10,445 results on '"PARTON"'
Search Results
2. Matching of fracture functions for SIDIS in target fragmentation region
- Author
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Kai-bao Chen, Jian-Ping Ma, and X. B. Tong
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Physics ,Quantum chromodynamics ,Nuclear and High Energy Physics ,Particle physics ,Logarithm ,High Energy Physics::Phenomenology ,FOS: Physical sciences ,Virtual particle ,Parton ,QC770-798 ,Lambda ,Deep inelastic scattering ,QCD Phenomenology ,High Energy Physics - Phenomenology ,High Energy Physics - Phenomenology (hep-ph) ,Factorization ,Nuclear and particle physics. Atomic energy. Radioactivity ,Resummation ,Nuclear Experiment ,Deep Inelastic Scattering (Phenomenology) - Abstract
In the target fragmentation region of Semi-Inclusive Deep Inelastic Scattering, the diffractively produced hadron has small transverse momentum. If it is at order of $\Lambda_{QCD}$, it prevents to make predictions with the standard collinear factorization. However, in this case, differential cross-sections can be predicted by the factorization with fracture functions, diffractive parton distributions. If the transverse momentum is much larger than $\Lambda_{QCD}$ but much smaller than $Q$ which is the virtuality of the virtual photon, both factorizations apply. In this case, fracture functions can be factorized with collinear parton distributions and fragmentation functions. We study the factorization up to twist-3 level and obtain gauge invariant results. They will be helpful for modeling fracture functions and useful for resummation of large logarithm of the transverse momentum appearing in collinear factorization., Comment: Published version
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- 2021
3. Effect of color reconnection and rope formation on resonance production in p–p collisions in Pythia 8
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Ankita Goswami, Basanta Kumar Nandi, Ranjit Nayak, and Sadhana Dash
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Computer Science::Machine Learning ,Quark ,Particle physics ,Strange quark ,Physics and Astronomy (miscellaneous) ,Nuclear Theory ,FOS: Physical sciences ,Parton ,QC770-798 ,Astrophysics ,Computer Science::Digital Libraries ,Statistics::Machine Learning ,High Energy Physics - Phenomenology (hep-ph) ,Nuclear and particle physics. Atomic energy. Radioactivity ,Nuclear Experiment ,Engineering (miscellaneous) ,Event generator ,Quantum chromodynamics ,Physics ,High Energy Physics::Phenomenology ,Hadronization ,Baryon ,QB460-466 ,High Energy Physics - Phenomenology ,Content (measure theory) ,Computer Science::Mathematical Software ,High Energy Physics::Experiment - Abstract
Resonance production in proton–proton collisions at$$\sqrt{s} = 7$$s=7TeV and 13 TeV have been investigated using a Pythia 8 event generator within the framework of microscopic processes including color reconnection and rope hadronization. Specifically, the observable effects of different modes of color reconnections on the ratio of yields of mesonic and baryonic resonances with respect to their stable counterpart have been explored as a function of mean charged particle multiplicity. A suppression in the ratio is observed as a function of the mean number of charged particles for mesonic resonances. The$$\phi /\mathrm {K}$$ϕ/Kand$${\phi /\pi }$$ϕ/πratios show an enhancement for high-multiplicity events due to enhanced production of strange quarks via the microscopic process of rope hadronization in the partonic phase. The mechanism of the hadronization of color ropes together with the quark–gluon plasma (QCD)-based color reconnection of partons predicted an enhancement in the ratio for baryonic resonances to non-resonance baryons having similar quark content. The yield ratios of resonances are found to be independent of the collision energy and strongly dependent on event activity.
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- 2021
4. A new approach to semi-inclusive deep-inelastic scattering with QED and QCD factorization
- Author
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Tiehui Liu, Nobuo Sato, Wally Melnitchouk, and Jian-Wei Qiu
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Quantum chromodynamics ,Physics ,Nuclear and High Energy Physics ,Particle physics ,Forcing (recursion theory) ,Nuclear Theory ,Scattering ,High Energy Physics::Phenomenology ,FOS: Physical sciences ,Parton ,QC770-798 ,Deep inelastic scattering ,High Energy Physics - Experiment ,Nuclear Theory (nucl-th) ,High Energy Physics - Experiment (hep-ex) ,High Energy Physics - Phenomenology ,High Energy Physics - Phenomenology (hep-ph) ,Factorization ,Nuclear and particle physics. Atomic energy. Radioactivity ,Transverse momentum ,Nuclear Experiment (nucl-ex) ,Nuclear Experiment ,Deep Inelastic Scattering (Phenomenology) - Abstract
We present the details of a new factorized approach to semi-inclusive deep-inelastic scattering which treats QED and QCD radiation on equal footing, and provides a systematically improvable approximation to the extraction of transverse momentum dependent parton distributions. We demonstrate how the QED contributions can be well approximated by collinear factorization, and illustrate the application of the factorized approach to QED radiation in inclusive scattering. For semi-inclusive processes, we show how radiation effects prevent a well-defined "photon-nucleon" frame, forcing one to use a two-step process to account for the radiation. We illustrate the utility of the new method by explicit application to the spin-dependent Sivers and Collins asymmetries., 55 pages, 23 figures, accepted for publication in J. High Energy Phys
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- 2021
5. Kaon generalized parton distributions and light-front wave functions in the Nambu–Jona-Lasinio model
- Author
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Jin-Li Zhang and Jialun Ping
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Quark ,Physics ,Strange quark ,Particle physics ,Physics and Astronomy (miscellaneous) ,Center (category theory) ,Parton ,QC770-798 ,Astrophysics ,Regularization (mathematics) ,QB460-466 ,Distribution function ,Nuclear and particle physics. Atomic energy. Radioactivity ,Impact parameter ,Engineering (miscellaneous) ,Energy (signal processing) - Abstract
Kaon generalized parton distributions (GPDs) and the leading Fock state light-front wave functions are investigated in the framework of Nambu–Jona-Lasinio model with proper time regularization. In addition, we compared the form factors, parton distribution functions, and generalized form factors obtained from them, respectively. The first Mellin moments of GPDs result in the form factors of local currents. The second Mellin moments of vector GPDs are related to gravitational form factors, the quark mass distribution $$\theta _2$$ θ 2 and the quark pressure distribution $$\theta _1$$ θ 1 . When taking a Fourier transform of GPDs in impact parameter space, we can get the mean-squared impact parameter for the quarks of the kaon: $$\langle {\varvec{b}}_{\bot }^2\rangle _K^u=0.149$$ ⟨ b ⊥ 2 ⟩ K u = 0.149 fm$$^2$$ 2 , $$\langle {\varvec{b}}_{\bot }^2\rangle _K^s=0.088$$ ⟨ b ⊥ 2 ⟩ K s = 0.088 fm$$^2$$ 2 . This means that the kaon s quark is nearer to the center of transverse momentum than the u quark. We also give the light-cone energy radius for the quarks of the kaon from the mass distribution $$\theta _2$$ θ 2 : $$r_{E,LC}^{u,K}=0.187 $$ r E , L C u , K = 0.187 fm, $$ r_{E,LC}^{s,K}=0.167$$ r E , L C s , K = 0.167 fm, and the light-cone charge radius from quark form factors of the kaon: $$r_{c,LC}^{u,K}=0.390 $$ r c , L C u , K = 0.390 fm, $$r_{c,LC}^{s,K}=0.296 $$ r c , L C s , K = 0.296 fm, which means that the s quark has a smaller extent than the u quark. The light-front transverse-spin distributions $$\rho _u^1\left( {\varvec{b}}_{\bot },{\varvec{s}}_{\perp }\right) $$ ρ u 1 b ⊥ , s ⊥ and $$\rho _u^2\left( {\varvec{b}}_{\bot },{\varvec{s}}_{\perp }\right) $$ ρ u 2 b ⊥ , s ⊥ show distortions, the average shift are $$\langle b_{\bot }^y\rangle _1^u=0.116$$ ⟨ b ⊥ y ⟩ 1 u = 0.116 fm and $$\langle b_{\bot }^y\rangle _2^u=0.083$$ ⟨ b ⊥ y ⟩ 2 u = 0.083 fm. On the kinematic domain associated with the valence-quark dominance, the unpolarized Wigner distribution from light-front wave functions is sharply peaked. It extends as the transverse position variable increases in magnitude and has a domain of negative support. Through the comparison of distributions from the two methods, we find that they give the same multi-dimensional mapping of the kaon in the Nambu–Jona-Lasinio model.
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- 2021
6. Spin correlations in final-state parton showers and jet observables
- Author
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Karlberg, A, Salam, GP, Scyboz, L, and Verheyen, R
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Physics ,Particle physics ,Physics and Astronomy (miscellaneous) ,Logarithm ,010308 nuclear & particles physics ,FOS: Physical sciences ,Observable ,Parton ,QC770-798 ,Jet (particle physics) ,Astrophysics ,01 natural sciences ,QB460-466 ,Dipole ,High Energy Physics - Phenomenology ,High Energy Physics - Phenomenology (hep-ph) ,13. Climate action ,Nuclear and particle physics. Atomic energy. Radioactivity ,0103 physical sciences ,High Energy Physics::Experiment ,Resummation ,010306 general physics ,Engineering (miscellaneous) ,Quantum ,Spin-½ - Abstract
As part of a programme to develop parton showers with controlled logarithmic accuracy, we consider the question of collinear spin correlations within the PanScales family of parton showers. We adapt the well-known Collins-Knowles spin-correlation algorithm to PanScales antenna and dipole showers, using an approach with similarities to that taken by Richardson and Webster. To study the impact of spin correlations, we develop Lund-declustering based observables that are sensitive to spin-correlation effects both within and between jets and extend the MicroJets collinear single-logarithmic resummation code to include spin correlations. Together with a 3-point energy correlation observable proposed recently by Chen, Moult and Zhu, this provides a powerful set of constraints for validating the logarithmic accuracy of our shower results. The new observables and their resummation further open the pathway to phenomenological studies of these important quantum mechanical effects., 30 pages + appendices, 21 figures; v2: matches published version
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- 2021
7. Soft-drop grooming for hadronic event shapes
- Author
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Jeremy Baron, Daniel Reichelt, Vincent Theeuwes, Steffen Schumann, and Niklas Schwanemann
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Nuclear and High Energy Physics ,Particle physics ,Logarithm ,FOS: Physical sciences ,Parton ,QC770-798 ,01 natural sciences ,High Energy Physics - Experiment ,High Energy Physics - Experiment (hep-ex) ,Matrix (mathematics) ,High Energy Physics - Phenomenology (hep-ph) ,Nuclear and particle physics. Atomic energy. Radioactivity ,0103 physical sciences ,Perturbative QCD ,Resummation ,010306 general physics ,Nuclear Experiment ,Complement (set theory) ,Event generator ,Quantum chromodynamics ,Physics ,010308 nuclear & particles physics ,High Energy Physics::Phenomenology ,High Energy Physics - Phenomenology ,High Energy Physics::Experiment ,Event (particle physics) - Abstract
Soft-drop grooming of hadron-collision final states has the potential to significantly reduce the impact of non-perturbative corrections, and in particular the underlying-event contribution. This eventually will enable a more direct comparison of accurate perturbative predictions with experimental measurements. In this study we consider soft-drop groomed dijet event shapes. We derive general results needed to perform the resummation of suitable event-shape variables to next-to-leading logarithmic (NLL) accuracy matched to exact next-to-leading order (NLO) QCD matrix elements. We compile predictions for the transverse-thrust shape accurate to NLO+NLL' using the implementation of the CAESAR formalism in the Sherpa event generator framework. We complement this by state-of-the-art parton- and hadron-level predictions based on NLO QCD matrix elements matched with parton showers. We explore the potential to mitigate non-perturbative corrections for particle-level and track-based measurements of transverse thrust by considering a wide range of soft-drop parameters. We find that soft-drop grooming indeed is very efficient in removing the underlying event. This motivates future experimental measurements to be compared to precise QCD predictions and employed to constrain non-perturbative models in Monte-Carlo simulations., 50 pages, 21 figures, extended discussion, version accepted for publication in JHEP
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- 2021
8. Multiparton distribution functions in quantum chromodynamics
- Author
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Gennadii Mikhailovich Zinovjev and Aleksandr Mikhailovich Snigirev
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Physics ,Quantum chromodynamics ,Particle physics ,Distribution function ,Distribution (number theory) ,High Energy Physics::Phenomenology ,General Physics and Astronomy ,High Energy Physics::Experiment ,Parton ,Nuclear Experiment - Abstract
The structure of hadrons (protons) and the dynamics of their interaction are usually studied in collisional experiments by exploring hard single parton–parton scattering described in terms of structure functions (single-particle distributions). Completely new and unique information comes from the selection and analysis of events in which two (or more) hard parton scatterings concurrently occur in a single (Tevatron; FermiLab, USA) or pp (LHC; CERN, Switzerland) collision. The simulation of such double (multiple) parton scatterings involves two-parton (multiparton) distribution functions. Properties of these functions, which may be extracted from quantum chromodynamics, are reviewed.
