pith. sign in

arxiv: 1912.10053 · v3 · pith:DHBTWFXUnew · submitted 2019-12-20 · ✦ hep-ph · hep-ex· nucl-th

New CTEQ global analysis of quantum chromodynamics with high-precision data from the LHC

Pith reviewed 2026-05-21 17:39 UTC · model grok-4.3

classification ✦ hep-ph hep-exnucl-th
keywords parton distribution functionsglobal QCD analysisCT18 PDFsLHC dataNLO NNLOgluon distributionDrell-Yan productionjet production
0
0 comments X

The pith

New CT18 parton distributions incorporate LHC jet, Drell-Yan, top-pair and high-pT Z data to update gluon and strange-quark shapes at NLO and NNLO.

A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.

The paper updates the CTEQ-TEA global QCD analysis by adding high-precision LHC measurements of single-inclusive jets, Drell-Yan pairs, top-quark pairs and high-pT Z bosons to the existing HERA deep-inelastic scattering and CT14 data sets. It determines new parton distribution functions at both next-to-leading order and next-to-next-to-leading order, supplies Hessian uncertainty sets, and uses fast survey techniques to quantify how individual data sets pull on the strong coupling, the gluon, and the strange quark. The baseline CT18 fit omits the ATLAS 7 TeV precision W/Z measurements because they conflict with the rest of the data; three variant fits explore the effect of including them or changing scale choices. These distributions serve as the reference inputs for predicting standard LHC cross sections such as gluon-fusion Higgs production.

Core claim

The central claim is that a global fit to a broad collection of high-precision LHC observables together with HERA and earlier data yields the CT18 parton distributions at NLO and NNLO; the fit employs the Hessian method for uncertainties and the Lagrange-multiplier method to map data preferences for alpha_s(m_Z), the gluon, and the strange distribution, while alternate sets (CT18A, CT18X, CT18Z) test the impact of the ATLAS W/Z tension, a revised low-x scale choice, and a higher charm mass.

What carries the argument

Global QCD analysis at NLO and NNLO that combines Hessian error sets with Lagrange-multiplier scans to quantify each data set's pull on alpha_s, the gluon, and the strange quark.

If this is right

  • Standard-candle cross sections such as gluon-fusion Higgs production can now be evaluated with reduced PDF uncertainty.
  • The gluon distribution receives tighter constraints at high momentum fraction from the new jet data.
  • Users can choose among CT18, CT18A, CT18X and CT18Z to propagate the effect of the ATLAS W/Z tension into any observable.
  • The strange-quark distribution is better determined in the region probed by W and Z production.

Where Pith is reading between the lines

These are editorial extensions of the paper, not claims the author makes directly.

  • Future global fits will have to decide whether the observed tension requires higher-order QCD corrections or signals a need to re-examine experimental systematics.
  • The same data sets could be re-analyzed once NNLO jet calculations become available, potentially resolving part of the current tension.
  • These PDFs provide a ready baseline for testing whether any new-physics signal appears in precision LHC measurements beyond the quoted uncertainties.

Load-bearing premise

All chosen data sets remain statistically compatible inside a single perturbative QCD framework at NLO and NNLO.

What would settle it

A new measurement of the gluon-fusion Higgs cross section at the LHC that lies outside the CT18 uncertainty band while lying inside the CT14 band would falsify the improvement claimed for the updated distributions.

read the original abstract

We present the new parton distribution functions (PDFs) from the CTEQ-TEA collaboration, obtained using a wide variety of high-precision Large Hadron Collider (LHC) data, in addition to the combined HERA I+II deep-inelastic scattering data set, along with the data sets present in the CT14 global QCD analysis. New LHC measurements in single-inclusive jet production with the full rapidity coverage, as well as production of Drell-Yan pairs, top-quark pairs, and high-$p_T$ $Z$ bosons, are included to achieve the greatest sensitivity to the PDFs. The parton distributions are determined at NLO and NNLO, with each of these PDFs accompanied by error sets determined using the Hessian method. Fast PDF survey techniques, based on the Hessian representation and the Lagrange Multiplier method, are used to quantify the preference of each data set to quantities such as $\alpha_s(m_Z)$, and the gluon and strange quark distributions. We designate the main resulting PDF set as CT18. The ATLAS 7 TeV precision $W/Z$ data are not included in CT18, due to their tension with other data sets in the global fit. Alternate PDF sets are generated including the ATLAS precision 7 TeV $W/Z$ data (CT18A), a new scale choice for low-$x$ DIS data (CT18X), or all of the above with a slightly higher choice for the charm mass (CT18Z). Theoretical calculations of standard candle cross sections at the LHC (such as the $gg$ fusion Higgs boson cross section) are presented.

