Next-to-Leading-Order QCD corrections to J/ψ(Υ)+γproduction at the LHC
arXiv:0811.0963 · doi:10.1016/j.physletb.2008.12.050
Abstract
In this work, we calculate the next-to-leading-order (NLO) QCD corrections to the process via the color-singlet mechanism at the LHC. The results show that the partial cross section (3GeV and 3) is enhanced by a factor of about 2.0, and the differential cross section can be enhanced by two orders of magnitude in the large transverse momentum region of . Furthermore, the polarization of changes from transverse polarization at leading-order to longitudinal polarization at NLO. For the inclusive hadroproduction, it is known that the color-octet contributions are one order of magnitude larger than the color-singlet contribution, and the polarization distribution is dominated by the color-octet behavior at NLO. In contrast, for production the color-singlet contribution is of the same order as the color-octet contribution, and the polarization distribution arises from both the color-singlet and color-octet. Therefore, measurements of production associated with a direct photon at the hadron collider could be an important supplement to testify the theoretical framework treating with the heavy quarkonium. In addition, an NLO QCD correction to production at the LHC is also presented in this paper.
13 pages, 6 figures, 1 table
References in corpus (9)
- QCD corrections to J/psi and Upsilon production at hadron colliders
- Upsilon production at the Tevatron and the LHC
- J/psi, psi' and Upsilon Production at Hadron Colliders: a review
- QCD corrections to J/psi polarization of hadronproduction at Tevatron and LHC
- QCD corrections to J/psi plus eta_c production in e+e- annihilation at sqrt{s}=10.6 GeV
- Double charm production e^+ e^- \to J/ψ+ c \bar{c} at B factories with next-to-leading order QCD corrections
- QCD corrections to polarization of J/ψand Υat Fermilab Tevatron and CERN LHC
- Factorization and NLO QCD correction in e^+ e^- \to J/ψ(ψ(2S))+ χ_{c0} at B Factories}
- QCD corrections to double J/ψproduction in e+e- annihilation at \sqrt{s}=10.6 GeV
Cited by in corpus (20)
- The automated computation of tree-level and next-to-leading order differential cross sections, and their matching to parton shower simulations
- Heavy quarkonium: progress, puzzles, and opportunities
- Search for direct production of charginos, neutralinos and sleptons in final states with two leptons and missing transverse momentum in pp collisions at sqrt(s) = 8 TeV with the ATLAS detector
- Search for squarks and gluinos with the ATLAS detector in final states with jets and missing transverse momentum using TeV proton--proton collision data
- Complete off-shell effects in top quark pair hadroproduction with leptonic decay at next-to-leading order
- Search for squarks and gluinos in events with isolated leptons, jets and missing transverse momentum at TeV with the ATLAS detector
- Next-to-Leading-Order QCD Corrections to e^ + e^- -> J/ψ+gg at the B Factories
- Numerical NLO QCD calculations
- Quarkonium Physics at a Fixed-Target Experiment using the LHC Beams
- Next-to-Leading-Order QCD Corrections to e+ e- --> J/psi c c_bar at the B Factories
- Real next-to-next-to-leading-order QCD corrections to J/psi and Upsilon hadroproduction in association with a photon
- QCD corrections to Upsilon production via color-octet states at the Tevatron and LHC
- J/ψpolarization in photo-production up-to the next-to-leading order of QCD
- Associated production of a quarkonium and a Z boson at one loop in a quark-hadron-duality approach
- QCD corrections to production in association with a -boson at the LHC
- Spin physics and TMD studies at A Fixed-Target ExpeRiment at the LHC (AFTER@LHC)
- production associated with a pair at hadron colliders
- QED contribution to the production of J/ψ+c\bar{c}+X at the Tevatron and LHC
- Prompt heavy quarkonium production in association with a massive (anti)bottom quark at the LHC
- Next-to-leading order QCD corrections to Higgs boson decay to quarkonium plus a photon