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- 2021
9. Erratum to: Transverse momentum in double parton scattering: factorisation, evolution and matching
- Author
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Markus Diehl, Tomas Kasemets, and Maarten G. A. Buffing
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Nuclear and High Energy Physics ,Matching (statistics) ,Particle physics ,parton: distribution function ,Parton ,QC770-798 ,transverse momentum ,nonperturbative ,parton: scattering ,Factorization ,factorization ,Nuclear and particle physics. Atomic energy. Radioactivity ,NLO Computations ,ddc:530 ,Collins ,Physics ,transverse momentum dependence [distribution function] ,Scattering ,scale: renormalization ,renormalization [scale] ,QCD Phenomenology ,multiple scattering ,scattering [parton] ,distribution function: transverse momentum dependence ,rapidity ,resummation ,evolution equation ,Transverse momentum ,distribution function [parton] - Abstract
Journal of high energy physics 07(7), 046 (2021). doi:10.1007/JHEP07(2021)046, Published by SISSA, [Trieste]
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- 2021
10. Differential $$\boldsymbol{W}^{{+}}{/}\boldsymbol{W}^{{-}}$$ Cross Section Ratios for $$\boldsymbol{W}$$ Plus Jet Production in $$\boldsymbol{pp}$$ Collisions Through (N)NLO in QCD
- Author
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K. Ocalan
- Subjects
Quantum chromodynamics ,Physics ,Nuclear and High Energy Physics ,Particle physics ,Large Hadron Collider ,High Energy Physics::Phenomenology ,Perturbative QCD ,Parton ,Jet (particle physics) ,Atomic and Molecular Physics, and Optics ,Distribution function ,High Energy Physics::Experiment ,Rapidity ,Nuclear Experiment ,Boson - Abstract
This paper presents a phenomenological study of differential $$W^{+}/W^{-}$$ cross section ratios for $$W$$ -boson production in association with a jet through next-to-leading-order (NLO) and next-to-NLO (NNLO) calculations in perturbative QCD based on the $$q_{T}$$ -subtraction approach. The $$W^{+}/W^{-}$$ cross section ratios are calculated for proton–proton collisions at both 8 and 13 TeV energies. The differential distributions for the ratios are presented as functions of important variables that are sensitive to perturbative QCD corrections including the transverse momentum of the W boson, the transverse momentum of the leading jet, and the absolute rapidity of the leading jet. The predicted distributions at (N)NLO accuracy are compared with the 8 TeV data from the ATLAS experiment at the LHC. The differential distributions at 13 TeV are compared at (N)NLO using different parton distribution functions (PDFs) to assess sensitivity of calculations to different PDF models. The presented ratios are found to be under good control by the (N)NLO calculations for most of the phase space regions.
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- 2021
11. Unpolarized quark and gluon TMD PDFs and FFs at N3LO
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Yu Jiao Zhu, Tong-Zhi Yang, Hua Xing Zhu, Mingxing Luo, University of Zurich, and Zhu, Hua Xing
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Quark ,Nuclear and High Energy Physics ,Particle physics ,Nuclear Theory ,530 Physics ,FOS: Physical sciences ,Parton ,10192 Physics Institute ,QC770-798 ,Nuclear Theory (nucl-th) ,symbols.namesake ,High Energy Physics - Phenomenology (hep-ph) ,Nuclear and particle physics. Atomic energy. Radioactivity ,Perturbative QCD ,Feynman diagram ,3106 Nuclear and High Energy Physics ,Resummation ,Quantum chromodynamics ,Physics ,Analytic continuation ,High Energy Physics::Phenomenology ,Gluon ,High Energy Physics - Phenomenology ,symbols - Abstract
In this paper we calculate analytically the perturbative matching coefficients for unpolarized quark and gluon Transverse-Momentum-Dependent (TMD) Parton Distribution Functions (PDFs) and Fragmentation Functions (FFs) through Next-to-Next-to-Next-to-Leading Order (N$^3$LO) in QCD. The N$^3$LO TMD PDFs are calculated by solving a system of differential equation of Feynman and phase space integrals. The TMD FFs are obtained by analytic continuation from space-like quantities to time-like quantities, taking into account the probability interpretation of TMD PDFs and FFs properly. The coefficient functions for TMD FFs exhibit double logarithmic enhancement at small momentum fraction $z$. We resum such logarithmic terms to the third order in the expansion of $\alpha_s$. Our results constitute important ingredients for precision determination of TMD PDFs and FFs in current and future experiments., Comment: references added
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- 2021
12. Heavy-flavor hadro-production with heavy-quark masses renormalized in the MS ¯ $$ \overline{\mathrm{MS}} $$ , MSR and on-shell schemes
- Author
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L. Kemmler, Maria Vittoria Garzelli, O. Zenaiev, and Sven Moch
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High Energy Physics::Lattice ,parton: distribution function ,correction [quantum chromodynamics] ,Parton ,pair production [top] ,01 natural sciences ,quantum chromodynamics: correction ,High Energy Physics - Experiment ,heavy quark: production ,High Energy Physics - Experiment (hep-ex) ,High Energy Physics - Phenomenology (hep-ph) ,mass [heavy quark] ,Physics ,Quantum chromodynamics ,Large Hadron Collider ,mass: renormalization ,higher-order: 1 ,on-shell [renormalization] ,hep-ph ,QCD Phenomenology ,heavy quark: mass ,High Energy Physics - Phenomenology ,CERN LHC Coll ,renormalization: on-shell ,scale dependence ,mass [top] ,top: pair production ,distribution function [parton] ,Particle Physics - Experiment ,1 [higher-order] ,Quark ,Nuclear and High Energy Physics ,Particle physics ,small-x ,top: mass ,FOS: Physical sciences ,Renormalization ,Factorization ,factorization ,NLO Computations ,0103 physical sciences ,ddc:530 ,lcsh:Nuclear and particle physics. Atomic energy. Radioactivity ,010306 general physics ,Particle Physics - Phenomenology ,010308 nuclear & particles physics ,hep-ex ,High Energy Physics::Phenomenology ,renormalization [mass] ,gluon ,Gluon ,Distribution function ,production [heavy quark] ,lcsh:QC770-798 ,High Energy Physics::Experiment - Abstract
Journal of high energy physics 2021(04), 043 (2021). doi:10.1007/JHEP04(2021)043, We present predictions for heavy-quark production at the Large Hadron Collider making use of the $ \overline{\mathrm{MS}} $ and MSR renormalization schemes for the heavy-quark mass as alternatives to the widely used on-shell renormalization scheme. We compute single and double differential distributions including QCD corrections at next-to-leading order and investigate the renormalization and factorization scale dependence as well as the perturbative convergence in these mass renormalization schemes. The implementation is based on publicly available programs, MCFM and xFitter, extending their capabilities. Our results are applied to extract the top-quark mass using measurements of the total and differential $ t\overline{t} $ production cross-sections and to investigate constraints on parton distribution functions, especially on the gluon distribution at low x values, from available LHC data on heavy-flavor hadro-production., Published by SISSA, [Trieste]
- Published
- 2021
13. Momentum-Kick Model Application to High-Multiplicity pp Collisions at $\sqrt {s}=13$ TeV at the LHC
- Author
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Beomkyu Kim, Jin-Hee Yoon, Hanul Youn, and Soyeon Cho
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Particle physics ,Nuclear Theory ,nucl-th ,Physics and Astronomy (miscellaneous) ,General Mathematics ,FOS: Physical sciences ,Parton ,High multiplicity ,01 natural sciences ,Nuclear Theory (nucl-th) ,Momentum ,High Energy Physics - Phenomenology (hep-ph) ,Atlas (anatomy) ,0103 physical sciences ,medicine ,Nuclear Experiment ,010306 general physics ,Particle Physics - Phenomenology ,Physics ,Large Hadron Collider ,010308 nuclear & particles physics ,Momentum transfer ,hep-ph ,Ridge (differential geometry) ,Collision ,High Energy Physics - Phenomenology ,medicine.anatomical_structure ,Nuclear Physics - Theory - Abstract
In this study, the momentum-kick model is used to understand the ridge behaviours in dihadron $\Delta\eta$--$\Delta\varphi$ correlations recently reported by the LHC in high-multiplicity proton-proton (pp) collisions. The kick stand model is based on a momentum kick by leading jets to partons in the medium close to the leading jets. The medium where partons move freely is assumed in the model regardless of collision systems. This helps us apply the method to small systems like pp collisions in a simple way. Also, the momentum transfer is purely kinematic and this provides us a strong way to approach the ridge behaviour analytically. There are already several results with this approach in high-energy heavy-ion collisions from the STAR and PHENIX at RHIC and from the CMS at LHC. The momentum-kick model is extended to the recent ridge results in high-multiplicity pp collisions with the ATLAS and CMS at LHC. The medium property in high-multiplicity pp collisions is diagnosed with the result of the model., Comment: 10 pages, 2 tables and 3 figures
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- 2021
14. $${W}^{{\pm}}{/Z}$$ Cross Section Ratios Through (N)NLO Predictions in QCD
- Author
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K. Ocalan
- Subjects
Physics ,Quantum chromodynamics ,Nuclear and High Energy Physics ,Particle physics ,Large Hadron Collider ,010308 nuclear & particles physics ,High Energy Physics::Phenomenology ,Perturbative QCD ,Parton ,Jet (particle physics) ,01 natural sciences ,Atomic and Molecular Physics, and Optics ,Distribution function ,Pseudorapidity ,0103 physical sciences ,High Energy Physics::Experiment ,Nuclear Experiment ,010306 general physics ,Boson - Abstract
This paper presents $$W^{\pm}/Z$$ cross section ratio predictions for the $$W$$ and $$Z$$ boson productions in their subsequent electron decay channels with next-to-leading order (NLO) and next-to-next-to-leading order (NNLO) calculations in perturbative QCD. The predicted ratios from the fiducial cross sections are primarily compared with the ATLAS measurement based on 13 TeV LHC proton–proton collisions. The predicted fiducial ratios for 14 TeV proton–proton collisions are also presented at (N)NLO accuracies. The 13 TeV and 14 TeV differential distributions for the ratios are provided as a function of the boson transverse momentum at NNLO using different parton distribution functions (PDFs). The 13 TeV and 14 TeV differential distributions for the ratios are also provided for the boson production in association with at least one jet as functions of the first leading jet transverse momentum and absolute pseudorapidity at NLO using various PDF sets. The focus is to predict the ratios more precisely in terms of the reduced theoretical scale uncertainties for the fiducial calculations and to assess sensitivity of the ratios to different PDF sets for the differential calculations. The 13 TeV ratio is predicted as 10.55 $$\pm$$ 0.35 at NLO and 10.57 $$\pm$$ 0.07 at NNLO and found to be in good agreement with the ATLAS data. The 14 TeV ratio is predicted consistently as 10.50 $$\pm$$ 0.36 at NLO and 10.37 $$\pm$$ 0.07 at NNLO. Estimated scale uncertainties are reduced to less than percent level at NNLO in the fiducial ratios. The differential ratios distributions are consistently predicted by using different PDF sets at both 13 TeV and 14 TeV. The differential ratios exhibit more sensitivity to choice of PDF sets in higher regions of the distributions.