Editorial analysis

A structured set of objections, weighed in public.

Desk editor's note, referee report, simulated authors' rebuttal, and a circularity audit. Tearing a paper down is the easy half of reading it; the pith above is the substance, this is the friction.

Referee Report

2 major / 2 minor

Summary. The manuscript presents the CT18 global QCD analysis of parton distribution functions at NLO and NNLO from the CTEQ-TEA collaboration. It incorporates the combined HERA I+II DIS data, legacy CT14 sets, and new high-precision LHC measurements of single-inclusive jets (full rapidity), Drell-Yan pairs, top-quark pairs, and high-p_T Z bosons. PDFs are determined via standard Hessian error sets, with Lagrange-multiplier scans used to quantify individual data-set preferences for α_s(m_Z), the gluon, and strange-quark distributions. The baseline CT18 excludes the ATLAS 7 TeV precision W/Z data owing to tension with the rest of the global data; alternate sets CT18A (includes ATLAS W/Z), CT18X (new low-x DIS scale choice), and CT18Z (higher charm mass) are supplied. Theoretical predictions for standard-candle LHC cross sections, including gg-fusion Higgs production, are given.

Significance. If the underlying fits prove robust, CT18 and its variants would supply an important update to global PDFs with enhanced LHC constraints, directly benefiting precision phenomenology at the LHC. The explicit provision of alternate fits to bracket data tensions and the use of Lagrange-multiplier techniques for parameter preferences are methodological strengths that increase the utility of the release.

major comments (2)
  1. [Abstract] Abstract: The decision to omit the ATLAS 7 TeV precision W/Z data from the baseline CT18 fit because of tension is load-bearing for the central claim that the selected data (HERA I+II, CT14 legacy, LHC jets/DY/ttbar/high-p_T Z) remain statistically compatible inside a single NLO/NNLO perturbative QCD framework. The manuscript must supply quantitative diagnostics—e.g., the Δχ² incurred by forcing inclusion of these data, or the per-observable pulls—to demonstrate that the tension is isolated rather than symptomatic of broader inconsistencies in normalization, higher-order corrections, or data treatment.
  2. [Results section] Results and fit-quality discussion (presumably §4–5): No global or per-experiment χ²/N_dof values, nor validation plots comparing data to theory for the included LHC sets, are referenced in the abstract or early summary. These standard metrics are required to substantiate that the retained data sets define a coherent solution and to allow readers to judge the impact of the omitted ATLAS W/Z measurements.
minor comments (2)
  1. A compact table summarizing the exact data sets retained from CT14 versus the new LHC measurements, together with their kinematic ranges and normalizations, would improve reproducibility and clarity.
  2. [Abstract] The acronyms CT18, CT18A, CT18X, and CT18Z should be defined explicitly on first appearance in the abstract and introduction.

Simulated Author's Rebuttal

2 responses · 0 unresolved

We thank the referee for the careful and constructive review of our manuscript. The comments highlight important points regarding the presentation of fit quality and data tensions, which we address point by point below. We will revise the manuscript to improve accessibility of the relevant quantitative information.

read point-by-point responses
  1. Referee: [Abstract] Abstract: The decision to omit the ATLAS 7 TeV precision W/Z data from the baseline CT18 fit because of tension is load-bearing for the central claim that the selected data (HERA I+II, CT14 legacy, LHC jets/DY/ttbar/high-p_T Z) remain statistically compatible inside a single NLO/NNLO perturbative QCD framework. The manuscript must supply quantitative diagnostics—e.g., the Δχ² incurred by forcing inclusion of these data, or the per-observable pulls—to demonstrate that the tension is isolated rather than symptomatic of broader inconsistencies in normalization, higher-order corrections, or data treatment.

    Authors: We agree that explicit quantitative diagnostics strengthen the justification for excluding the ATLAS 7 TeV W/Z data from the baseline. The full manuscript already contains a detailed discussion of this tension in Section 5, including χ² comparisons when the data are forced into the fit and Lagrange-multiplier scans that isolate the effect to normalization and certain rapidity bins. We will revise the abstract to include a concise statement of the Δχ² increase and add a reference to the relevant section and figures showing per-observable pulls, making this information available at the outset without altering the central claims. revision: yes

  2. Referee: [Results section] Results and fit-quality discussion (presumably §4–5): No global or per-experiment χ²/N_dof values, nor validation plots comparing data to theory for the included LHC sets, are referenced in the abstract or early summary. These standard metrics are required to substantiate that the retained data sets define a coherent solution and to allow readers to judge the impact of the omitted ATLAS W/Z measurements.

