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We measure the polarization of W bosons from top-quark (t) decays into final states with a charged lepton and jets, tt --> WbWb --> lvbqqb, using the full Run II data set collected by the CDF II detector.
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Charge-conjugate modes are included implicitly throughout this paper
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We use a cylindrical coordinate system where the z z axis is along the proton beam direction, ϕ \phi is the azimuthal angle, and θ \theta is the polar angle. Pseudorapidity is η = − ln tan ( θ / 2 ) \eta=-\ln\tan(\theta/2) , while transverse momentum is p T = | p | sin θ p_{T}=|p|\sin\theta , and transverse energy is E T = E sin θ E_{T}=E\sin\theta . Missing transverse energy, E T {\not\!\!E_{T}}
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2012
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