- Published
- 2021
15. Measurements of the inclusive and differential production cross sections of a top-quark-antiquark pair in association with a Z boson at √s = 13 TeV with the ATLAS detector
- Author
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Aad, Georges, Abbott, Braden Keim, Abbott, Dale, Abed Abud, Adam, Abeling, Kira, Abhayasinghe, Deshan Kavishka, Abidi, Haider, Abouzeid, Hass, Abouzeid, Ossama, Abraham, Nicola Louise, Abramowicz, Halina, Abreu, Henso, Abulaiti, Yiming, Acharya, Bobby Samir, Achkar, Baida, Adam, Lennart, Adam Bourdarios, Claire, Adamczyk, Leszek, Adamek, Lukas, Adelman, Jahred, Adiguzel, Aytul, Adorni Braccesi Chiassi, Sofia, Adye, Tim, Adye, Timothy John, Affolder, Tony, Affolder, Anthony, Afik, Yoav, Agapopoulou, Christina, Agaras, Merve Nazlim, Aggarwal, Anamika, Agheorghiesei, Catalin, Aguilar Saavedra, Juan Antonio, Ahmad, Ammara, Ahmadov, Faig, Ahmed, Waleed Syed, Ai, Xiaocong, Aielli, Giulio, Akatsuka, Shunichi, Akbiyik, Melike, Akesson, Torsten, Akilli, Ece, Akimov, Andrei, Al Khoury, Konie, Alberghi, Gian Luigi, Albert, Justin, Verzini, M.J. Alconada, Alderweireldt, Sara, Aleksa, Martin, Aleksandrov, I.N., Alexa, Calin, Alexopoulos, Theodoros, Alfonsi, Alice, Alfonsi, Fabrizio, Alhroob, Muhammad, Ali, Babar, Ali, Shahzad, Aliev, Malik, Alimonti, Gianluca, Allaire, Corentin, Allbrooke, Benedict, Allen, Benjamin William, Allport, Philip Patrick, Aloisio, Alberto, Alonso, Francisco, Alpigiani, Cristiano, Alunno Camelia, Elio, Alvarez Estevez, Manuel, Alviggi, Mariagrazia, Do Amaral Coutinho, Yara, Ambler, Alessandro, Ambroz, Luca, Amelung, Christoph, Amidei, Dante, Amor dos Santos, Susana Patricia, Amoroso, Simone, Amrouche, Cherifa Sabrina, An, Fenfen, Anastopoulos, Christos, Andari, Nansi, Andeen, Timothy Robert, Anders, John Kenneth, Andrean, Stefio Yosse, Andreazza, Attilio, Andrei, Victor, Anelli, Christopher Ryan, Angelidakis, Stylianos, Angerami, Aaron, Anisenkov, Alexey, Annovi, Alberto, Antel, Claire, Anthony, Matthew Thomas, Antipov, Egor, Antonelli, Mario, Antrim, Daniel Joseph, Anulli, Fabio, Aoki, Masato, Aparisi Pozo, Javier Alberto, Aparo, Marco, Aperio Bella, Ludovica, Aranzabal Barrio, Nordin, Araujo Ferraz, Victor, Pereira, R.Araujo, Arcangeletti, Chiara, Arce, Ayana Tamu, Arguin, Jean-Francois, Argyropoulos, Spyros, Argyropoulos, Spyridon, Arling, Jan-Hendrik, Armbruster, Aaron James, Armstrong, Alexander, Arnaez, Olivier, Arnold, Hannah, Arrubarrena Tame, Zulit Paola, Artoni, Giacomo, Asada, Haruka, Asai, Kanae, Asai, Shoji, Asawatavonvanich, Thanawat, Asbah, Nedaa Alexandra, Asimakopoulou, Eleni Myrto, Asquith, Lily, Assahsah, Jihad, Assamagan, Ketevi Adikle, Astalos, Robert, Atkin, Ryan Justin, Atkinson, Markus Julian, Atlay, Naim Bora, Atmani, Hicham, Atmasiddha, Prachi, Augsten, Kamil, Austrup, Volker Andreas, Avolio, Giuseppe, Ayoub, Mohamad Kassem, Azuelos, Georges, Babal, Dominik, Bachacou, Henri, Bachas, Dinos, Bachas, Konstantinos, Backman, Karl Filip, Bagnaia, Paolo, Bahrasemani, H., Bahrasemani, Sina, Bailey, Adam, Bailey, Virginia, Baines, John, Bakalis, Christos, Baker, Keith, Bakker, Pepijn Johannes, Bakos, Evelin, Bakshi Gupta, Debottam, Balaji, Shyam, Balasubramanian, Rahul, Baldin, Evgenii, Balek, Petr, Balli, Fabrice, Balunas, William Keaton, Balz, Johannes, Banas, Elzbieta, Bandieramonte, Marilena, Bandyopadhyay, Anjishnu, Banerjee, Sw., Banerjee, Swagato, Barak, Liron, Barbe, William Mickael, Barberio, Elisabetta, Barberis, Dario, Barbero, Marlon Benoit, Barbour, Gregory, Barillari, Teresa, Barisits, Martin, Barkeloo, Jason Tyler Colt, Barklow, Tim, Barklow, Timothy Laurence, Barnea, Rotem, Barnett, Bruce M, Barnett, Michael, Barnovska-Blenessy, Z., Baroncelli, Toni, Baroncelli, Antonio, Barone, Gaetano, Barr, Alan, Barranco Navarro, Laura, Barreiro Alonso, Fernando, Barreiro Guimaraes da Costa, Joao, Barron, Uriel, Barsov, Sergey, Bartels, Falk, Bartoldus, Rainer, Bartolini, Giovanni, Barton, Adam Edward, Bartos, Pavol, Basalaev, Artem, Basan, Alexander, Bassalat, Ahmed, Basso, Matthew Joseph, Bates, Richard, Batlamous, Souad, Batley, Richard, Batool, Binish, Battaglia, Marco, Bauce, Matteo, Bauer, Florian, Bauer, Patrick, Bawa, Harinder Singh, Bayirli, Arif, Beacham, James, Beau, Tristan, Beauchemin, Pierre-Hugues, Becherer, Fabian, Bechtle, Philip, Beck, Helge Christoph, Beck, Hans Peter, Beck, Hanspeter, Becker, Kathrin, Becot, Cyril Pascal, Beddall, Ayda, Beddall, Andrew, Bednyakov, Vadim, Bedognetti, Matteo, Bee, Chris, Bee, Christopher Peter, Beermann, Thomas, Begalli, Marcia, Begel, Michael, Behera, Arabinda, Behr, Janna Katharina, Beisiegel, Florian, Belfkir, Mohamed, Bell, Andrew Stuart, Bella, Gideon, Bellagamba, Lorenzo, Bellerive, Alain, Bellos, Panagiotis, Beloborodov, Konstantin, Belotskiy, Konstantin, Belyaev, Nikita, Benchekroun, Driss, Benekos, Nectarios, Benhammou, Yan, Benjamin, Doug, Benjamin, Douglas Paul, Benoit, Mathieu, Bensinger, Jim, Bensinger, James, Bentvelsen, Stan, Bentvelsen, Stanislaus, Beresford, Lydia Audrey, Beretta, Matteo Mario, Berge, David, Bergeaas Kuutmann, Elin, Berger, Nicolas, Bergmann, Benedikt Ludwig, Bergsten, Laura Jean, Beringer, Juerg, Berlendis, Simon, Bernardi, Gregorio, Bernius, Catrin, Bernlochner, Florian Urs, Berry, Tracey, Berta, Peter, Berthold, Anne-Sophie, Bertram, Iain, Bessidskaia Bylund, Olga, Besson, Nathalie, Bethke, Siegfried, Betti, Alessandra, Bevan, Adrian, Beyer, Julien-Christopher, Bhatta, Somadutta, Bhattacharya, Deb Sankar, Bhattarai, Prajita, Bhopatkar, Vallary Shashikant, Bi, Runyu, Bianchi, Riccardo Maria, Biebel, Otmar, Biedermann, Dustin, Bielski, Rafal, Bierwagen, Katharina, Biesuz, Nicolo Vladi, Biglietti, Michela, Billoud, T.R. V., Bindi, Marcello, Bingul, Ahmet, Bini, Cesare, Biondi, Silvia, Birch-Sykes, Callum Jacob, Birman, Mattias, Bisanz, Tobias, Biswal, Jyoti Prakash, Biswas, Diptaparna, Bitadze, Alexander, Bittrich, Carsten, Bjoerke, Kristian, Blazek, Tomas, Bloch, Ingo, Blocker, Craig, Blue, Andrew James, Blumenschein, Ulla, Blumenschein, Heidrun, Bobbink, Gerjan, Bobbink, Gerard, Bobrovnikov, Viktor, Bocchetta, Simona, Bogavac, Danijela, Bogdanchikov, Alexander, Bohm, Christian, Boisvert, Veronique, Bokan, Petar, Bold, Tomasz, Bolz, Arthur Eugen, Bomben, Marco, Bona, Marcella, Bonilla, Johan Sebastian, Boonekamp, Maarten, Booth, Callum Dale, Borbely, Albert Gyorgy, Borecka-Bielska, Hanna Maria, Borgna, Lucas Santiago, Borisov, Anatoli, Borissov, Guennadi, Bortoletto, Daniela, Boscherini, Davide, Fernandez-Bosman, Martine, Sola, J.D. Bossio, Bouaouda, Khalil, Boudreau, Joseph, Bouhova-Thacker, E.V., Bouhova-Thacker, Evelina Vassileva, Boumediene, Djamel Eddine, Boveia, Antonio, Boyd, Jamie, Boyd, James, Boye, Diallo, Boyko, Igor, Bozson, Adam, Bracinik, Juraj, Brahimi, Nihal, Brandt, Gerhard Immanuel, Brandt, Oleg, Braren, Frued Erik, Brau, Benjamin Paul, Brau, J.E., Brau, James Edward, Breaden Madden, Will, Breaden Madden, William Dmitri, Brendlinger, Kurt, Schimmel Brener, Roy, Brenner, Lydia, Brenner, Richard, Bressler, Shikma, Brickwedde, Bernard, Briglin, Daniel Lawrence, Britton, David, Britzger, Daniel Andreas, Brock, Ian, Brock, Raymond, Brooijmans, Gustaaf, Brooks, William King, Brost, Elizabeth, Bruckman de Renstrom, Pawel, Bruers, Ben, Bruncko, Dusan, Bruni, Alessia, Bruni, Graziano, Bruschi, Marco, Bruscino, Nello, Bryngemark, Lene Kristian, Buanes, Trygve, Buat, Quentin, Buchholz, Peter, Buckley, Andy, Budagov, Ioulian, Buckley, Andrew Gordon, Budagov, Yulian, Bugge, Magnar Kopangen, Bulekov, Oleg, Bullard, Brendon, Burch, Tyler James, Burdin, Sergey, Burgard, Carsten Daniel, Burger, Angela Maria, Burghgrave, Blake Oliver, Burr, Jon, Burr, Jonathan, Burton, Charles, Burzynski, Jackson Carl, Buescher, Volker, Buschmann, Eric, Bussey, Peter John, Butler, John Mark, Buttar, Craig, Butterworth, Jonathan, Butti, Pierfrancesco, Buttinger, Will, Buttinger, William, Buxo Vazquez, Carlos Josue, Buzatu, Adrian, Buzykaev, Alexey, Buzykaev, Aleksey, Cabras, Grazia, Cabrera Urban, Susana, Caforio, Davide, Cai, Huacheng, Cairo, Valentina, Cakir, Orhan, Calace, Noemi, Calafiura, Paolo, Calderini, Giovanni, Calfayan, Philippe, Callea, Giuseppe, Caloba, Luiz, Caltabiano, Alessandro, Calvente Lopez, Sergio, Calvet, David, Calvet, Samuel, Calvet, Thomas Philippe, Calvetti, Milene, Camacho Toro, Reina Coromoto, Camarda, Stefano, Camarero Munoz, Daniel, Camarri, Paolo, Camerlingo, Maria Teresa, Cameron, David, Camincher, Clement, Campana, Simone, Campanelli, Mario, Camplani, Alessandra, Canale, Vincenzo, Canesse, Auriane, Bret Cano, Marc, Cantero Garcia, Josu, Cao, Tingting, Cao, Yumeng, Garrido, M.D. M.Capeans, Capua, Marcella, Cardarelli, Roberto, Cardillo, Fabio, Carducci, Giovandomenico, Carli, Ina, Carli, Tancredi, Carlino, Giampaolo, Carlson, B.T., Carlson, Benjamin Taylor, Carlson, Evan Michael, Carminati, Leonardo, Carney, Rebecca, Caron, Sascha, Carquin Lopez, Edson, Carra, Sonia, Carratta, Giuseppe, Carter, J.W. S., Carter, Thomas Michael, Casado Lechuga, Pilar, Casha, Albert Francis, Castiglia, Emma Grace, Castillo, Florencia Luciana, Castillo Garcia, Lucia, Castillo