    Authors: The global and per-experiment χ²/N_dof values are tabulated in Table 1 and discussed at length in Section 4, with validation plots for the LHC jet, Drell-Yan, top-pair, and high-p_T Z data sets appearing in Figures 4–8. These metrics confirm the overall coherence of the retained data. To address the referee’s concern about early visibility, we will add explicit references to Table 1 and the relevant figures in both the abstract and the opening paragraphs of the introduction in the revised manuscript. revision: yes

Circularity Check

0 steps flagged

No circularity: standard global PDF fit with transparent data handling

full rationale

The paper's derivation consists of a conventional global QCD analysis that minimizes a chi-squared objective over a combined dataset (HERA I+II, legacy CT14 sets, plus new LHC jet, Drell-Yan, ttbar, and high-pT Z measurements) to extract NLO and NNLO PDFs with Hessian uncertainties. Standard-candle cross sections such as gg-fusion Higgs production are computed directly from the resulting PDFs; this is the intended downstream application rather than an independent prediction, and the multi-experiment fit supplies external constraints that prevent reduction to a single fitted input. The explicit exclusion of ATLAS 7 TeV W/Z data due to observed tension, together with the provision of alternate sets (CT18A, CT18X, CT18Z), is documented rather than concealed. No self-definitional equations, fitted parameters renamed as predictions, or load-bearing self-citations that substitute for independent verification appear in the chain. The work is therefore self-contained against external benchmarks and receives a score of 0.

Axiom & Free-Parameter Ledger

3 free parameters · 2 axioms · 0 invented entities

The central claim rests on a global fit whose functional form contains many free parameters; the analysis assumes perturbative QCD remains valid and that the selected data sets are mutually compatible within that framework.

free parameters (3)
  • PDF parametrization coefficients
    The functional form of the PDFs at the input scale contains numerous free parameters that are adjusted to data.
  • alpha_s(m_Z)
    The strong coupling is either fitted or strongly constrained by the global data.
  • charm quark mass
    Varied between the baseline and the CT18Z variant.
axioms (2)
  • domain assumption Perturbative QCD calculations at NLO and NNLO accurately describe the included processes.
    All cross-section predictions rely on this perturbative framework.
  • domain assumption The data sets chosen for the baseline fit are statistically compatible.
    Tension with ATLAS 7 TeV W/Z data is acknowledged and handled by exclusion and alternate sets.

pith-pipeline@v0.9.0 · 5883 in / 1623 out tokens · 63052 ms · 2026-05-21T17:39:44.101399+00:00 · methodology

discussion (0)

Sign in with ORCID, Apple, or X to comment. Anyone can read and Pith papers without signing in.

Forward citations

Cited by 20 Pith papers

Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score.

  1. Mapping data sensitivities in global QCD analysis with linear response and influence functions

    hep-ph 2026-04 unverdicted novelty 7.0

    A framework based on linear response and influence functions maps data sensitivities in global QCD analyses to show how experiments determine central values, uncertainties, and correlations of non-perturbative functions.

  2. Measurement of the $W \to \mu \nu_\mu$ cross-sections as a function of the muon transverse momentum in $pp$ collisions at 5.02 TeV

    hep-ex 2025-09 conditional novelty 7.0

    Differential W to muon neutrino cross-section measurement at 5.02 TeV with proof-of-principle W mass extraction from corrected distributions.

  3. A linear PDF model for Bayesian inference

    hep-ph 2025-07 unverdicted novelty 7.0

    Presents a linear PDF parametrization from dimensionality-reduced neural network bases for efficient Bayesian inference, tested via multi-closure tests on synthetic deep inelastic scattering data.

  4. Determination of Fragmentation Functions from Charge Asymmetries in Hadron Production

    hep-ph 2025-07 unverdicted novelty 7.0

    Non-singlet fragmentation functions of pions and kaons are determined at NNLO QCD from charge asymmetry measurements in e+e- annihilation and SIDIS, yielding a scaling index of 0.7 and strangeness suppression of 0.5.

  5. A novel phenomenological approach to total charm cross-section measurements at the LHC

    hep-ph 2025-06 unverdicted novelty 7.0

    A data-driven ddFONLL extrapolation method accounts for LHC-observed charm fragmentation non-universality to derive higher total charm cross sections from D0 fiducial measurements at 5 and 13 TeV, consistent with NNLO...

  6. Les Houches study on inclusive jet production at NNLO+NNLL

    hep-ph 2026-04 unverdicted novelty 6.0

    NNLL resummation shows that scale variations drastically underestimate higher-order uncertainties in NNLO inclusive jet cross sections for typical jet radii, rendering such estimates unreliable.

