Search for charged Higgs bosons in decays of top quarks in p-pbar collisions at sqrt(s) = 1.96 TeV

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Particles with a superscript ( H + H^{+} ) include the opposite charged particle ( H − H^{-} ), and decay processes such as t → H + ​ b t\rightarrow H^{+}b imply also their charge conjugate processes

Cited in the paper.

The t ∗ t^{*} is a virtual top quark with an off-shell mass

Cited in the paper.

The positive and negative charged weak boson ( W ± W^{\pm} ) is presented as W W in this Letter

Cited in the paper.

In this Letter, the word lepton ( l l ) stands for an electron or a muon. The tau lepton is not referred to as a lepton, but is specified as τ \tau

Cited in the paper.

The detector uses cylindrical coordinates where θ \theta is the polar angle with respect to the proton beam and ϕ \phi is the azimuthal angle. The direction of a particle in the detector is expressed with the pseudorapidity, η = − ln ⁡ tan ⁡ ( θ / 2 ) \eta=-\ln\tan(\theta/2)

Cited in the paper.

Transverse energy is E T = E ​ sin ⁡ θ E_{T}=E\sin\theta , where E E is the measured energy. Transverse momentum, p T p_{T} , of charged particles, is calculated similarly. From energy-momentum conservation, ∑ i E T i ​ n i ^ = 0 \sum_{i}E^{i}_{T}\hat{n_{i}}=0 for radial unit vector n i ^ \hat{n_{i}} in the azimuthal plane. Missing transverse energy is defined as − ∑ i E i T n i ^ -\sum_{i}E^{i}_{T}\hat{n_{i}} , representing undetected particles such as neutrinos. The missing E T E_{T} is further corrected for the energy and momentum of identified muons

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