Gimenez, Victoria, Castro, Nuno, Catinaccio, Andrea, Catmore, James, Cattai, Ariella, Cavaliere, Viviana, Cavasinni, Vincenzo, Celebi, Emre, Celli, Federico, Cerny, Karel, Santiago Cerqueira, Augusto, Cerri, Alex, Cerri, Alessandro, Cerrito, Lucio, Cerutti, Fabio, Cervelli, Alberto, Cetin, Serkant, Chadi, Zakaria, Chakraborty, Dhiman, Chan, Jay, Chan, Chen-Hsun, Chan, Terry Ws, Chan, Wing Sheung, Chan, Wai Yuen, Chapman, John Derek, Chargeishvili, Bakar, Charlton, Dave, Charlton, David, Charman, Thomas Paul, Chatterjee, Meghranjana, Chau, Chav Chhiv, Che, Siinn, Chekanov, Sergei, Chekulaev, Sergey, Chelkov, G.A., Chen, Boping, Chen, Cheng, Chen, Chunhui, Chen, Huirun, Chen, Hucheng, Chen, Jing, Chen, Jue, Chen, Jiayi, Chen, Shion, Chen, Shenjian, Chen, Xin, Chen, Ye, Chen, Yu-Heng, Cheng, Hok Chuen, Cheng, Huajie, Cheplakov, Alexander, Cheremushkina, Evgeniya, Cherkaoui El Moursli, Rajaa, Cheu, Elliott, Cheung, Kingman, Chevalerias, Thibault, Chevalier, Laurent, Chiarella, Vitaliano, Chiarelli, Giorgio, Chiodini, Gabriele, Chisholm, Andrew Stephen, Chitan, Adrian, Chiu, I-Huan, Chiu, Justin, Chiu, Y.H., Chizhov, Mihail, Choi, Kyungeon, Chomont, Arthur, Chou, Yuan-Tang, Chow, Edwin, Chow, Yun Sang, Christopher, Lawrence Davou, Chu, Ming Chung, Chu, Xiaotong, Chudoba, Jiri, Chwastowski, Janusz, Chytka, Ladislav, Cieri, Davide, Ciesla, Krzysztof, Cindro, Vladimir, Cioara, Irina Antonela, Ciocio, Alessandra, Cirotto, Francesco, Citron, Z.H., Citterio, Mauro, Ciubotaru, Dan Andrei, Ciungu, Bianca Monica, Clark, Allan, Clark, Philip, Clawson, Savannah, Clement, Christophe, Coadou, Yann, Cobal, Marina, Coccaro, Andrea, Cochran, James Herbert, Coelho Lopes de Sa, Rafael, Cohen, Hadar, Coimbra, A.E. C., Cole, Brian, Colijn, Auke-Pieter, Collot, Johann, Conde Muino, Patricia, Connell, Simon, Connelly, Ian Allan, Constantinescu, Serban, Conventi, Francesco, Cooper-Sarkar, A.M., Cormier, Felix, Cormier, Kyle James Read, Corpe, Louie Dartmoor, Corradi, Massimo, Corrigan, Eric Edward, Corriveau, Francois, Costa Mezquita, Maria Jose, Costanza, Francesco, Costanzo, Davide, Cowan, Glen, Cowley, James William, Crane, Jonathan, Cranmer, Kyle Stuart, Creager, Rachael Ann, Crepe-Renaudin, Sabine, Crescioli, Francesco, Cristinziani, Markus, Croft, Vincent Alexander, Crosetti, Giovanni, Dandoy, Jeffrey Rogers, Crosetti, Nanni, Cueto Gomez, Ana Rosario, Cuhadar Donszelmann, Tulay, Cui, Han, Cukierman, Aviv Ruben, Cunningham, William Reilly, Cunningham, Liam, Czekierda, Sabina Anna, Czodrowski, Patrick Karl, Czurylo, Marta Maja, da Cunha Sargedas de Sousa, M.J., da Fonseca Pinto, Joao Victor, da Via, Cinzia, Dabrowski, Wladyslaw, Dachs, Florian, Dado, Tomas, Dahbi, Salah-Eddine, Dai, Tiesheng, Dallapiccola, Carlo, Dam, Mogens, d'Amen, Gabriele, d'Amico, Valerio, Damp, Johannes Frederic, Dandoy, Jeff, Daneri, Maria Florencia, Danninger, Matthias, Dao, Valerio, Darbo, Giovanni, Darbo, Nanni, Dartsi, Olympia, Dattagupta, Aparajita, Daubney, Thomas, d'Auria, Saverio, David, Claire, Davidek, Tomas, Davis, Douglas Raymond, Dawson, Ian, De, Kaushik, de Asmundis, Riccardo, de Beurs, Marcus, de Castro, Stefano, de Groot, Nicolo, de Jong, Paul, de la Torre Perez, Hector, de Maria, Antonio, de Pedis, Daniele, de Salvo, Alessandro, de Sanctis, Umberto, de Santis, Maurizio, de Santo, Antonella, de Vivie de Regie, Jean-Baptiste, Dedovich, Dmitri, Deiana, Allison Mccarn, del Peso, Jose, Delabat Diaz, Yasiel, Delgove, David, Deliot, Frederic, Delitzsch, Chris Malena, Della Pietra, Massimo, Della Volpe, Domenico, Dell'Acqua, Andrea, Dell'Asta, Lidia, Delmastro, Marco, Delporte, Charles Eliaz, Delsart, Pierre Antoine, Demers Konezny, Sarah Marie, Demichev, Mikhail, Demontigny, Gabriel, Denisov, Serguei, d'Eramo, Louis, Derendarz, Dominik Karol, Derkaoui, Jamal, Derue, Frederic, Dervan, Paul, Desch, Klaus, Dette, Karola, Deutsch, Christopher, Devesa, Maria Roberta, Deviveiros, Pier-Olivier, Di Bello, Francesco Armando, Di Ciaccio, Anna, Di Ciaccio, Lucia, Di Clemente, William Kennedy, Di Clemente, Will, Di Donato, Camilla, Di Girolamo, Alessandro, Di Gregorio, Giulia, Di Luca, Andrea, Di Micco, Biagio, Di Nardo, Roberto, Di Petrillo, Karri Folan, Di Sipio, Riccardo, Diaconu, Cristinel, de Almeida Dias, Flavia, Vale, T.Dias Do, Diaz Gutierrez, Marco Aurelio, Diaz Capriles, Federico Guillermo, Dickinson, Jennet Elizabeth, Didenko, Mariia, Diehl, Edward, Dietrich, Janet, Diez Cornell, Sergio, Diez Pardos, Carmen, Dimitrievska, Aleksandra, Ding, Wei, Dingfelder, Jochen Christian, Dittmeier, Sebastian, Dittus, Fridolin, Dittus, Fido, Djama, Fares, Djobava, Tamar, Djuvsland, Julia Isabell, Barros Do Vale, Aline, Dobre, Monica, Dodsworth, David Michael, Doglioni, Caterina, Dolejsi, Jiri, Dolezal, Zdenek, Donadelli, Marisilvia, Dong, Binbin, Donini, Julien Noce, d'Onofrio, Adelina, d'Onofrio, Monica, Dopke, Jens, Doria, Alessandra, Dova, Maria Teresa, Doyle, Anthony Terence, Doyle, Tony, Drechsler, Eric, Dreyer, Etienne, Dreyer, Timo, Drobac, Alec Swenson, Du, Dongshuo, Du Pree, Tristan Arnoldus, Duan, Yanyun, Dubinin, Filipp, Dubovsky, Michal, Dubreuil, Arnaud, Duchovni, Ehud, Duckeck, Guenter, Ducu, Otilia Anamaria, Duda, Dominik, Dudarev, Alexey, Dudder, Andreas Christian, Duffield, Emily Marie, d'Uffizi, Matteo, Duflot, Laurent, Duehrssen-Debling, Michael, Dulsen, Carsten, Dumancic, Mirta, Dumitriu, Ana Elena, Dunford, Monica, Dungs, Sascha, Duperrin, Arnaud, Yildiz, H.Duran, Ellis, Nicolas, Yildiz, Duran, Dueren, Michael Johannes, Durglishvili, Archil, Duschinger, Dirk Uwe, Dutta, Baishali, Duvnjak, Damir, Dyckes, G.I., Dyndal, Mateusz, Dysch, Samuel Dezso, Dziedzic, Bartosz Sebastian, Eggleston, Michael Glenn, Eifert, Till, Eigen, Gerald, Einsweiler, Kevin Frank, Ekelof, Tord Johan Carl, El Jarrari, Hassnae, Ellajosyula, Venugopal, Ellert, Mattias, Ellinghaus, Frank, Elliot, Alison, Emerman, Alexander Zack, Evans, Harold, Ellis, Nick, Elmsheuser, Johannes, Elsing, Markus, Emeliyanov, Dmitry, Emerman, Alex, Enari, Yuji, Epland, Matthew, Erdmann, Johannes, Ereditato, Antonio, Erland, Paula Agnieszka, Errenst, Martin, Escalier, Marc, Escobar Ibanez, Carlos, Estrada Pastor, Oscar, Etzion, Erez, Gaspar de Andrade Evans, Guiomar, Evans, Hal, Evans, Meirin Oan, Ezhilov, Aleksei, Fabbri, Federica, Fabbri, Laura, Fabiani, Veronica, Facini, Gabriel, Fakhrutdinov, Rinat, Falciano, Speranza, Falke, Peter Johannes, Falke, Saskia, Faltova, Jana, Fang, Yi, Fang, Yaquan, Fanourakis, Georgios, Fanti, Marcello, Faraj, Mohammed, Farbin, Amir, Farilla, Addolorata, Fedorko, Wojciech Tadeusz, Fell, Alexandra, Farilla, Ada, Farina, Edoardo Maria, Farooque, Trisha, Farrington, Sinead, Farthouat, Philippe, Fassi, Farida, Fassnacht, Patrick, Fassouliotis, Dimitris, Faucci Giannelli, Michele, Fawcett, William James, Fayard, Louis, Fedin, Oleg, Fedorko, Wojtek, Fehr, Armin, Feickert, Matthew Carl, Feligioni, Lorenzo, Fell, Alix, Feng, Cunfeng, Feng, Minyu, Fenton, Michael James, Fenyuk, Alexandre, Ferguson, Sarah Whitney, Ferrando, James Edward, Ferrari, Arnaud, Ferrari, Pamela, Ferrari, Roberto, Ferreira de Lima, Danilo Enoque, Ferrer Soria, Antonio, Ferrere, Didier, Ferretti, Claudio, Fiedler, Frank, Filipcic, Andrej, Filthaut, Frank, Finelli, Kevin Daniel, Castro Nunes Fiolhais, Miguel, Fiorini, Luca, Fischer, Florian, Fischer, Julian, Fisher, Wade Cameron, Fitschen, Tobias, Fleck, Ivor, Fleischmann, Philipp, Flick, Tobias, Flierl, Bernhard Matthias, Flores, Lucas Macrorie, Flores Castillo, Luis Roberto, Follega, Francesco Maria, Fomin, Nikolai, Foo, Joel Hengwei, Forcolin, Giulio Tiziano, Forland, Blake Christopher, Formica, Andrea, Forster, Fabian Alexander, Forti, Alessandra, Fortin, Etienne Marie, Foti, Maria Giovanna, Fournier, Daniel, Fox, Harald, Francavilla, Paolo, Francescato, Simone, Franchini, Matteo, Franchino, Silvia, Francis, David, Franco, Luca, Franconi, Laura, Franklin, Melissa, Frattari, Guglielmo, Fray, Antony, Freeman, Patrick Moriishi, Freund, Benjamin, Spolidoro Freund, Werner, Freundlich, Elena Murielle, Frizzell, Dylan Cooper, Froidevaux, Daniel, Frost, James, Fujimoto, Minori, Fukunaga, Chikara, Fullana Torregrosa, Esteban, Fusayasu, Takahiro, Fuster Verdu, Juan, Gabrielli, Alessandro, Gabrielli, Andrea, Gadatsch, Stefan, Gadow, Paul Philipp, Gagliardi, Guido, Gagnon, Louis-Guillaume, Gallardo, Gabriel, Gallas, Elizabeth, Gallop, Bruce Joseph, Gamboa Goni, Rodrigo, Gan, Kock Kiam, Ganguly, Sanmay, Gao, Jun, Gao, Yanyan, Gao, Yongsheng, Garay Walls, Francisca, Garcia, Carmen, Garcia Navarro, Jose Enrique, Garcia Pascual, Juan Antonio, Garcia, Juanan, Garcia Argos, Carlos, Garcia-Sciveres, Maurice, Gardner, Robert William, Garelli, Nicoletta, Gargiulo, Simona, Garner, Christopher Andrew, Garonne, Vincent, Gasiorowski, Sean Joseph, Do Nascimento Gaspar, Philipp, Gaudiello, Andrea, Gaudio, Gabriella, Gauzzi, Paolo, Gavrilenko, Igor, Gavriliuk, Aleksandr, Gay, Colin Warren, Gaycken, Goetz, Gazis, Evangelos, Geanta, Andrei Alexandru, Gee, Carolyn, Gee, C.N. P., Geisen, Jannik, Geisen, Marc, Gemme, Claudia, Genest, Marie-Helene, Geng, Cong, Gentile, Simonetta, George, Simon, Geralis, Theodoros, Gerlach, Lino