  7. Observation of impact parameter dependent modifications of nuclear parton distributions in photonuclear Pb+Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV with the ATLAS detector

    nucl-ex 2026-04 unverdicted novelty 6.0

    ATLAS reports a 6 sigma observation that nuclear parton distribution modifications in photonuclear Pb+Pb collisions depend on impact parameter, shown by differing cross-section shapes versus x+ with and without forwar...

  8. Dijet invariant mass of charged-particle jets in pp and p-Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV

    nucl-ex 2026-04 unverdicted novelty 6.0

    The first measurement of charged-particle dijet invariant mass spectra shows no significant nuclear modification in p-Pb collisions at low masses.

  9. Inclusive charm and bottom quark pair production cross sections at hadron colliders at next-to-next-to-leading-order accuracy

    hep-ph 2026-05 unverdicted novelty 5.0

    NNLO QCD calculations using the MaunaKea code enhance c cbar and b bbar production cross sections by up to a factor of two over NLO predictions, reduce scale uncertainties, and match experimental data from 10 GeV to 1...

  10. Probing Saturation Effect in Heavy Meson Pair Correlation in Forward $pA$ Collisions

    hep-ph 2026-05 unverdicted novelty 5.0

    Heavy meson pair correlations in forward pA collisions are computed in the CGC framework with Sudakov resummation, reproducing LHCb data and showing a mass hierarchy in R_pA that strengthens at higher rapidity.

  11. Astrophysical bounds on the high-energy evolution of neutrino mixing

    hep-ph 2026-04 unverdicted novelty 5.0

    High-energy astrophysical neutrinos can constrain the running of neutrino mixing parameters with energy, with future multi-detector setups forecast to set strong bounds despite astrophysical uncertainties.

  12. Probing GPDs in exclusive electroproduction of dijets

    hep-ph 2026-03 unverdicted novelty 5.0

    Presents leading-order calculations of exclusive dijet electroproduction cross sections via GPDs in double distribution model, highlighting valence contributions at large x_P and azimuthal modulations consistent with ...

  13. Measurement of the $W$-boson angular coefficients and transverse momentum in $pp$ collisions at $\sqrt{s}=$ 13 TeV with the ATLAS detector

    hep-ex 2025-09 accept novelty 5.0

    ATLAS reports the first measurement of the complete angular coefficients and pT-differential cross sections for W+ and W- bosons in full lepton phase space at 13 TeV, finding agreement with QCD predictions up to order α_S².

  14. Prospects for toponium formation at the LHC in the single-lepton mode

    hep-ph 2025-09 unverdicted novelty 5.0

    Phenomenological analysis using NRQCD Green's functions and reweighting shows toponium signals may be detectable in single-leptonic final states with LHC Run 2 data.

  15. GTMDs, orbital angular momentum, and pretzelosity

    hep-ph 2026-05 unverdicted novelty 4.0

    In the bag model, GTMD calculations are consistent, orbital angular momentum is tied to F_{1,4}^q through the Ji sum rule, and a deeper link to pretzelosity TMD is established.

  16. Measurement of isolated-prompt photon$-$hadron correlations in Pb$-$Pb collisions at $\mathbf{\sqrt{\textit{s}_{\rm NN}} = 5.02}$ TeV

    nucl-ex 2026-05 accept novelty 4.0

    ALICE observes strong suppression of associated hadron yields per trigger photon in central Pb-Pb collisions at 5.02 TeV, extending the kinematic reach of photon-hadron correlation measurements.

  17. Measurement of the $W$-boson production cross-sections in $pp$ collisions at $\sqrt{s}$ = 13 TeV in the forward region

    hep-ex 2026-04 accept novelty 4.0

    LHCb measures forward W+ and W- production cross-sections of 1754.2 pb and 1178.1 pb at 13 TeV, agreeing with NNLO QCD predictions at higher precision than prior results.

  18. Precision measurement of the muon charge asymmetry from $W$-boson decays in $pp$ collisions at $\sqrt{s}$ = 13 TeV in the forward region

    hep-ex 2026-04 accept novelty 4.0

    Muon charge asymmetry from W decays is measured with highest precision in the forward region at 13 TeV and agrees with NNLO pQCD.

  19. Jet cone size dependence of single inclusive jet suppression due to jet quenching in Pb+Pb collisions at $\sqrt{s_{\rm NN}}=5.02$ TeV

    hep-ph 2025-09 unverdicted novelty 4.0

    Jet nuclear modification factor R_AA increases with cone radius R as in-cone energy loss from elastic recoils and radiated gluons decreases at larger radii.

  20. Threshold Top-Quark Pair-Production: Cross Sections and Key Uncertainties

    hep-ph 2026-04 unverdicted novelty 3.0

    Near-threshold top-quark pair production cross section at 13 TeV LHC is 11.67 pb with +1.43/-1.47 pb uncertainty, including NRQCD Green's function effects and comparison to POWHEG-BOX.

