Search for a New Heavy Gauge Boson Wprime with Electron + missing ET Event Signature in ppbar collisions at sqrt(s)=1.96 TeV

J. C. Pati and A. Salam, Phys. Rev. D 10

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We omit charge, anti-particle, and flavor-tagging neutrino symbols when representing the decay modes but assume proper charge conjugation throughout this report. For example, W ′ ⁣ + → e + ​ ν e W^{\prime+}\to e^{+}\nu_{e} and its charge conjugate are denoted as W ′ → e ​ ν W^{\prime}\to e\nu

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Missing transverse energy, E / T \mathbin{E\mkern-11.0mu/_{T}} , is defined as the magnitude of − ∑ i E T i n ^ i -\sum_{i}E_{T}^{i}\hat{n}_{i} , where n ^ i \hat{n}_{i} is a unit vector in the azimuthal plane that points from the beam line to the center of the i i th calorimeter tower

Cited in the paper.

We use a coordinate system where θ \theta is the polar angle to the proton beam, ϕ \phi is the azimuthal angle about the beam axis, and η \eta is the pseudorapidity defined as − ln ⁡ ( tan ⁡ ( θ / 2 ) ) -\ln(\tan(\theta/2)) . Energy (track momentum) measured transverse to the beam line is denoted as E T E_{T} ( p T p_{T} )

Cited in the paper.

The additional energy ( ≡ E T 0.4 − E T e ​ l ​ e \equiv E_{T}^{0.4}-E_{T}^{ele} ) must be less then 3 + 0.02 × E T e ​ l ​ e 3+0.02\times E_{T}^{ele} , where E T 0.4 E_{T}^{0.4} is the transverse energy in the cone of Δ ​ R ( ≡ ( Δ ​ ϕ ) 2 + ( Δ ​ η ) 2 ) < 0.4 \Delta R(\equiv\sqrt{(\Delta\phi)^{2}+(\Delta\eta)^{2}})<0.4 centered on the electron track and E T e ​ l ​ e E_{T}^{ele} is the transverse energy of the electron candidate. Both energies are in units of GeV

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