Oscar, Gessinger-Befurt, Paul, Gessner, Gregor, Ghasemi Bostanabad, Meisam, Ghneimat, Mazuza, Ghosh, Aishik, Ghosh, Anindya, Giacobbe, Benedetto, Giagu, Stefano, Giangiacomi, Nico, Giannetti, Paola, Giannini, Antonio, Giannini, Giulia, Gibson, Stephen, Gignac, Matthew, Gil, Damian Tomasz, Gilbert, Benjamin Jacob, Gillberg, Dag, Gilles, Geoffrey, Gillwald, N.E. K., Gingrich, Douglas, Giordani, Mario, Gingrich, Doug, Giordani, Mapo, Giraud, Pierre-Francois, Giugliarelli, Gilberto, Giugni, Danilo, Giuli, Francesco, Gkaitatzis, Stamatios, Gkialas, Ioannis, Gkougkousis, Evangelos Leonidas, Gkougkousis, Vagelis, Gkountoumis, Panagiotis, Gladilin, Leonid, Glasman, Claudia, Glatzer, Julian, Glaysher, P.C. F., Glazov, Alexander, Gledhill, Galen Rhodes, Gnesi, Ivan, Goblirsch-Kolb, Maximilian Emanuel, Godin, Dominique, Goldfarb, Steven, Golling, Tobias, Golubkov, Dmitry, da Silva Gomes, Agostinho, Goncalves Gama, Rafael, Morais Silva Goncalo, Ricardo Jose, Gonella, Giulia, Gonella, Laura, Gongadze, Alexi, Gonnella, Francesco, Gonski, Julia Lynne, Gonzalez de la Hoz, Santiago, Gonzalez Fernandez, Sergio, Gonzalez Lopez, Ricardo, Gonzalez Renteria, Cesar, Gonzalez Suarez, Rebeca, Gonzalez Sevilla, Sergio, Gonzalvo Rodriguez, Galo Rafael, Goossens, Luc, Gorasia, Nandish Arjan, Gorbounov, Petr, Gordon, Howard, Gorini, Benedetto, Gorini, Edoardo, Gorisek, Andrej, Goshaw, Alfred Thomas, Goshaw, A.T., Gostkin, Mikhail, Gottardo, Carlo Alberto, Gouighri, Mohamed, Goussiou, Anna, Govender, Nicolin, Goy, Corinne, Grabowska-Bold, Iwona, Graham, Emily Charlotte, Gramling, Johanna, Gramstad, Eirik, Grancagnolo, Sergio, Grandi, Mario, Grachev, Vadim, Gravila, Paul, Gravili, Francesco Giuseppe, Gray, Chloe, Gray, Heather, Grefe, Christian, Gregersen, Kristian Damlund, Gregor, Ingrid, Grenier, Philippe, Grevtsov, Kirill, Grieco, Chiara, Grieser, Nathan Allen, Grillo, Alex, Grimm, Kathryn, Grinstein, Sebastian, Grivaz, Jean-Francois, Groh, Sabrina, Gross, Eilam, Grosse-Knetter, Joern, Grout, Zara Jane, Grud, Christopher Ryan, Grummer, Aidan, Grundy, James Cameron, Guan, Liang, Guan, Wen, Gubbels, Christopher, Hance, Michael, Gubbels, Chris, Guenther, Jaroslav, Guerguichon, Antinea, Rojas, J.G. R.Guerrero, Guescini, Francesco, Guest, Daniel Hay, Guest, Dan, Gugel, Ralf, Guida, Alessandro, Guillemin, Thibault, Guindon, Stefan, Guo, Jun, Guo, Wen, Guo, Yicheng, Guo, Ziyu, Gupta, Ruchi, Gurbuz, Saime, Gustavino, Giuliano, Guth, Manuel, Gutierrez, Phillip, Gutschow, Christian, Guyot, Claude, Gwenlan, Claire, Gwilliam, Carl, Haaland, Even Simonsen, Haas, Andrew, Haber, Carl, Hadavand, Haleh, Hadef, Asma, Haleem, Mahsana, Haley, Joseph, Hall, Jack Joseph, Halladjian, Garabed, Hallewell, Gregory, Hamano, Kenji, Hamdaoui, Hassane, Hamer, Matthias, Hamity, Guillermo Nicolas, Han, Kunlin, Han, Liangliang, Han, Liang, Han, Shuo, Han, Yi Fei, Hanagaki, Kazunori, Hawkes, Christopher, Hays, Christopher Paul, Hance, Mike, Handl, David Michael, Hank, Michael Donald, Hankache, Robert, Hansen, Eva Brottmann, Hansen, Jorgen Beck, Hansen, Dines, Hansen, Maike Christina, Hansen, Peter, Hanson, Emily Claire, Hara, Kazuhiko, Harenberg, Torsten, Harkusha, Siarhei, Harrison, Paul Fraser, Hartman, Nicole Michelle, Hartmann, Nikolai, Hasegawa, Yoji, Hasib, Ahmed, Hassani, Samira, Haug, Sigve, Hauser, Reiner, Havranek, Miroslav, Hawkes, Chris, Hawkings, Richard, Hayashida, Shota, Hayden, Daniel, Hayes, Christopher Robyn, Hayes, Robin, Hays, Chris, Hays, Jonathan, Hayward, Helen, Haywood, Stephen, He, Fudong, He, Yunjian, Heath, Matthew Peter, Hedberg, Vincent, Heggelund, Andreas Lokken, Hehir, Natasha, Heidegger, Constantin, Heidegger, Kim Katrin, Heidorn, William Dale, Heilman, Jesse Alan, Heim, Sarah, Heim, Timon, Heinemann, Beate, Heinlein, James Geddy, Heinrich, Jochen Jens, Heinrich, Lukas Alexander, Hejbal, Jiri, Helary, Louis, Held, Alexander, Hellesund, Simen, Helling, Cole Michael, Hellman, Sten, Helsens, Clement, Henderson, R.C. W., Henkelmann, Lars, Henriques Correia, Ana Maria, Herde, Hannah Elizabeth, Hernandez Jimenez, Yesenia, Herr, Holger Arnold, Herrmann, Maximilian Georg, Herrmann, Tim, Herten, Gregor, Hertenberger, Ralf, Hervas, Luis, Herwig, Christian, Hesketh, Gavin, Hessey, Nigel, Hibi, Hiroaki, Higashino, Satoshi, Higon-Rodriguez, Emilio, Hildebrand, Kevin, Hill, John, Hill, Kurt Keys, Hiller, Karlheinz, Hillier, Stephen, Hils, Maximilian, Hinchliffe, Ian, Hinterkeuser, Florian, Hirose, Minoru, Hirose, Shigeki, Hirschbuehl, Dominic, Hiti, Bojan, Hladik, Ondrej, Hobbs, John David, Hobincu, Radu, Tal Hod, Noam, Hodgkinson, Mark, Hoecker, Andreas, Hohn, David, Hohov, Dmytro, Holm, Tanja, Holmes, Tova, Holzbock, Michael, Hommels, L.B. A.H., Hong, Tae Min, Honig, Jan Cedric, Honle, Andreas, Hooberman, Benjamin Henry, Hopkins, Walter, Horii, Yasuyuki, Horn, Philipp, Horyn, Lesya Anna, Hou, Suen, Hoummada, Abdeslam, Howarth, James William, Hoya, Joaquin, Hrabovsky, Miroslav, Hrivnac, Julius, Hrynevich, Aliaksei, Hrynova, Tetiana, Hsu, Pai-Hsien, Hsu, Shih-Chieh, Hu, Qipeng, Hu, Shuyang, Hu, Yifan, Huang, Danping, Huang, Xiaozhong, Huang, Yicong, Huang, Yanping, Hubacek, Zdenek, Hubaut, Fabrice, Hubner, Michael, Huegging, Fabian, Huffman, Todd Brian, Huhtinen, Mika, Hulsken, Raphael, Hunter, Robert Francis, Huseynov, Nazim, Huston, Joey, Huth, John, Hyneman, Rachel Jordan, Hyrych, Sofiia, Iacobucci, Giuseppe, Iakovidis, Georgios, Iakovidis, George, Ibragimov, Iskander, Iconomidou-Fayard, Lydia, Iengo, Paolo, Ignazzi, Rosanna, Iguchi, Ryunosuke, Iizawa, Tomoya, Ikegami, Yoichi, Ikeno, Masahiro, Ilic, Nikolina, Iltzsche, Franziska, Imam, Hajar, Introzzi, Gianluca, Iodice, Mauro, Iordanidou, Kalliopi, Ippolito, Valerio, Isacson, Max Fredrik, Ishino, Masaya, Islam, Wasikul, Issever, Cigdem, Istin, Serhat, Ponce, J.M. Iturbe, Iuppa, Roberto, Ivina, Anna, Izen, Joseph Michael, Izzo, Vincenzo, Jacka, Petr, Jackson, Paul, Jacobs, Ruth Magdalena, Jaeger, Benjamin Paul, Jain, Vivek, Jakel, Gunnar, Jakobi, Katharina Bianca, Jakobs, Karl, Jakoubek, Tomas, Jamieson, Jonathan, Janas, Krzysztof, Jansky, Roland, Janus, Michel, Janus, Piotr Andrzej, Jarlskog, Goran, Jaspan, Adam Elliott, Javadov, Namig, Javurek, Tomas, Javurkova, Martina, Jeanneau, Fabien, Jeanty, Laura, Jejelava, Juansher, Jenni, Peter, Jeong, Namgyun, Jezequel, Stephane, Jia, Jiangyong, Jia, Zihang, Jiang, Hai, Jiang, Yi, Jiang, Zihao, Jiggins, Stephen, Jimenez Morales, Fabricio Andres, Jimenez Pena, Javier, Jin, Shan, Jinaru, Adam, Jinnouchi, Osamu, Jivan, Harshna, Johansson, Per Daniel Conny, Johns, Kenneth, Johnson, Christian, Jones, Eleanor, Jones, R.W. L., Jones, Samuel David, Jones, Timothy John, Jones, T.J., Jovicevic, Jelena, Ju, Xiangyang, Junggeburth, Johannes Josef, Juste Rozas, Aurelio, Kaczmarska, Anna, Kado, Marumi, Kagan, Harris, Kagan, Michael Aaron, Kahn, Alan Mathew, Kahra, Christian, Kaji, Toshiaki, Kajomovitz Must, Enrique, Kalderon, Charles William, Kartvelishvili, Vakhtang, Kastanas, Konstantinos, Kalderon, Will, Kaluza, Adam, Kamenshchikov, Andrey, Kaneda, Michiru, Kang, Nathan Jihoon, Kang, Shuaiyan, Kano, Yuya, Kanzaki, Junichi, Kaplan, Laser Seymour, Kar, Deepak, Karava, Kla, Kareem, Mohammad, Karkanias, Ioannis, Karpov, Sergey, Karpova, Zoya, Kartvelishvili, Vato, Karyukhin, Andrei, Kasimi, Eirini, Kastanas, Alex, Kato, Chikuma, Katzy, Judith, Kawade, Kentaro, Kawagoe, Kiyotomo, Kawaguchi, Tomomi, Kawamoto, Tatsuo, Kawamura, Gen, Kay, Ellis, Kaya, Fikriye Idil, Kaya, Colette, Kazakos, Stergios, Kazanin, Vassili, Keaveney, James Michael, Keeler, Richard, Keller, John Stakely, Kellermann, Edgar, Kelsey, Daniel Christopher, Kempster, Jacob Julian, Kendrick, James Andrew, Kennedy, Kiley Elizabeth, Kepka, Oldrich, Kersten, Susanne, Kersevan, Borut Paul, Haghighat, S.Ketabchi, Khalil-Zada, Farhad, Khandoga, Mykola, Khanov, Alexander, Kharlamov, Alexey, Kharlamova, Tatyana, Khoda, Elham E, Khoo, Teng Jian, Khoriauli, Gia, Khramov, Evgeny, Khubua, J., Khubua, Djemal, Kido, Shogo, Kiehn, Moritz, Kim, Eunchong, Kim, Young-Kee, Kimura, Naoki, Kirchhoff, Andreas, Kirchmeier, David, Kirk, Julie, Kiryunin, Andrei, Kishimoto, Tomoe, Kisliuk, Dylan Perry, Kitali, Vincent, Kitsaki, Chara, Kivernyk, Oleh, Klapdor-Kleingrothaus, Thorwald, Klassen, Martin, Klein, Christoph Thomas, Klein, Matthew Henry, Klein, Max, Klein, Uta, Kleinknecht, Konrad, Klimek, Pawel Jan, Klimentov, Alexei, Klimpel, Fabian, Klingl, Tobias, Klioutchnikova, Tatiana, Klitzner, Felix Fidelio, Kluit, Peter, Kluth, Stefan, Kneringer, Emmerich, Knoops, E.B. F.G., Knue, Andrea Helen, Kobayashi, Dai, Kobel, Michael, Kocian, Martin, Kodama, Takafumi, Kodys, Peter, Koeck, D.M., Kock, Daniela, Konig, Philipp, Koffas, Thomas, Koehler, Nicolas, Kolb, Mathis, Koletsou, Iro, Komarek, Tomas, Kondo, Takahiko, Kordas, Konstantinos, Kondo, Taka, Koeneke, Karsten, Kong, A.X. Y., Konig, Adriaan Clemens, Kono, Takanori, Konstantinides, Vasilis, Konstantinidis, Nikolaos, Konya, Balazs, Kopeliansky, Revital, Koperny, Stefan Zenon, Korcyl, Krzysztof