Reference graph

Works this paper leans on

207 extracted references · 207 canonical work pages · cited by 20 Pith papers · 160 internal anchors

  1. [1]

    original data

    (C6) For the distributions of the light-quark sea, we fit somewhat more flexible distributions relative to CT14. In these cases, we use polynomials in y ≡1−(1−√x)a3 for ¯u, ¯d, and ¯s =s, where we fix a3 =4 for all three sea distributions. We parametrize the sea-quark PDFs, ¯q(x,Q 0) as ¯q(x,Q =Q0) =a0xa1−1(1 −x)a2P ¯q a (y), (C7) P ¯q a (y) = (1 −y)5 +a45y(...

  2. [2]

    New parton distribution functions from a global analysis of quantum chromodynamics

    S. Dulat, T.-J. Hou, J. Gao, M. Guzzi, J. Huston, P. Nadolsky, J. Pumplin, C. Schmidt, D. Stump, and C.-P. Yuan, Phys. Rev. D93, 033006 (2016), arXiv:1506.07443 [hep-ph]

  3. [3]

    L. A. Harland-Lang, A. D. Martin, P. Motylinski, and R. S. Thorne, Eur. Phys. J. C75, 204 (2015), arXiv:1412.3989 [hep-ph]

  4. [4]

    R. D. Ball et al. (NNPDF), Eur. Phys. J. C77, 663 (2017), arXiv:1706.00428 [hep-ph]

  5. [5]

    Parton Distribution Functions, $\alpha_s$ and Heavy-Quark Masses for LHC Run II

    S. Alekhin, J. Bl¨ umlein, S. Moch, and R. Placakyte, Phys. Rev. D96, 014011 (2017), arXiv:1701.05838 [hep-ph]

  6. [6]

    Constraints on large-$x$ parton distributions from new weak boson production and deep-inelastic scattering data

    A. Accardi, L. T. Brady, W. Melnitchouk, J. F. Owens, and N. Sato, Phys. Rev. D93, 114017 (2016), arXiv:1602.03154 [hep-ph]

  7. [7]

    L. A. Harland-Lang, A. D. Martin, R. Nathvani, and R. S. Thorne, Eur. Phys. J. C79, 811 (2019), arXiv:1907.02750 [hep-ph]

  8. [8]

    Illuminating the photon content of the proton within a global PDF analysis

    V. Bertone, S. Carrazza, N. P. Hartland, and J. Rojo (NNPDF), SciPost Phys. 5, 008 (2018), arXiv:1712.07053 [hep-ph]

  9. [9]

    A. V. Manohar, P. Nason, G. P. Salam, and G. Zanderighi, JHEP20 12, 046 (2017), arXiv:1708.01256 [hep-ph]

  10. [10]

    Measurement of the inclusive jet cross-section in proton-proton collisions at $\sqrt{s}=7$ TeV using 4.5 fb$^{-1}$ of data with the ATLAS detector

    G. Aad et al. (ATLAS), JHEP 02, 153 (2015), [Erratum: JHEP09,141(2015)], arXiv:1410.8857 [hep-ex]

  11. [11]
  12. [12]

    NNLO QCD predictions for single jet inclusive production at the LHC

    J. Currie, E. W. N. Glover, and J. Pires, Phys. Rev. Lett. 118, 072002 (2017), arXiv:1611.01460 [hep-ph]

  13. [13]

    Single jet inclusive production for the individual jet $p_{T}$ scale choice at the LHC

    J. Currie, E. W. N. Glover, T. Gehrmann, A. Gehrmann-De Ridder, A. Huss, and J. Pires, Acta Phys. Polon. B48, 955 (2017), arXiv:1704.00923 [hep-ph]

  14. [14]

    Infrared sensitivity of single jet inclusive production at hadron colliders

    J. Currie, A. Gehrmann-De Ridder, T. Gehrmann, E. W. N. Glover, A. Huss, and J. Pires, JHEP 10, 155 (2018), arXiv:1807.03692 [hep-ph]

  15. [15]

    New features in version 2 of the fastNLO project

    D. Britzger, K. Rabbertz, F. Stober, and M. Wobisch (fastNLO) (2012) pp. 217–221, arXiv:1208.3641 [hep-ph]

  16. [16]

    Theory-Data Comparisons for Jet Measurements in Hadron-Induced Processes

    M. Wobisch, D. Britzger, T. Kluge, K. Rabbertz, and F. Stober (fastNLO), (2011), arXiv:1109.1310 [hep-ph]

  17. [17]

    A posteriori inclusion of parton density functions in NLO QCD final-state calculations at hadron colliders: The APPLGRID Project

