Three-jet cross section in hadron collisions at next-to-leading order: pure gluon processes
arXiv:hep-ph/9610499 · doi:10.1103/PhysRevLett.77.2182
Abstract
The next-to-leading order three-jet cross section in hadron collisions is calculated in the simplified case when the matrix elements of all QCD subprocesses are approximated by the pure gluon matrix element. The longitudinally-invariant jet-clustering algorithm is used. The important property of reduced renormalization and factorization scale dependence of the next-to-leading order physical cross section as compared to the Born cross section is demonstrated.
10 pages, RevTeX + epsf.sty
Cited by in corpus (12)
- A parton shower algorithm based on Catani-Seymour dipole factorisation
- Next-to-leading order calculation of three-jet observables in hadron-hadron collision
- Three-jet cross sections in hadron-hadron collisions at next-to-leading order
- Two-Loop Four-Gluon Amplitudes in N=4 Super-Yang-Mills
- Two-loop QCD corrections to gluon-gluon scattering
- Second order QCD corrections to jet production at hadron colliders: the all-gluon contribution
- Two-loop QCD corrections to massless quark-gluon scattering
- Regularization Scheme Independence and Unitarity in QCD Cross Sections
- Calculation of QCD jet cross sections at next-to-leading order
- NLO QCD corrections to multi-jet production at the LHC with a centre-of-mass energy of sqrt(s)=8 TeV
- Next-to-Leading Order Gluonic Three Jet Production at Hadron Colliders
- Jet Cross-Section Measurements In CMS