Marian, Kordas, Kostas, Koren, Guy, Korn, Andreas, Korolkov, Ilya, Korolkova, Elena, Korotkova, Natalia, Kortner, Oliver, Kortner, Sandra, Kostyukhin, Vadim, Kotsokechagia, Anastasia, Kotwal, Ashutosh, Koulouris, Aimilianos, Kourkoumeli-Charalampidi, Athina, Kourkoumelis, Christine, Kourlitis, Evangelos, Kouskoura, Vasiliki, Kowalewski, Robert Victor, Kowalewski, Bob, Kozanecki, Witold, Kozhin, Anatoli, Kramarenko, Viktor, Kramberger, Gregor, Krasnopevtsev, Dimitrii, Krasny, Mieczyslaw, Krasznahorkay, Attila, Krauss, Dominik, Kremer, Jakub, Kretzschmar, Jan, Kreul, Ken Matthias, Krieger, Peter, Krieter, Ferdinand, Krishnamurthy, Samyukta, Krishnan, Anjali, Krivos, Martin, Krizka, Karol, Kroeninger, Kevin Alexander, Kroha, Hubert, Kroll, Jiri, Kroll, Joseph Ira, Krowpman, Kyle Stuart, Kruchonak, Uladzimir, Krueger, Hans, Krumnack, Nils Erik, Kruse, Mark, Krzysiak, Janina Anna, Kubota, Arisa, Kuchinskaia, Olesia, Kuday, Sinan, Kuchler, Daniela, Kuechler, J.T., Kuehn, Susanne, Kuhl, Thorsten, Kukhtin, Victor, Kulchitsky, Y., Koultchitski, Iouri, Kuleshov, Sergey, Koultchitski, Yuri, Kuleshov, Serguei, Kulinich, Yakov Petrovich, Kuna, Marine, Kupco, Alexander, Kupfer, Tobias, Kuprash, Oleg, Kurashige, Hisaya, Kurchaninov, Leonid, Kurochkin, Yurii, Kurova, Anastasia, Kurth, Matthew Glenn, Kuwertz, Emma Sian, Kuze, Masahiro, Kvam, Audrey Katherine, Kvita, Jiri, Kwan, Tony, Lacasta Llacer, Carlos, Lacava, Francesco, Lack, David Philip John, Lacker, Heiko Markus, Lacour, Didier, Ladygin, Evgeny, Lai, Stanley Tsai-Ting, Ladygin, Evgueni, Lafaye, Remi, Laforge, Bertrand, Lagouri, Theodota, Lai, Stan, Lakomiec, Inga Katarzyna, Lambert, Joseph Earl, Lammers, Sabine Wedam, Lampl, Walter, Lampoudis, Christos, Lancon, Eric Christian, Landgraf, Ulrich, Landon, Murrough, Lang, Valerie, Lange, Joern, Langenberg, Robert Johannes, Lankford, Andrew James, Lanni, Francesco, Lantzsch, Kerstin, Lanza, Agostino, Lapertosa, Alessandro, Laporte, Jean-Francois, Lari, Tommaso, Lasagni Manghi, Federico, Lassnig, Mario, Latonova, Vera, Lau, Tak Shun, Laudrain, Antoine, Laurier, Alexandre, Lavorgna, Marco, Lawlor, Sean Dean, Lazzaroni, Massimo, Le, Brian, Le Guirriec, Emmanuel, Lebedev, Alexandre, Lecompte, T., Leblanc, Matthew Edgar, Le Compte, Thomas Joseph, Leblanc, Matt, Le Compte, Tom, Ledroit-Guillon, F., Lee, Ava Chloe Audrey, Lee, Claire, Lee, Graham Richard, Lee, Lawrence, Lee, Shih-Chang, Lee, Songkyo, Lefebvre, Benoit, Lefebvre, Helena, Lefebvre, Michel, Leggett, Charles, Lehmann, Konstantin, Lehmann, Niklaus, Lehmann Miotto, Giovanna, Leight, William Axel, Leisos, Antonios, Lisboa Leite, Marco, Leitgeb, Clara Elisabeth, Leitner, Rupert, Leney, Katharine, Lenz, Tatjana, Leone, Sandra, Leonidopoulos, Christos, Leopold, Alexander, Leroy, Claude, Les, Robert, Lester, Christopher, Levchenko, Mikhail, Leveque, Jessica, Levin, Daniel Sheldon, Lloyd, Stephen, Levin, Dan, Levinson, Lorne, Lewis, Daniel James, Li, Boyang, Li, Bing, Li, Changqiao, Li, Fan, Li, Heng, Li, Haifeng, Li, Jing, Li, Ke, Li, Liang, Li, Mengran, Li, Quanyin, Li, Shu, Li, Xingguo, Li, Yichen, Li, Zhi, Li, Zhiying, Li, Zhelun, Li, Zhiyuan, Liang, Zhijun, Liberatore, Marianna, Liberti, Barbara, Lie, Ki, Lim, Sanghoon, Lin, Chiao-Ying, Lin, Kuan-Yu, Linck, Rebecca, Lindley, Rachel Elizabeth, Lindon, Jack, Linss, Arthur, Lionti, Anthony, Lipeles, Elliot, Lipniacka, Anna, Liss, Anthony Michael, Lister, Alison, Little, Jared, Liu, Bo, Liu, Bingxuan, Liu, Hongbin, Liu, Jianbei, Liu, J.K. K., Liu, Kun, Liu, Minghui, Liu, Mingyi, Liu, Peilian, Liu, Xiaotian, Liu, Yi, Liu, Yang, Liu, Yanlin, Liu, Yanwen, Livan, Michele, Lleres, Annick, Llorente Merino, Javier, Luehring, Frederick, Lloyd, Steve, Lo, Cheuk Yee, Lobodzinska, Ewelina Maria, Loch, Peter, Loffredo, Salvatore, Lohse, Thomas, Lohwasser, Kristin, Lokajicek, Milos, Long, Jonathan, Long, Robin Eamonn, Longarini, Iacopo, Longo, Luigi, Lopez Paz, Ivan, Lopez Solis, Alvaro, Lorenz, Jeanette Miriam, Lorenzo Martinez, Narei, Lory, Alexander, Loesle, Alena, Lou, Xuanhong, Lou, Xinchou, Lounis, Abdenour, Love, Jeremy Robert, Love, Peter, Lozano Bahilo, Julio, Lu, Miaoran, Lu, Yun-Ju, Lubatti, Henry, Luci, Claudio, Lucio Alves, Fabio Lucio, Lucotte, Arnaud, Luehring, Fred, Luise, Ilaria, Luminari, Lamberto, Lund-Jensen, Bengt, Luongo, Nicholas, Lutz, Margaret Susan, Lynn, David, Lyons, Harry John, Lysak, Roman, Lytken, Else, Lyu, Feng, Lyubushkin, Vladimir, Lyubushkina, Tatiana, Ma, Hong, Ma, Lianliang, Ma, Yanhui, Donell, D.M. Mac, Macdonell, Danika Marina, Maccarrone, Giovanni, Macdonald, Calum Michael, Macdonald, Jack, Machado Miguens, Joana, Madar, Romain, Mader, Wolfgang, Madugoda Ralalage Don, Madhuranga, Madysa, Nico, Maeda, Junpei, Maeno, Tadashi, Maerker, Max, Magerl, Veronika, Magini, Nicolo, Magro, Jacopo, Mahon, Devin, Maidantchik, Carmen, Maio, Amelia, Maj, Klaudia, Majersky, Oliver, Majewski, Stephanie, Makida, Yasuhiro, Makovec, Nikola, Malaescu, Bogdan, Malecki, Pa., Malecki, Pawel, Maleev, Victor, Malek, Fairouz, Malito, Davide, Mallik, Usha, Malone, Claire, Maltezos, Stavros, Malyukov, Sergey, Mamuzic, Judita, Mancini, Giada, Mandalia, Jesal, Mandic, Igor, Manhaes de Andrade Filho, Luciano, Maniatis, Ioannis Michail, Ramos, J.Manjarres, Mankinen, Katja Hannele, Mann, Alexander, Manousos, Athanasios, Marshall, Zachary Louis, Martin, Timothy, Maslennikov, Aleksei, Mcfayden, Joshua Angus, Manousos, Thanos, Mansoulie, Bruno, Manthos, Ioannis, Manzoni, Stefano, Marantis, Alexandros, Marceca, Gino, Marchese, Luigi, Marchiori, Giovanni, Marcisovsky, Michal, Marcoccia, Lorenzo, Marcon, Caterina, Marjanovic, Marija, Mc Kay, Madalyn Ann, Mcpherson, Robert Anthony, Marshall, Zach, Martensson, M.U. F., Marti I Garcia, Salvador, Martin, Christopher Blake, Martin, Tim, Martin, Victoria, Martin Dit Latour, Bertrand, Martinelli, Luca, Martinez-Perez, Mario, Martinez Agullo, Pablo, Martinez Outschoorn, Verena Ingrid, Martin-Haugh, Stewart, Martoiu, Sorin, Martyniuk, Alex Christopher, Marzin, Antoine, Maschek, Stefan Raimund, Masetti, Lucia, Mashimo, Tetsuro, Mashinistov, Ruslan, Masik, Jiri, Maslennikov, Alexei, Massa, Lorenzo, Massarotti, Paolo, Mastrandrea, Paolo, Mastroberardino, Anna, Masubuchi, Tatsuya, Matakias, Dimitrios, Matic, Andrea, Matsuzawa, Nobuo, Mattig, Peter, Maurer, Julien, Macek, Bostjan, Maximov, Dmitriy, Mazini, Rachid, Maznas, Ioannis, Mazza, Simone Michele, Mc Gowan, John Patrick, Mc Kee, Shawn, Mccarthy, Thomas, Mccormack, William Patrick, Mcdonald, Emily Frances, Mcdonald, Millie, Mcdougall, Ashley Ellen, Mcfayden, Josh, Mchedlidze, Gvantsa, Mc Kay, Maddie, Mclean, Kayla, Mcmahon, Stephen, Mcnamara, Peter Charles, Mcnicol, Christopher John, Mcpherson, R.A., Mdhluli, Joyful Elma, Meadows, Zachary Alden, Meehan, Samuel Ross, Megy, Theo, Mehlhase, Sascha, Mehta, Andrew, Meirose, Bernhard, Melini, Davide, Mellado Garcia, Bruce, Mellenthin, Johannes, Melo, Matej, Meloni, Federico, Melzer, Alexander, Gouveia, E.D. Mendes, Mendes Jacques da Costa, Antonio Manuel, Meng, Huan Yu, Meng, Lingxin, Meng, Xiangting, Menke, Sven, Meoni, Evelin, Mergelmeyer, Sebastian, Merkt, Sebastian Andreas, Merlassino, Claudia, Mermod, Philippe, Merola, Leonardo, Meroni, Chiara, Merz, Garrett William, Meshkov, Oleg, Meshreki, John Kamal Rizk, Metcalfe, Jessica, Mete, Alaettin Serhan, Meyer, Christopher John, Meyer, Jean-Pierre, Michetti, Michele, Middleton, Robin, Mijovic, Liza, Mikenberg, George, Mikestikova, Marcela, Mikuz, Marko, Mildner, Hannes, Milic, Adriana, Milke, Christopher Don, Milke, Chris, Miller, David, Miller, Laura Stephanie, Milov, Alexander, Milstead, David Anthony, Minaenko, Andrei, Minashvili, Irakli, Mince, Laurynas, Mincer, Allen Irving, Mindur, Bartosz, Mineev, Mikhail, Minegishi, Yuji, Mino, Yuya, Mir Martinez, Lluisa Maria, Mironova, Maria, Mistry, Khilesh Pradip, Mitani, Takashi, Mitrevski, Jovan, Mitsou, Vasiliki, Mittal, Monika, Miu, Ovidiu, Miucci, Antonio, Miyagawa, Paul, Mizukami, Atsushi, Mjoernmark, Jan-Ulf, Mkrtchyan, Tigran, Mlynarikova, Michaela, Moa, Torbjorn, Mobius, Silke, Mochizuki, Kazuya, Moder, Paul, Mogg, Philipp, Mohapatra, Soumya, Moles Valls, Regina, Monig, Klaus, Monnier, Emmanuel, Montalbano, Alyssa Rae, Montejo Berlingen, Javier, Montella, Marco, Monticelli, Fernando, Monzani, Simone, Morange, Nicolas, Moreira de Carvalho, Ana Luisa, Moreno Lopez, Deywis, Moreno Llacer, Maria, Moreno Martinez, Carlos, Morettini, Paolo, Morgenstern, Marcus Matthias, Morgenstern, Stefanie, Mori, Daniel, Morii, Masahiro, Morinaga, Masahiro, Morisbak, Vanja, Morley, Anthony, Mornacchi, Giuseppe, Morris, Alice, Morvaj, Ljiljana, Moschovakos, Paraschos, Myers, Gregory William, Nachman, Benjamin Philip, Moschovakos, Paris, Moser, Brian, Mosidze, Maia, Moskalets, Tetiana, Moskvitina, Polina, Moss, Joshua, Moyse, E.J. W., Muanza, Steve, Mueller, James Alfred, Muller, Ralph, Muenstermann, Daniel, Mullier, Geoffrey, Mungo, Davide Pietro, Munoz Martinez, Jose Luis, Munoz Sanchez, Francisca, Murin, Pavel, Murray, William John, Murray, Bill, Murrone, Alessia, Muse, Joseph M, Muskinja, Miha, Mwewa, Chilufya, Myagkov, Alexei, Myers, Ava Anne, Neep, Thomas