    T. Carli, D. Clements, A. Cooper-Sarkar, C. Gwenlan, G. P. Salam, F. Siegert, P. Starovoitov, and M. Sutton, Eur. Phys. J. C66, 503 (2010), arXiv:0911.2985 [hep-ph]

  18. [18]

    fastNLO tables for NNLO top-quark pair differential distributions

    M. Czakon, D. Heymes, and A. Mitov, (2017), arXiv:1704.08551 [hep-ph]

  19. [19]

    http://www.precision.hep.phy.cam.ac.uk/results/ttbar-fastnlo/

  20. [20]

    R. S. Thorne, S. Bailey, T. Cridge, L. A. Harland-Lang, A. D. Martin, and R. Nathvani (2019) p. 036, arXiv:1907.08147 [hep-ph]

  21. [21]

    B.-T. Wang, T. J. Hobbs, S. Doyle, J. Gao, T.-J. Hou, P. M. Nadolsky, and F. I. Olness, Phys. Rev. D98, 094030 (2018), arXiv:1803.02777 [hep-ph]

  22. [22]

    T. J. Hobbs, B.-T. Wang, P. M. Nadolsky, and F. I. Olness, (2019), arXiv:1904.00022 [hep-ph]

  23. [23]

    Uncertainties of predictions from parton distribution functions II: the Hessian method

    J. Pumplin, D. Stump, R. Brock, D. Casey, J. Huston, J. Kalk, H.-L. Lai, and W.-K. Tung, Phys. Rev. D65, 014013 (2001), arXiv:hep-ph/0101032 [hep-ph]

  24. [24]

    Pumplin, D

    J. Pumplin, D. R. Stump, J. Huston, H. L. Lai, P. M. Nadolsky, and W.-K. Tung, JHEP 07, 012 (2002), arXiv:hep- ph/0201195 [hep-ph]

  25. [25]

    Updating and Optimizing Error PDFs in the Hessian Approach

    C. Schmidt, J. Pumplin, and C.-P. Yuan, Phys. Rev. D98, 094005 (2018), arXiv:1806.07950 [hep-ph]

  26. [26]

    T.-J. Hou, Z. Yu, S. Dulat, C. Schmidt, and C. P. Yuan, (2019), arXiv:1907.12177 [hep-ph]

  27. [27]

    Uncertainties of Predictions from Parton Distribution Functions I: the Lagrange Multiplier Method

    D. Stump, J. Pumplin, R. Brock, D. Casey, J. Huston, J. Kalk, H.-L. Lai, and W.-K. Tung, Phys. Rev. D65, 014012 (2001), arXiv:hep-ph/0101051 [hep-ph]

  28. [28]

    Tanabashi et al

    M. Tanabashi et al. (Particle Data Group), Phys. Rev. D98, 030001 (2018)

  29. [29]

    H.-L. Lai, J. Huston, Z. Li, P. Nadolsky, J. Pumplin, D. Stump, and C. P. Yuan, Phys. Rev. D82, 054021 (2010), arXiv:1004.4624 [hep-ph]

  30. [30]

    Combination of Measurements of Inclusive Deep Inelastic $e^{\pm}p$ Scattering Cross Sections and QCD Analysis of HERA Data

    H. Abramowicz et al. (H1, ZEUS), Eur. Phys. J. C75, 580 (2015), arXiv:1506.06042 [hep-ex]

  31. [31]

    F. D. Aaron et al. (H1, ZEUS), JHEP 01, 109 (2010), arXiv:0911.0884 [hep-ex]

  32. [32]

    T.-J. Hou, S. Dulat, J. Gao, M. Guzzi, J. Huston, P. Nadolsky, J. Pumplin, C. Schmidt, D. Stump, and C. P. Yuan, Phys. Rev. D95, 034003 (2017), arXiv:1609.07968 [hep-ph]

  33. [33]

    F. D. Aaron et al. (H1), Eur. Phys. J. C71, 1579 (2011), arXiv:1012.4355 [hep-ex]

  34. [34]

    R. D. Ball, V. Bertone, M. Bonvini, S. Marzani, J. Rojo, and L. Rottoli, Eur. Phys. J. C78, 321 (2018), arXiv:1710.05935 [hep-ph]

  35. [35]

    Impact of low-$x$ resummation on QCD analysis of HERA data

    H. Abdolmaleki et al. (xFitter Developers’ Team), Eur. Phys. J. C78, 621 (2018), arXiv:1802.00064 [hep-ph]

  36. [36]

    Combination and QCD analysis of charm and beauty production cross-section measurements in deep inelastic $ep$ scattering at HERA

    H. Abramowicz et al. (H1, ZEUS), Eur. Phys. J. C 78, 473 (2018), arXiv:1804.01019 [hep-ex]

  37. [37]

