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Using data corresponding to 6.0/fb of ppbar collisions at sqrt(s) = 1.96 TeV collected by the CDF II detector, we present a cross section measurement of top-quark pair production with an additional radiated photon.
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The CDF coordinate system of r r , φ \varphi , and z z is cylindrical, with the z z -axis along the proton beam. The pseudorapidity is η = − ln ( tan ( θ / 2 ) ) \eta=-\ln(\tan(\theta/2)) . Transverse momentum and energy are defined as p T = p sin θ {p}_{T}=p\sin\theta and E T = E sin θ {E}_{T}=E\sin\theta , respectively. We use the convention that “momentum” refers to p c pc and “mass” to m c 2 mc^{2} . The coordinate y y points up and down, and x x completes the right-handed system
Cited in the paper.
The CMU consists of a central barrel of gas proportional wire chambers in the region | η | < 0.6 |\eta|<0.6 ; the CMP system consists of chambers after an additional meter of steel, also for | η | < 0.6 |\eta|<0.6 . The CMX chambers cover 0.6 < | η | < 1.0 0.6<|\eta|<1.0
Cited in the paper.
The fraction of electromagnetic energy allowed to leak into the hadron compartment E had / E em \rm E_{had}/E_{em} must be less than 0.055 + 0.00045 × E em ( GeV ) \rm 0.055\kern-1.79993pt+\kern-1.79993pt0.00045\times E_{em}(\rm GeV) for central electrons, less than 0.05 for electrons in the end-plug calorimeters, less than max[0.125, 0.055 + 0.00045 × E em ( GeV ) \rm 0.055\kern-1.79993pt+\kern-1.79993pt0.00045\times E_{em}(\rm GeV) ] for photons
Cited in the paper.
Missing E T \rm E_{T} ( E → T {\not\!\!\vec{E}_{T}} ) is defined by E → T = − ∑ i E T i n ^ i {\not\!\!\vec{E}_{T}}=-\sum_{i}E_{T}^{i}\hat{n}_{i} , where i i is the calorimeter tower number for | η | < |\eta|< 3.6, and n ^ i \hat{n}_{i} is a unit vector perpendicular to the beam axis and pointing at the i t h i^{th} tower. We correct E → T {\not\!\!\vec{E}_{T}} for jets and muons. We define the magnitude E T = | E → T | \mbox{${\not\!E}_{T}$}=|{\not\!\!\vec{E}_{T}}|
Cited in the paper.
R. Field and R. C. Group, arXiv, hep-ph/0510198v1
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