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A precision measurement of the top quark mass m_t is obtained using a sample of ttbar events from ppbar collisions at the Fermilab Tevatron with the CDF II detector.
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A particle’s transverse momentum p T p_{T} and tranverse energy E T E_{T} are given by | p → | sin θ |\vec{p}|\sin\theta and E sin θ E\sin\theta respectively, where θ \theta is the polar angle with respect to the proton direction (z-axis). The pseudorapidity η \eta of a particle’s three-momentum is defined by η = − ln ( tan ( θ / 2 ) ) \eta=-\ln(\tan(\theta/2)) . The missing E T E_{T} , E̸ T {\not}{E_{T}} , is defined by E̸ T → = − | ∑ i E T i n ^ T i | \vec{{\not}{E_{T}}}=-|\sum_{i}{E_{T_{i}}{\hat{n}_{T_{i}}}}| , where n ^ T i \hat{n}_{T_{i}} is the unit vector in the x x – y y plane pointing from the primary vertex to a given calorimeter tower i \it{i} , and E T i E_{T_{i}} is the E T E_{T} measured in that tower
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2010
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