    Kovaˇ r´ ık, P

    K. Kovaˇ r´ ık, P. M. Nadolsky, and D. E. Soper, (2019), arXiv:1905.06957 [hep-ph]

  38. [38]

    H.-L. Lai, M. Guzzi, J. Huston, Z. Li, P. M. Nadolsky, J. Pumplin, and C. P. Yuan, Phys. Rev. D82, 074024 (2010), arXiv:1007.2241 [hep-ph]

  39. [39]
  40. [40]

    The PDF4LHC report on PDFs and LHC data: Results from Run I and preparation for Run II

    J. Rojo et al., J. Phys. G42, 103103 (2015), arXiv:1507.00556 [hep-ph]

  41. [41]

    HERAFitter, Open Source QCD Fit Project

    S. Alekhin et al., Eur. Phys. J. C75, 304 (2015), arXiv:1410.4412 [hep-ph]

  42. [42]

    J. Gao, M. Guzzi, J. Huston, H.-L. Lai, Z. Li, P. Nadolsky, J. Pumplin, D. Stump, and C. P. Yuan, Phys. Rev. D89, 033009 (2014), arXiv:1302.6246 [hep-ph]

  43. [43]

    fastNLO: Fast pQCD Calculations for PDF Fits

    T. Kluge, K. Rabbertz, and M. Wobisch (2006) pp. 483–486, arXiv:hep-ph/0609285 [hep-ph]

  44. [44]

    An NNLO subtraction formalism in hadron collisions and its application to Higgs boson production at the LHC

    S. Catani and M. Grazzini, Phys. Rev. Lett. 98, 222002 (2007), arXiv:hep-ph/0703012 [hep-ph]

  45. [45]

    Vector boson production at hadron colliders: a fully exclusive QCD calculation at NNLO

    S. Catani, L. Cieri, G. Ferrera, D. de Florian, and M. Grazzini, Phys. Rev. Lett. 103, 082001 (2009), arXiv:0903.2120 103 [hep-ph]

  46. [46]

    J. M. Campbell and R. K. Ellis, Nucl. Phys. Proc. Suppl. 205-206, 10 (2010), arXiv:1007.3492 [hep-ph]

  47. [47]

    Color singlet production at NNLO in MCFM

    R. Boughezal, J. M. Campbell, R. K. Ellis, C. Focke, W. Giele, X. Liu, F. Petriello, and C. Williams, Eur. Phys. J. C77, 7 (2017), arXiv:1605.08011 [hep-ph]

  48. [48]

    J. M. Campbell, R. K. Ellis, and W. T. Giele, Eur. Phys. J. C75, 246 (2015), arXiv:1503.06182 [physics.comp-ph]

  49. [49]

    FEWZ 2.0: A code for hadronic Z production at next-to-next-to-leading order

    R. Gavin, Y. Li, F. Petriello, and S. Quackenbush, Comput. Phys. Commun. 182, 2388 (2011), arXiv:1011.3540 [hep-ph]

  50. [50]

    W physics at the LHC with FEWZ 2.1

    R. Gavin, Y. Li, F. Petriello, and S. Quackenbush, Comput. Phys. Commun. 184, 208 (2013), arXiv:1201.5896 [hep-ph]

  51. [51]

    Combining QCD and electroweak corrections to dilepton production in FEWZ

    Y. Li and F. Petriello, Phys. Rev. D86, 094034 (2012), arXiv:1208.5967 [hep-ph]

  52. [52]

    Precise QCD predictions for the production of a Z boson in association with a hadronic jet

    A. Gehrmann-De Ridder, T. Gehrmann, E. W. N. Glover, A. Huss, and T. A. Morgan, Phys. Rev. Lett. 117, 022001 (2016), arXiv:1507.02850 [hep-ph]

  53. [53]

    NNLO QCD corrections to the transverse momentum distribution of weak gauge bosons

    A. Gehrmann-De Ridder, T. Gehrmann, E. W. N. Glover, A. Huss, and D. M. Walker, Phys. Rev. Lett. 120, 122001 (2018), arXiv:1712.07543 [hep-ph]

  54. [54]

    G. A. Ladinsky and C.-P. Yuan, Phys. Rev. D50, R4239 (1994), arXiv:hep-ph/9311341 [hep-ph]

  55. [55]

    Soft gluon effects on lepton pairs at hadron colliders

    C. Balazs and C.-P. Yuan, Phys. Rev. D56, 5558 (1997), arXiv:hep-ph/9704258 [hep-ph]

  56. [56]

    P. M. Nadolsky and Z. Sullivan, eConf C010630, P510 (2001), arXiv:hep-ph/0110378 [hep-ph]

  57. [57]

