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Subsections
Definition of the observable
We apply the algorithm in ref. [2] only to particles in a
central rapidity region
. We cluster until two jets are left and study
 |
(34) |
with
the sum of the transverse energies of the two
remaining jets.
The hard scale (Q) is taken to be the Born partonic center-of-mass energy.
Rapidity of the center of mass of the outgoing pair: 0.000
Cosine of the angle between outgoing jet and beam (in the partonic CM frame): 0.200
| Test |
result |
| check number of jets |
T |
| all legs positive |
T |
| globalness |
F |
Since this observable is non-global, the analysis has not been continued.
Since this observable is discontinuosly global, multiple emission effects have not been computed.
y3_DeltaRE_HH_cut.tar.gz
collects all files produced automatically by Caesar.
Next: Central y3 (kt algorithm,
Up: Observables in hadronic dijet
Previous: Directly global y3 (kt
Giulia Zanderighi
2005-05-27