strong>in</strong>e [48]. As its name implies, it searches for muon-like en-<br />
ergy deposit signatures <strong>in</strong> <strong>the</strong> Tile hadronic calorimeter. It starts by look<strong>in</strong>g at <strong>the</strong><br />
outermost radial layer <strong>of</strong> <strong>the</strong> TileCal. If it f<strong>in</strong>ds an energy deposit compatible with<br />
<strong>the</strong> passage <strong>of</strong> a m<strong>in</strong>imum ioniz<strong>in</strong>g particle (MIP), it cont<strong>in</strong>ues <strong>the</strong> search <strong>in</strong> <strong>the</strong> mid-<br />
dle layer along a direction po<strong>in</strong>t<strong>in</strong>g to <strong>the</strong> <strong>in</strong>teraction region. If this search yields<br />
MIP-like energy deposit, it moves to <strong>the</strong> <strong>in</strong>ner layer. A MIP-like energy deposit <strong>in</strong><br />
this segment confirms a muon, <strong>the</strong> direction <strong>of</strong> which is estimated us<strong>in</strong>g <strong>the</strong> average<br />
coord<strong>in</strong>ates <strong>of</strong> <strong>the</strong> cells <strong>in</strong> <strong>the</strong> three layers.<br />
CaloTrkMuId<br />
CaloTrkMuId provides two algorithms: one which returns a likelihood value, and<br />
<strong>the</strong> o<strong>the</strong>r a tag. The former uses a likelihood ratio function <strong>in</strong>corporat<strong>in</strong>g longitud<strong>in</strong>al<br />
energy deposits <strong>in</strong> all layers <strong>of</strong> <strong>the</strong> EM and hadronic calorimeters. The tagg<strong>in</strong>g<br />
algorithm starts with an <strong>in</strong>ner detector track, propagates it through <strong>the</strong> calorimetry,<br />
and computes <strong>the</strong> energy deposit <strong>in</strong> a cone around <strong>the</strong> track. If <strong>the</strong> energy deposit is<br />
consistent with a MIP, <strong>the</strong> track is tagged as a muon.<br />
4.2.4 Efficiencies <strong>in</strong> <strong>the</strong> muon system<br />
S<strong>in</strong>ce we are <strong>in</strong>terested <strong>in</strong> muons <strong>in</strong> <strong>the</strong> f<strong>in</strong>al state for our analysis, it behooves<br />
us to study <strong>the</strong> hardware and s<strong>of</strong>tware efficiencies associated with <strong>the</strong> muon system.<br />
The most important hardware efficiencies are drift tube efficiency for detect<strong>in</strong>g hits<br />
from s<strong>in</strong>gle muons and trigger chamber efficiency for trigger<strong>in</strong>g on muons pass<strong>in</strong>g <strong>the</strong><br />
preset thresholds. Crucial s<strong>of</strong>tware efficiencies <strong>in</strong>clude reconstruction efficiency for<br />
muon tracks and efficiencies <strong>of</strong> <strong>the</strong> Level-2 and Level-3 trigger algorithms. In this