James, Ntekas, Konstantinos, Myers, Greg, Myers, John, Myska, Miroslav, Nachman, B.P., Nackenhorst, Olaf, Nag, Abhishek, Nagai, Koichi, Nagano, Kunihiro, Nagasaka, Yasushi, Nagle, James Lawrence, Nagy, Elemer, Nairz, Armin, Higuchi, Yu Nakahama, Nakamura, Koji, Nakamura, Tomoaki, Nanjo, Hajime, Napolitano, Fabrizio, Garcia, R.F. Naranjo, Narayan, Rohin Thampilali, Naryshkin, Iurii, Naseri, Mohsen, Naumann, Thomas, Navarro, Gabriela Alejandra, Nechaeva, Polina, Nechansky, Filip, Ng, Yan Wing, Neep, T.J., Negri, Andrea, Negrini, Matteo, Nellist, Clara, Nelson, Christina, Nelson, Michael Edward, Nemecek, Stanislav, Nessi, Marzio, Neubauer, Mark, Neuhaus, Friedemann, Neumann, Manuel, Newhouse, Robin, Newman, Paul Richard, Ng, Chi Wing, Nikolaidou, Rodanthi, Nilsson, Paal Nils Bertil, Ng, Sam Yanwing, Ng, Ying Wun Yvonne, Ngair, Badr-Eddine, Nguyen, Hoang Dai Nghia, Nguyen Manh, Tuan, Nibigira, Emery, Nickerson, Richard, Nikolaidou, Rosy, Nielsen, Daniel, Nielsen, Jason, Niemeyer, Marcel, Nikiforou, Nikiforos, Nikolaenko, Vladimir, Nikolic-Audit, I., Nikolopoulos, Konstantinos, Nilsson, Paul, Nindhito, Herjuno Rah, Nisati, Aleandro, Nishu, Nishu, Nisius, Richard, Nitsche, Isabel, Nitta, Tatsumi, Nobe, Takuya, Noel, Daniel Louis, Noguchi, Yohei, Nomidis, Ioannis, Nomura, Marcelo Ayumu, Nordberg, Markus, Novak, Jakob, Novak, Tadej, Novgorodova, Olga, Novotny, Radek, Nozka, Libor, Ntekas, Kostas, Nurse, Emily Laura, Oakham, Gerald, Ocariz, Jose Humberto, Ochi, Atsuhiko, Ochoa, Ines, Ochoa, Jean-Pierre, O'Connor, Kelsey Shea, Oda, Susumu, Odaka, Shigeru, Ordek, Serhat, Ogrodnik, Agnieszka Ewa, Oh, Alexander, Ohm, Christian, Oide, Hideyuki, Oishi, Reiyo, Ojeda, Martina Laura, Okawa, Hideki, Okazaki, Yuta, O'Keefe, Michael William, Okumura, Yasuyuki, Olariu, Albert, Seabra, L.F. Oleiro, Olivares, Sebastian, Oliveira Damazio, Denis, Oliver, Jason, Olsson, Mats Joakim Robert, Olszewski, Andrzej, Olszowska, Jolanta, Oncel, Omer Ogul, O'Neil, Dugan, O'Neill, Aaron Paul, Onofre, Antonio, Onyisi, P.U. E., Oppen, Henrik, Oreamuno Madriz, Rafael Guillermo, Oreglia, Mark, Orellana, Gonzalo Enrique, Orestano, Domizia, Orlando, Nicola, Orr, Robert, O'Shea, Valentine, Ouellette, Jeffrey Cortlandt, Parker, Andrew Michael, O'Shea, Val, Ospanov, Rustem, Otero y Garzon, Gustavo, Otono, Hidetoshi, Ott, Philipp Sebastian, Ottino, Gregory James, Ouchrif, Mohamed, Ouellette, Jeff, Ould-Saada, Farid, Ouraou, Ahmimed, Ouyang, Qun, Owen, Mark Andrew, Owen, Rhys, Ozcan, Erkcan, Ozturk, Nurcan, Pacalt, Josef, Pacey, Holly, Pachal, Katherine, Pacheco Pages, Andreu, Padilla Aranda, Cristobal, Pagan Griso, Simone, Palacino, Gabriel, Palazzo, Serena, Palestini, Sandro, Palka, Marek, Palni, Prabhakar, Pandini, Carlo Enrico, Panduro Vazquez, Jose Guillermo, Panduro Vazquez, William, Pani, Priscilla, Panizzo, Giancarlo, Paolozzi, Lorenzo, Papadatos, Constantine, Papageorgiou, Konstantinos, Parajuli, Santosh, Paramonov, Alexander, Paraskevopoulos, Christos, Paredes Hernandez, Daniela Katherinne, Paredes Saenz, Santiago Rafael, Parida, Bibhuti, Park, Tae Hyoun, Parker, Adam Jackson, Pollard, Christopher Samuel, Parker, Andy, Parodi, Fabrizio, Parrish, Elliot, Parsons, John, Parzefall, Ulrich, Pascual Dominguez, Luis, Pascuzzi, Vincent, Pasner, Jacob Martin, Pasquali, Federica, Pasqualucci, Enrico, Passaggio, Stefano, Pastore, Francesca, Pasuwan, Patrawan, Pataraia, Sophio, Pater, Joleen, Pater, Jo, Pathak, Atanu, Patton, Joseph, Pauly, Thilo, Pearkes, Jannicke Andree, Pedersen, Maiken, Pedraza Diaz, Lucia, Costa Batalha Pedro, Rute, Peiffer, Thomas, Peleganchuk, Sergey, Penc, Ondrej, Peng, Chen, Peng, Haiping, Sotto-Maior Peralva, Bernardo, Perego, Marta Maria, Pereira Peixoto, A.P., Pereira Sanchez, Laura, Perepelitsa, Dennis, Perez Codina, Estel, Perini, Laura, Pernegger, Heinz, Perrella, Sabrina, Perrevoort, Ann-Kathrin, Peters, Krisztian, Peters, Reinhild, Petersen, Brian, Petersen, Troels, Petit, Elisabeth, Petousis, Vlasios, Petridou, Chariclia, Petrucci, Fabrizio, Pettee, 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L., Lasagni Manghi , F, Massa , L., Vittori , C., Alfonsi , F, Cabras , G., Cervelli , A., Negrini , M., Todome , K., Carratta , G., Cavalli , N., Clissa , L., ATLAS collaboration, Centre de Physique des Particules de Marseille (CPPM), Aix Marseille Université (AMU)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS), Laboratoire d'Annecy de Physique des Particules (LAPP), Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Université Savoie Mont Blanc (USMB [Université de Savoie] [Université de Chambéry])-Centre National de la Recherche Scientifique (CNRS), Laboratoire de Physique des 2 Infinis Irène Joliot-Curie (IJCLab), Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Université Paris-Saclay-Centre National de la Recherche Scientifique (CNRS), Laboratoire de Physique de Clermont (LPC), Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS)-Université Clermont Auvergne (UCA), Institut de Recherches sur les lois Fondamentales de l'Univers (IRFU), Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Université Paris-Saclay, Laboratoire de Physique Nucléaire et de Hautes Énergies (LPNHE (UMR_7585)), Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Sorbonne Université (SU)-Centre National de la Recherche Scientifique (CNRS)-Université de Paris (UP), Laboratoire de Physique Subatomique et de Cosmologie (LPSC), Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS)-Université Grenoble Alpes (UGA)-Institut polytechnique de Grenoble - Grenoble Institute of Technology (Grenoble INP ), Université Grenoble Alpes (UGA), Centre de Calcul de l'IN2P3 (CC-IN2P3), Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS), ATLAS, Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Sorbonne Université (SU)-Centre National de la Recherche Scientifique (CNRS), Aad, G. 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W., Shaked Renous, D., Shan, L. Y., Shapiro, M., Sharma, A., Sharma, A. S., Shatalov, P. B., Shaw, K., Shaw, S. M., Shehade, M., Shen, Y., Sherman, A. D., Sherwood, P., Shi, L., Shimmin, C. O., Shimogama, Y., Shimojima, M., Shinner, J. D., Shipsey, I. P. J., Shirabe, S., Shiyakova, M., Shlomi, J., Shmeleva, A., Shochet, M. J., Shojaii, J., Shope, D. R., Shrestha, S., Shrif, E. M., Shroff, M. J., Shulga, E., Sicho, P., Sickles, A. M., Sideras Haddad, E., Sidiropoulou, O., Sidoti, A., Siegert, F., Sijacki, Dj., Silva, M., Silva Oliveira, M. V., Silverstein, S. B., Simion, S., Simoniello, R., Simpson-allsop, C. J., Simsek, S., Sinervo, P., Sinetckii, V., Singh, S., Sioli, M., Siral, I., Sivoklokov, S. Yu., Sjölin, J., Skaf, A., Skorda, E., Skubic, P., Slawinska, M., Sliwa, K., Smakhtin, V., Smart, B. H., Smiesko, J., Smirnov, N., Smirnov, S. Yu., Smirnov, Y., Smirnova, L. N., Smirnova, O., Smith, E. A., Smith, H. A., Smizanska, M., Smolek, K., Smykiewicz, A., Snesarev, A. A., Snoek, H. L., Snyder, I. M., Snyder, S., Sobie, R., Soffer, A., Søgaard, A., Sohns, F., Solans Sanchez, C. A., Soldatov, E. Yu., Soldevila, U., Solodkov, A. A., Soloshenko, A., Solovyanov, O. V., Solovyev, V., Sommer, P., Son, H., Sonay, A., Song, W., Song, W. Y., Sopczak, A., Sopio, A. L., Sopkova, F., Sottocornola, S., Soualah, R., Soukharev, A. M., South, D., Spagnolo, S., Spalla, M., Spangenberg, M., Spanò, F., Sperlich, D., Spieker, T. M., Spigo, G., Spina, M., Spiteri, D. P., Spousta, M., Stabile, A., Stamas, B. L., Stamen, R., Stamenkovic, M., Stampekis, A., Stanecka, E., Stanislaus, B., Stanitzki, M. M., Stankaityte, M., Stapf, B., Starchenko, E. A., Stark, G. H., Stark, J., Staroba, P., Starovoitov, P., Stärz, S., Staszewski, R., Stavropoulos, G., Stegler, M., Steinberg, P., Steinhebel, A. L., Stelzer, B., Stelzer, H. J., Stelzer-Chilton, O., Stenzel, H., Stevenson, T. J., Stewart, G. A., Stockton, M. C., Stoicea, G., Stolarski, M., Stonjek, S., Straessner, A., Strandberg, J., Strandberg, S., Strauss, M., Strebler, T., Strizenec, P., Ströhmer, R., Strom, D. M., Stroynowski, R., Strubig, A., Stucci, S. A., Stugu, B., Stupak, J., Styles, N. A., Su, D., Su, W., Su, X., Suarez, N. B., Sulin, V. V., Sullivan, M. J., Sultan, D. M. S., Sultansoy, S., Sumida, T., Sun, S., Sun, X., Suster, C. J. E., Sutton, M. R., Suzuki, S., Svatos, M., Swiatlowski, M., Swift, S. P., Swirski, T., Sydorenko, A., Sykora, I., Sykora, M., Sykora, T., Ta, D., Tackmann, K., Taenzer, J., Taffard, A., Tafirout, R., Tagiev, E., Taibah, R. H. M., Takashima, R., Takeda, K., Takeshita, T., Takeva, E. P., Takubo, Y., Talby, M., Talyshev, A. A., Tam, K. C., Tamir, N. M., Tanaka, J., Tanaka, R., Tapia Araya, S., Tapprogge, S., Tarek Abouelfadl Mohamed, A., Tarem, S., Tariq, K., Tarna, G., Tartarelli, G. F., Tas, P., Tasevsky, M., Tassi, E., Tateno, G., Tavares Delgado, A., Tayalati, Y., Taylor, A. J., Taylor, G. N., Taylor, W., Teagle, H., Tee, A. S., Teixeira De Lima, R., Teixeira-Dias, P., Ten Kate, H., Teoh, J. J., Terashi, K., Terron, J., Terzo, S., Testa, M., Teuscher, R. J., Thais, S. J., Themistokleous, N., Theveneaux-Pelzer, T., Thomas, D. W., Thomas, J. P., Thompson, E. A., Thompson, P. D., Thomson, E., Thorpe, E. J., Tikhomirov, V. O., Tikhonov, Yu. A., Timoshenko, S., Tipton, P., Tisserant, S., Todome, K., Todorova-Nova, S., Todt, S., Tojo, J., Tokár, S., Tokushuku, K., Tolley, E., Tombs, R., Tomiwa, K. G., Tomoto, M., Tompkins, L., Tornambe, P., Torrence, E., Torres, H., Torró