Resolving negative cross section of quarkonium hadroproduction using soft gluon factorization
arXiv:2304.04552 · doi:10.1103/PhysRevD.108.014003
Abstract
It was found that, using nonrelativistic QCD factorization, the predicted hadroproduction cross section at large can be negative. The negative cross sections originate from terms proportional to plus function in channels, which are remnants of the infrared subtraction in matching the short-distance coefficients. In this article, we find that the above terms can be factorized into the nonperturbative soft gluon distribution function in the soft gluon factorization (SGF) framework. Therefore, the problem can be naturally resolved in SGF. With an appropriate choice of nonperturbative parameters, the SGF can indeed give positive predictions for production rates within the whole region. The production of is also discussed, and there is no negative cross section problem.
15 pages, 8 figures
References in corpus (27)
- J/psi (psi') production at the Tevatron and LHC at O(α_s^4v^4) in nonrelativistic QCD
- Reconciling J/psi production at HERA, RHIC, Tevatron, and LHC with NRQCD factorization at next-to-leading order
- QCD corrections to J/psi and Upsilon production at hadron colliders
- Polarization for Prompt J/psi, psi(2s) production at the Tevatron and LHC
- QCD corrections to J/psi polarization of hadronproduction at Tevatron and LHC
- QCD radiative corrections to production at hadron colliders
- Hadroproduction of J/psi and Upsilon in association with a heavy-quark pair
- production at the LHC challenges nonrelativistic-QCD factorization
- Impact of hadroproduction data on charmonium production and polarization within NRQCD framework
- production at LHC and indications on the understanding of production
- QCD corrections to at B Factories
- Next-to-Leading-Order QCD Corrections to e^ + e^- -> J/ψ+gg at the B Factories
- QCD corrections to polarization of J/ψand Υat Fermilab Tevatron and CERN LHC
- Measurement of J/psi and psi(2S) prompt double-differential cross sections in pp collisions at sqrt(s) = 7 TeV
- Heavy Quarkonium Production at Collider Energies: Partonic Cross Section and Polarization
- Measurement of chi_c1 and chi_c2 production with sqrt(s) = 7 TeV pp collisions at ATLAS
- Factorized power expansion for high- heavy quarkonium production
- Measurement of the production cross-section of in collisions at TeV at ATLAS
- Quark fragmentation into spin-triplet -wave quarkonium
- Revisiting NLO QCD corrections to total inclusive J/psi and Upsilon photoproduction cross sections in lepton-proton collisions
- production associated with a pair at hadron colliders
- Matching next-to-leading-order and high-energy-resummed calculations of heavy-quarkonium-hadroproduction cross sections
- Analytical calculation for the gluon fragmentation into spin-triplet S-wave quarkonium
- NLO fragmentation functions for a quark into a spin-singlet quarkonium: Same flavor case
- Global analysis of inclusive hadroproduction at next-to-leading order in nonrelativistic-QCD factorization
- Next-to-leading-order QCD corrections to heavy quark fragmentation into quarkonia
- Color-octet contributions for inclusive production at B factories in soft gluon factorization