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A search for high-mass resonances in the $e^+e^-$ final state is presented based on 2.5 fb$^{-1}$ of $\sqrt{s}=$1.96 TeV $p\bar{p}$ collision data from the CDF II detector at the Fermilab Tevatron.
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We use a cylindrical coordinate system where θ \theta is the polar angle with respect to the proton beam axis (positive z z direction) and ϕ \phi is the azimuthal angle. The pseudorapidity is η = − ln [ tan ( θ / 2 ) ] \eta=-\ln[\tan(\theta/2)] . We define transverse energy as E T = E sin θ E_{T}=E\sin\theta and transverse momentum as p T = p sin θ p_{T}=p\sin\theta , where E E is the energy measured in the calorimeter and p p is the magnitude of the momentum measured by the spectrometer
Cited in the paper.
Throughout this Letter the charge conjugate state is implied
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Missing transverse energy ( E T = | E → T | {\not\!\!E_{T}}=|{\not\!\!\vec{E}_{T}}| ) is defined as E → T = − ∑ i E i T n ^ i {\not\!\!\vec{E}_{T}}=-\sum_{i}E^{i}_{T}\hat{n}_{i} where n ^ i \hat{n}_{i} is a unit vector in the transverse plane that points from the beam-line to the i t h i^{th} calorimeter tower
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σ B \sigma_{B} is N B + σ N B 2 \sqrt{N_{B}+\sigma^{2}_{N_{B}}} , where N B N_{B} is the number of expected backgrounds and σ N B \sigma_{N_{B}} is the systematic uncertainty of the N B N_{B}
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