B. Abbott et al
2000
Cited alongside, same era.
T. Sjostrand et al
2001
Cited alongside, same era.
G. Corcella et al
2001
Cited alongside, same era.
B. L. Winer, Int. J. Mod. Phys. A 16S1C
2001
Cited alongside, same era.
J. Pumplin et al
2002
Cited alongside, same era.
R. Field, in Proceedings of the TeV4LHC Workshop, 2005. (Report No. FERMILAB-CONF-06-408-E, FNAL)
2005
Cited alongside, same era.
D. Acosta et al
2005
Cited alongside, same era.
R. Field and R. Group, arXiv: hep-ph/0510198
Cited in the paper.
The transverse momentum, p T p_{T} , is defined as the momentum transverse to the beam axis; The transverse energy E T E_{T} , is defined as the energy multiplied by the sine of the angle with respect to the beam axis; The pseudorapidity is defined as η = − ln ( tan ( θ / 2 ) ) \eta=-\ln{(\tan(\theta/2))} , where the polar angle θ \theta is taken with respect to the proton beam direction. The rapidity is defined as y = 1 2 ln ( E + p z E − p z ) y=\frac{1}{2}\ln{(\frac{E+p_{z}}{E-p_{z}})} where E E denotes the energy and p z p_{z} is the component of the momentum along the beam direction. ϕ \phi is measured in the plane orthogonal to the beam direction
Cited in the paper.
S. Vallecorsa, Proceedings of DIS2007, (to be published)
Cited in the paper.
G. C. Blazey et al
Cited in the paper.
In order to reduce online trigger rates, different prescale factors are applied to trigger paths. For a given trigger path, a prescale of 1000 would indicate that only one in every 1000 events satisfying the trigger requirements is selected
Cited in the paper.