Line: 1 to 1 | ||||||||
---|---|---|---|---|---|---|---|---|
Exclusive Jet Study With Kt, AntiKt and Cambridge Aachen Jet Finders
| ||||||||
Line: 48 to 48 | ||||||||
| ||||||||
Changed: | ||||||||
< < | This process ends when all dij and diB are above the dcut value | |||||||
> > | This process ends when all dij and diB are above the dcut value. The dcut variable again varies when considering an inclusive or exclusive event. When looking at an exclusive n-jet event. dcut = Ptmin^(2) This maintains the jet algorithm ability to factorize the initial-state of the collinear singularities, which allows you to obtain a finite cross-section. When looking at an inclusive jet event. dcut = Et^(2) | |||||||
Signal and Background Comparisons (Bin Width 100 GeV^2)Signal and Background Comparisons Not Normalized | ||||||||
Line: 84 to 96 | ||||||||
AntiKt Jet Finder | ||||||||
Changed: | ||||||||
< < | The Anti-Kt Algorithm follows the same procedure as the Kt algorithm explained above. The difference between these two algorithms is the dij and diB definitions. | |||||||
> > | The Anti-Kt Algorithm follows the same procedure as the Kt algorithm explained above. The differences between these two algorithms are the definitions for dij and diB. | |||||||
dij = min(1/P^2ti,1/P^2tj) ΔR ^2ij / R |