The effect on PDFs and due to changes in flavour scheme and higher twist contributions
arXiv:1402.3536 · doi:10.1140/epjc/s10052-014-2958-4
Abstract
I consider the effect on MSTW partons distribution functions (PDFs) due to changes in the choices of theoretical procedure used in the fit. I first consider using the 3-flavour fixed flavour number scheme instead of the standard general mass variable flavour number scheme used in the MSTW analysis. This results in the light quarks increasing at all relatively small values, the gluon distribution becoming smaller at high values of and larger at small , the preferred value of the coupling constant falling, particularly at NNLO, and the fit quality deteriorates. I also consider lowering the kinematic cut on for DIS data and simultaneously introducing higher twist terms which are fit to data. This results in much smaller effects on both PDFs and than the scheme change, except for quarks at very high . I show that the structure function one obtains from a fixed input set of PDFs using the fixed flavour scheme and variable flavour scheme differ significantly for at high , and that this is due to the fact that in the fixed flavour scheme there is a slow convergence of large logarithmic terms of the form relevant for this regime. I conclude that some of the most significant differences in PDF sets are largely due to the choice of flavour scheme used.
23 pages, 19 figures. Final version. Sioke slightly extended discussion
References in corpus (12)
- Parton distributions for the LHC
- The PDF4LHC Working Group Interim Recommendations
- Mellin Moments of the {)} Heavy Flavor Contributions to unpolarized Deep-Inelastic Scattering at and Anomalous Dimensions
- Heavy-quark mass dependence in global PDF analyses and 3- and 4-flavour parton distributions
- Second order QCD corrections to jet production at hadron colliders: the all-gluon contribution
- Two-Loop Massive Operator Matrix Elements and Unpolarized Heavy Flavor Production at Asymptotic Values Q^2 >> m^2
- Two--Loop Massive Operator Matrix Elements for Unpolarized Heavy Flavor Production to $O(ε)
- The Transition Matrix Element A_{gq}(N) of the Variable Flavor Number Scheme at O(α_s^3)
- Extended Parameterisations for MSTW PDFs and their effect on Lepton Charge Asymmetry from W Decays
- The Heavy Quark Corrections to Charged Current Deep-Inelastic Scattering at large Virtualities
- The Effect of LHC Jet Data on MSTW PDFs
- Including heavy flavour production in PDF fits
Cited by in corpus (22)
- PDF4LHC recommendations for LHC Run II
- Parton distributions in the LHC era: MMHT 2014 PDFs
- Parton distributions from LHC, HERA, Tevatron and fixed target data: MSHT20 PDFs
- The Structure of the Proton in the LHC Precision Era
- A Critical Appraisal and Evaluation of Modern PDFs
- The 3-Loop Pure Singlet Heavy Flavor Contributions to the Structure Function and the Anomalous Dimension
- Hadron structure in high-energy collisions
- Precision determination of the strong coupling constant within a global PDF analysis
- Matching the Nagy-Soper parton shower at next-to-leading order
- Charm and beauty quark masses in the MMHT2014 global PDF analysis
- The impact of the final HERA combined data on PDFs obtained from a global fit
- On the Consistent Use of Scale Variations in PDF Fits and Predictions
- An investigation of the and heavy quark mass dependence in the MSHT20 global PDF analysis
- Precision physics with inclusive QCD processes
- Phenomenology of diffractive DIS in the framework of fracture functions and determination of diffractive parton distribution functions
- Improved nonsinglet QCD analysis of the fixed-target DIS data
- Heavy-flavor PDF evolution and variable-flavor number scheme uncertainties in deep-inelastic scattering
- NNLO PDFs driven by top-quark data
- Higher Order Heavy Quark Corrections to Deep-Inelastic Scattering
- A determination of mc(mc) from HERA data using a matched heavy-flavor scheme
- 3-loop Massive Contributions to the DIS Operator Matrix Element
- Recent progress on the calculation of three-loop heavy flavor Wilson coefficients in deep-inelastic scattering