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We present a simple method for the extraction of corrections for bias in the measurement of the momentum of muons in hadron collider experiments.
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T. Sjostrand, S. Mrenna, and P. Skands, ÒPYTHIA 6.4 Physics and ManualÓ, J. High Energy Phys. 05
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S. Alioli, P. Nason, C. Oleari and E. Re, J. High Energy Phys. 0807 (2008) 060, arXiv:0805.4802
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The coordinates in the laboratory frame are ( θ \theta , ϕ \phi , z z ), where θ \theta is the polar angle relative to the direction of one of the proton beams(the + z +z axis), and ϕ \phi the azimuth. The pseudorapidity is η = − l n t a n ( θ / 2 ) \eta=-ln~tan(\theta/2) . For an μ + + μ − \mu^{+}+\mu^{-} pair p T = P s i n θ p_{T}=Psin\theta , E T = E s i n θ E_{T}=Esin\theta , the rapidity y = 1 2 l n E + p z E − p z y=\frac{1}{2}ln\frac{E+p_{z}}{E-p_{z}} , where P P and p z p_{z} are the magnitude and z component of the momentum, and E is the energy of the μ + + μ − \mu^{+}+\mu^{-} pair
Cited in the paper.
Serguei Chatrchyan et al. (CMS Collaboration ), Phys.Rev. D 85
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