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CERN-THESIS-2012-153 26/07/2012 - CERN Document Server

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event is also discarded. Events with noise bursts in the LAr calorimeter are removed. Events with exactly<br />

three leptons, two ID leptons and one exclusive TL, are selected. The three leptons have to be matched<br />

to the same good primary vertex, which suppresses events from pile-up and secondary interactions. The<br />

TL is required to have pT > 25 GeV, whereas the ID leptons are required to have pT > 20 GeV. At least<br />

two ID jets and E miss<br />

T<br />

> 20 Gev are required. At least one of the ID jets in the event must be b-tagged.<br />

The preselection is completed by requiring at least two leptons of the same flavor and opposite charge, to<br />

account for the Z-boson from the FCNC decay of one of the top quarks. For this requirement, the TL (of<br />

unknown flavor) it is assigned the flavor of the lepton with which it is paired. In 2.05 fb −1 there are a total<br />

of 28 events passing the preselection criteria and an expected background of <strong>26</strong>.5 ± 4.9. The details of the<br />

background evaluation are given in Chapter 6. Distributions of relevant variables obtained after these cuts<br />

are shown in Figure 5.9.<br />

Event Reconstruction<br />

To complete the event selection the mass of the two top quarks can be reconstructed from the corresponding<br />

decay particles, taking advantage of the energy-momentum conservation. Background events are expected to<br />

fit less well with the t¯t hypothesis, this provides an opportunity for furher signal and background separation.<br />

Given that the neutrino from the SM single lepton decay of the top quark (t → Wb → bℓν) goes undetected,<br />

its four-momentum needs to be evaluated. This can be done by assuming the E miss<br />

T<br />

to be the neutrino<br />

transverse momentum, p ν T . The longitudinal component of the neutrino momentum (pν z) is then determined<br />

together with the choice for the jet and lepton combination by minimizing the following expression:<br />

χ 2 =<br />

<br />

mreco 2 − mt<br />

jaℓaℓb<br />

σ 2 t<br />

where mreco , mreco<br />

jaℓaℓb jbℓcν , mreco<br />

ℓcν<br />

+<br />

<br />

mreco 2 jbℓcν − mt<br />

σ 2 t<br />

+<br />

m reco<br />

ℓcν<br />

2 − mW<br />

σ 2 W<br />

+<br />

<br />

reco 2<br />

m − mZ ℓaℓb<br />

σ2 , (5.2)<br />

Z<br />

and mreco,<br />

are the reconstructed masses of the top quark candidate decaying<br />

ℓaℓb<br />

through the FCNC decay, the top quark candidate with SM decay, the W boson candidate from the top<br />

quark with SM decay and of the Z boson candidate from the top quark FCNC decay, respectively. There<br />

the masses are mt = 172.5 GeV, mW = 80.4 GeV, and mZ = 91.2 GeV, and the widths are σt = 14 GeV,<br />

σW = 10 GeV and σZ = 3 GeV. For each ID jet and lepton (the two ID leptons and the unique TL) com-<br />

bination, in which the Z-boson candidate is built from two leptons of the same flavor and opposite charges,<br />

the χ 2 minimization gives the value for p ν z. From all combinations, the one with the minimum χ 2 is chosen<br />

along with the corresponding p ν z value. Only the two leading ID jets are used in the reconstruction of the<br />

64

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