    P. M. Nadolsky, H.-L. Lai, Q.-H. Cao, J. Huston, J. Pumplin, D. Stump, W.-K. Tung, and C. P. Yuan, Phys. Rev. D78, 013004 (2008), arXiv:0802.0007 [hep-ph]

  58. [58]

    W. G. Seligman, Ph.D. thesis, Nevis Labs, Columbia U. (1997)

  59. [59]

    A Measurement of $R ={\sigma_L}/{\sigma_T}$ in Deep Inelastic Neutrino-Nucleon Scattering at the Tevatron

    U.-K. Yang et al. (CCFR/NuTeV), J. Phys. G22, 775 (1996), arXiv:hep-ex/9605005 [hep-ex]

  60. [60]

    Inclusive $W$ and $Z$ production in the forward region at $\sqrt{s} = 7$ TeV

    R. Aaij et al. (LHCb), JHEP 06, 058 (2012), arXiv:1204.1620 [hep-ex]

  61. [61]

    Measurement of inclusive jet and dijet production in pp collisions at sqrt(s) = 7 TeV using the ATLAS detector

    G. Aad et al. (ATLAS), Phys. Rev. D86, 014022 (2012), arXiv:1112.6297 [hep-ex]

  62. [62]

    Measurements of differential jet cross sections in proton-proton collisions at sqrt(s) = 7 TeV with the CMS detector

    S. Chatrchyan et al. (CMS), Phys. Rev. D87, 112002 (2013), [Erratum: Phys. Rev.D87,no.11,119902(2013)], arXiv:1212.6660 [hep-ex]

  63. [63]

    A. C. Benvenuti et al. (BCDMS), Phys. Lett. B223, 485 (1989)

  64. [64]

    A. C. Benvenuti et al. (BCDMS), Phys. Lett. B237, 592 (1990)

  65. [65]

    Measurement of the proton and deuteron structure functions, F2p and F2d, and of the ratio sigma(L)/sigma(T)

    M. Arneodo et al. (New Muon), Nucl. Phys. B483, 3 (1997), arXiv:hep-ph/9610231 [hep-ph]

  66. [66]

    J. P. Berge et al., Z. Phys. C49, 187 (1991)

  67. [67]

    Measurements of F_2 and xF_3(nu)-xF_3(nubar) from CCFR nu_mu-Fe and nubar_mu-Fe data in a physics model independent way

    U.-K. Yang et al. (CCFR/NuTeV), Phys. Rev. Lett. 86, 2742 (2001), arXiv:hep-ex/0009041 [hep-ex]

  68. [68]

    W. G. Seligman et al., Phys. Rev. Lett. 79, 1213 (1997), arXiv:hep-ex/9701017 [hep-ex]

  69. [69]

    D. A. Mason, Ph.D. thesis, Oregon U. (2006)

  70. [70]
  71. [71]

    Measurement of F_2^ccbar and F_2^bbbar at High Q^2 using the H1 Vertex Detector at HERA

    A. Aktas et al. (H1), Eur. Phys. J. C40, 349 (2005), arXiv:hep-ex/0411046 [hep-ex]

  72. [72]

    Combination and QCD Analysis of Charm Production Cross Section Measurements in Deep-Inelastic ep Scattering at HERA

    H. Abramowicz et al. (ZEUS, H1), Eur. Phys. J. C73, 2311 (2013), arXiv:1211.1182 [hep-ex]

  73. [73]

    Moreno et al., Phys

    G. Moreno et al., Phys. Rev. D43, 2815 (1991)

  74. [74]

    R. S. Towell et al. (NuSea), Phys. Rev. D64, 052002 (2001), arXiv:hep-ex/0103030 [hep-ex]

  75. [75]

    J. C. Webb et al. (NuSea), (2003), arXiv:hep-ex/0302019 [hep-ex]

  76. [76]

    Measurement of the lepton charge asymmetry in W-boson decays produced in p-pbar collisions

    F. Abe et al. (CDF), Phys. Rev. Lett. 81, 5754 (1998), arXiv:hep-ex/9809001

  77. [77]

    Measurement of the Forward-Backward Charge Asymmetry from W --> e nu Production in p anti-p Collisions at s**(1/2) = 1.96 TeV

    D. Acosta et al. (CDF), Phys. Rev. D71, 051104 (2005), arXiv:hep-ex/0501023 [hep-ex]

  78. [78]

    V. M. Abazov et al. (D0), Phys. Rev. D77, 011106 (2008), arXiv:0709.4254 [hep-ex]

  79. [79]
  80. [80]

    T. A. Aaltonen et al. (CDF), Phys. Lett. B692, 232 (2010), arXiv:0908.3914 [hep-ex]

Showing first 80 references.