Production and polarization of prompt (S) in the improved color evaporation model using the -factorization approach
arXiv:1811.11570 · doi:10.1103/PhysRevD.99.034007
Abstract
We calculate the polarization of prompt (S) production in the improved color evaporation model at leading order employing the -factorization approach. We present the polarization parameter of prompt (S) as a function of transverse momentum in and collisions to compare with data in the helicity, Collins-Soper and Gottfried-Jackson frames. We also present calculations of the bottomonium production cross sections as a function of transverse momentum and rapidity. This is the first -dependent calculation of bottomonium production and polarization in the improved color evaporation model. We find agreement with both bottomonium cross sections and polarization measurements.
arXiv commentarXiv admin note: substantial text overlap with arXiv:1808.02909
References in corpus (27)
- Heavy-flavour and quarkonium production in the LHC era: from proton-proton to heavy-ion collisions
- Quarkonium Feed-Down and Sequential Suppression
- Polarization for Prompt J/psi, psi(2s) production at the Tevatron and LHC
- Measurement of the Inclusive Upsilon production cross section in pp collisions at sqrt(s)=7 TeV
- Towards the experimental clarification of quarkonium polarization
- Transverse momentum dependent gluon density from DIS precision data
- Measurement of the Y(1S), Y(2S), and Y(3S) polarizations in pp collisions at sqrt(s) = 7 TeV
- Quarkonium Production in an Improved Color Evaporation Model
- Measurement of Upsilon production in 7 TeV pp collisions at ATLAS
- Measurement of Upsilon production in pp collisions at \sqrt{s} = 7 TeV
- Charmonium Production at High Energy in the k_T-Factorization Approach
- Production of J/psi and Upsilon mesons in pp collisions at sqrt(s) = 8 TeV
- Complete next-to-leading-order study on the yield and polarization of Upsilon(1S,2S,3S) at the Tevatron and LHC
- Measurement of the Y(1S), Y(2S), and Y(3S) cross sections in pp collisions at sqrt(s) = 7 TeV
- Systematics of quarkonium production
- Comparison of the color-evaporation model and the NRQCD factorization approach in charmonium production
- and production at hadron colliders in nonrelativistic QCD
- Production and polarization of prompt in the improved color evaporation model using the -factorization approach
- Forward production of mesons in collisions at and 8TeV
- An Updated Study for Production and Polarization at the Tevatron and LHC
- Measurement of the mass and of the relative rate of and production
- Measurement of the Upsilon(1S) Production Cross-Section in pp Collisions at sqrt(s) = 7 TeV in ATLAS
- Measurement of the fraction of \Y1S originating from \chib1P decays in collisions at $\sqrt{s} = 7\tev$
- Measurement of the production cross section ratio sigma(chi[b2](1P)) / sigma(chi[b1](1P)) in pp collisions at sqrt(s) = 8 TeV
- Polarization of prompt and (1S) production in the color evaporation model
- Measurement of the polarizations in collisions at =7 and 8TeV
- Polarized Heavy Quarkonium Production in the Color Evaporation Model
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- Heavy Quarkonium in Extreme Conditions
- The ALICE experiment: a journey through QCD
- New Observables in Inclusive Production of Quarkonia
- The Present and Future of QCD
- Production and polarization of direct to in the improved color evaporation model in collinear factorization
- Limits on Intrinsic Charm Production from the SeaQuest Experiment
- Inclusive quarkonium production in pp collisions at TeV
- Energy Dependence of Intrinsic Charm Production: What is the Best Energy for Observation?
- Production of bottomonia states in proton+proton and heavy-ion collisions
- and (2S) polarization in proton-proton collisions at energies available at the CERN Large Hadron Collider using PYTHIA8
- Quarkonium production and suppression: Theory
- Experimental Review of the Quarkonium Physics at the LHC
- Charmonium pair production at the LHCb in the ICEM using the -factorization: DPS versus SPS
- Physics with charmonia at the SPD experiment