Hadroproduction of electroweak gauge boson plus jets and TMD parton density functions
arXiv:1406.2994 · doi:10.1016/j.physletb.2014.07.035
Abstract
If studies of electroweak gauge boson final states at the Large Hadron Collider, for Standard Model physics and beyond, are sensitive to effects of the initial state's transverse momentum distribution, appropriate generalizations of QCD shower evolution are required. We propose a method to do this based on QCD transverse momentum dependent (TMD) factorization at high energy. The method incorporates experimental information from the high-precision deep inelastic scattering (DIS) measurements, and includes experimental and theoretical uncertainties on TMD parton density functions. We illustrate the approach presenting results for production of W-boson + n jets at the LHC, including azimuthal correlations and subleading jet distributions.
9 pages, 4 figures. v2: comments and references added, typos corrected; results unchanged
References in corpus (6)
- The CCFM Monte Carlo generator CASCADE 2.2.0
- Forward Jet Production at the Large Hadron Collider
- Endpoint singularities in unintegrated parton distributions
- High Energy Resummation of Drell-Yan Processes
- Angular correlations in multi-jet final states from kt-dependent parton showers
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Cited by in corpus (12)
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- Associated production of bosons and -jets at the LHC in the combined + collinear QCD factorization approach
- Azimuthal correlations of high transverse momentum jets at next-to-leading order in the parton branching method
- Charm quark and meson production in association with single-jet at the LHC
- Numerical evaluation of multi-gluon amplitudes for High Energy Factorization
- TMD parton showers for associated +jet production in electron-proton collisions at high energies
- On relation between Parton Branching Approach and CCFM evolution
- Associated Higgs + jet(s) production at the LHC and CCFM gluon dynamics in a proton
- TMD parton densities in associated real and virtual photon and jet production at LHC
- Dijet photoproduction at low at next-to-leading order and its back-to-back limit