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We present a measurement of the cross section for W-boson production in association with jets in pbar-p collisions at sqrt(s)=1.96 TeV.
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We use a cylindrical coordinate system along the proton direction in which θ \theta ( ϕ ) (\phi) is the polar (azimuthal) angle. We define η = − ln ( tan ( θ / 2 ) ) \eta=-\ln(\tan(\theta/2)) , p T = p sin θ p_{T}=p\sin\theta , E T = E sin θ E_{T}=E\sin\theta , E / T E\!\!\!/_{T} = − | ∑ 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 beamline to the i t h i^{th} calorimeter tower, and m T W = 2 E T e l e E / T ( 1 − cos Δ ϕ ( E T ele , E / T ) ) m_{T}^{W}=\sqrt{2E_{T}^{ele}E\!\!\!/_{T}(1-\rm{cos}\Delta\phi(E_{T}^{ele},E\!\!\!/_{T}))}
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