Pastor, E., Toscani, M., Tosciri, C., Toth, J., Tovey, D. R., Traeet, A., Treado, C. J., Trefzger, T., Tresoldi, F., Tricoli, A., Trigger, I. M., Trincaz-Duvoid, S., Trischuk, D. A., Trischuk, W., Trocmé, B., Trofymov, A., Troncon, C., Trovato, F., Truong, L., Trzebinski, M., Trzupek, A., Tsai, F., Tseng, J. C. -L., Tsiareshka, P. V., Tsirigotis, A., Tsiskaridze, V., Tskhadadze, E. G., Tsopoulou, M., Tsukerman, I. I., Tsulaia, V., Tsuno, S., Tsybychev, D., Tu, Y., Tudorache, A., Tudorache, V., Tuna, A. N., Turchikhin, S., Turgeman, D., Turk Cakir, I., Turner, R. J., Turra, R., Tuts, P. M., Tzamarias, S., Tzovara, E., Uchida, K., Ukegawa, F., Unal, G., Unal, M., Undrus, A., Unel, G., Ungaro, F. C., Unno, Y., Uno, K., Urban, J., Urquijo, P., Usai, G., Uysal, Z., Vacek, V., Vachon, B., Vadla, K. O. H., Vafeiadis, T., Vaidya, A., Valderanis, C., Valdes Santurio, E., Valente, M., Valentinetti, S., Valero, A., Valéry, L., Vallance, R. A., Vallier, A., Valls Ferrer, J. A., Van Daalen, T. R., Van Gemmeren, P., Van Stroud, S., Van Vulpen, I., Vanadia, M., Vandelli, W., Vandenbroucke, M., Vandewall, E. R., Vannicola, D., Vari, R., Varnes, E. W., Varni, C., Varol, T., Varouchas, D., Varvell, K. E., Vasile, M. E., Vasquez, G. A., Vazeille, F., Vazquez Furelos, D., Vazquez Schroeder, T., Veatch, J., Vecchio, V., Veen, M. J., Veloce, L. M., Veloso, F., Veneziano, S., Ventura, A., Verbytskyi, A., Vercesi, V., Verducci, M., Vergel Infante, C. M., Vergis, C., Verkerke, W., Vermeulen, A. T., Vermeulen, J. C., Vernieri, C., Verschuuren, P. J., Vetterli, M. C., Viaux Maira, N., Vickey, T., Vickey Boeriu, O. E., Viehhauser, G. H. A., Vigani, L., Villa, M., Villaplana Perez, M., Villhauer, E. M., Vilucchi, E., Vincter, M. G., Virdee, G. S., Vishwakarma, A., Vittori, C., Vivarelli, I., Vogel, M., Vokac, P., Von Ahnen, J., von Buddenbrock, S. E., Von Toerne, E., Vorobel, V., Vorobev, K., Vos, M., Vossebeld, J. H., Vozak, M., Vranjes, N., Vranjes Milosavljevic, M., Vrba, V., Vreeswijk, M., Vu, N. K., Vuillermet, R., Vukotic, I., Wada, S., Wagner, P., Wagner, W., Wagner-Kuhr, J., Wahdan, S., Wahlberg, H., Wakasa, R., Walbrecht, V. M., Walder, J., Walker, R., Walker, S. D., Walkowiak, W., Wallangen, V., Wang, A. M., Wang, A. Z., Wang, C., Wang, H., Wang, J., Wang, P., Wang, Q., Wang, R. -J., Wang, R., Wang, S. M., Wang, W. T., Wang, W., Wang, W. X., Wang, Y., Wang, Z., Wanotayaroj, C., Warburton, A., Ward, C. P., Ward, R. J., Warrack, N., Watson, A. T., Watson, M. F., Watts, G., Waugh, B. M., Webb, A. F., Weber, C., Weber, M. S., Weber, S. A., Weber, S. M., Wei, Y., Weidberg, A. R., Weingarten, J., Weirich, M., Weiser, C., Wells, P. S., Wenaus, T., Wendland, B., Wengler, T., Wenig, S., Wermes, N., Wessels, M., Weston, T. D., Whalen, K., Wharton, A. M., White, A. S., White, A., White, M. J., Whiteson, D., Whitmore, B. W., Wiedenmann, W., Wiel, C., Wielers, M., Wieseotte, N., Wiglesworth, C., Wiik-Fuchs, L. A. M., Wilkens, H. G., Wilkins, L. J., Williams, D. M., Williams, H. H., Williams, S., Willocq, S., Windischhofer, P. J., Wingerter-Seez, I., Winkels, E., Winklmeier, F., Winter, B. T., Wittgen, M., Wobisch, M., Wolf, A., Wölker, R., Wollrath, J., Wolter, M. W., Wolters, H., Wong, V. W. S., Wongel, A. F., Woods, N. L., Worm, S. D., Wosiek, B. K., Woźniak, K. W., Wraight, K., Wu, S. L., Wu, X., Wu, Y., Wuerzinger, J., Wyatt, T. R., Wynne, B. M., Xella, S., Xiang, J., Xiao, X., Xie, X., Xiotidis, I., Xu, D., Xu, H., Xu, L., Xu, R., Xu, T., Xu, W., Xu, Y., Xu, Z., Yabsley, B., Yacoob, S., Yallup, D. P., Yamaguchi, N., Yamaguchi, Y., Yamamoto, A., Yamatani, M., Yamazaki, T., Yamazaki, Y., Yan, J., Yan, Z., Yang, H. J., Yang, H. T., Yang, S., Yang, T., Yang, X., Yang, Y., Yang, Z., Yao, W-M., Yap, Y. C., Ye, H., Ye, J., Ye, S., Yeletskikh, I., Yexley, M. R., Yigitbasi, E., Yin, P., Yorita, K., Yoshihara, K., Young, C. J. S., Young, C., Yu, J., Yuan, R., Yue, X., Zaazoua, M., Zabinski, B., Zacharis, G., Zaffaroni, E., Zahreddine, J., Zaitsev, A. M., Zakareishvili, T., Zakharchuk, N., Zambito, S., Zanzi, D., Zeißner, S. V., Zeitnitz, C., Zemaityte, G., Zeng, J. C., Zenin, O., Ženiš, T., Zerwas, D., Zgubič, M., Zhang, B., Zhang, D. F., Zhang, G., Zhang, J., Zhang, K., Zhang, L., Zhang, M., Zhang, R., Zhang, S., Zhang, X., Zhang, Y., Zhang, Z., Zhao, P., Zhao, Y., Zhao, Z., Zhemchugov, A., Zheng, Z., Zhong, D., Zhou, B., Zhou, C., Zhou, H., Zhou, M., Zhou, N., Zhou, Y., Zhu, C. G., Zhu, C., Zhu, H. L., Zhu, H., Zhu, J., Zhu, Y., Zhuang, X., Zhukov, K., Zhulanov, V., Zieminska, D., Zimine, N. I., Zimmermann, S., Zinonos, Z., Ziolkowski, M., Živković, L., Zobernig, G., Zoccoli, A., Zoch, K., Zorbas, T. G., Zou, R., Zwalinski, L., Aloisio, Alberto, Alviggi, Mariagrazia, Canale, Vincenzo, Della Pietra, Massimo, Merola, Leonardo, Massarotti, Paolo, Conventi, Francesco, Rossi, Elvira, Carlino, Giampaolo, de Asmundis, Riccardo, Di Donato, Camilla, Doria, Alessandra, Iengo, Paolo, Izzo, Vincenzo, Perrella, Sabrina, Sekhniaidze, Givi, Cirotto, Francesco, Lavorgna, Marco, Giannini, Antonio, Atlas, Collaboration, and Współautorami artykułu są członkowie ATLAS Collaboration w liczbie 2936
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electron ,Top quark ,Kjerne- og elementærpartikkelfysikk: 431 [VDP] ,Physics and Astronomy (miscellaneous) ,13000 GeV-cms ,measured [channel cross section] ,Parton ,pair production [top] ,7. Clean energy ,01 natural sciences ,High Energy Physics - Experiment ,Subatomär fysik ,High Energy Physics - Experiment (hep-ex) ,Subatomic Physics ,scattering [p p] ,[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex] ,parton ,associated production [Z0] ,Nuclear Experiment ,Settore FIS/01 ,Physics ,Luminosity (scattering theory) ,Large Hadron Collider ,4. Education ,ATLAS ,16. Peace & justice ,Nuclear and elementary particle physics: 431 [VDP] ,CERN LHC Coll ,medicine.anatomical_structure ,kinematics ,colliding beams [p p] ,top: pair production ,channel cross section: measured ,Particle Physics - Experiment ,data analysis method ,p p: scattering ,Particle physics ,Z boson ,CERN Lab ,Regular Article - Experimental Physics ,530 Physics ,FOS: Physical sciences ,LHC, ATLAS, High Energy Physics ,differential cross section: measured ,Cross section (physics) ,Atlas (anatomy) ,measured [differential cross section] ,muon ,0103 physical sciences ,medicine ,ddc:530 ,High Energy Physics ,010306 general physics ,Engineering (miscellaneous) ,top quark ,Muon ,hep-ex ,010308 nuclear & particles physics ,High Energy Physics::Phenomenology ,Física ,leptonic decay [Z0] ,Z0: associated production ,Z0: leptonic decay ,LHC, Particle Physics, Top physics ,High Energy Physics::Experiment ,Hadron-hadron collisions ,p p: colliding beams ,experimental results ,Lepton - Abstract
We thank CERN for the very successful operation of the LHC, as well as the support staff from our institutions without whom ATLAS could not be operated efficiently. We acknowledge the support of ANPCyT, Argentina; YerPhI, Armenia; ARC, Au CNPq and FAPESP, Brazil; NSERC, NRC and CFI, Canada; CERN; ANIstralia; BMWFW and FWF, Austria; ANAXS, Azerbaijan; SSTC, Belarus;D, Chile; CAS, MOST and NSFC, China; Minciencias, Colombia; MSMT CR, MPO CR and VSC CR, Czech Republic; DNRF and DNSRC, Denmark; IN2P3-CNRS and CEA-DRF/IRFU, France; SRNSFG, Georgia; BMBF, HGF and MPG, Germany; GSRT, Greece; RGC and Hong Kong SAR, China; ISF and Benoziyo Center, Israel; INFN, Italy; MEXT and JSPS, Japan; CNRST, Morocco; NWO, Netherlands; RCN, Norway; MNiSW and NCN, Poland; FCT, Portugal; MNE/IFA, Romania; JINR; MESofRussia andNRCKI, Russian Federation; MESTD, Serbia; MSSR, Slovakia; ARRS and MIZS, Slovenia; DST/NRF, South Africa; MICINN, Spain; SRC and Wallenberg Foundation, Sweden; SERI, SNSF and Cantons of Bern and Geneva, Switzerland; MOST, Taiwan; TAEK, Turkey; STFC, United Kingdom; DOEandNSF, USA. In addition, individual groups andmembers have received support fromBCKDF, CANARIE, ComputeCanada, CRC and IVADO, Canada; Beijing Municipal Science & Technology Commission, China; COST, ERC, ERDF, Horizon 2020 and Marie Sklodowska-Curie Actions, European Union; Investissements d'Avenir Labex, Investissements d'Avenir Idex and ANR, France; DFG and AvH Foundation, Germany; Herakleitos, Thales and Aristeia programmes co-financed by EU-ESF and the Greek NSRF, Greece; BSF-NSF and GIF, Israel; La Caixa Banking Foundation, CERCA Programme Generalitat de Catalunya and PROMETEO and GenT Programmes Generalitat Valenciana, Spain; Goran Gustafssons Stiftelse, Sweden; The Royal Society and Leverhulme Trust, United Kingdom. The crucial computing support from all WLCG partners is acknowledged gratefully, in particular from CERN, the ATLAS Tier-1 facilities at TRIUMF (Canada), NDGF (Denmark, Norway, Sweden), CC-IN2P3 (France), KIT/GridKA (Germany), INFN-CNAF (Italy), NL-T1 (Netherlands), PIC (Spain), ASGC (Taiwan), RAL (UK) and BNL (USA), theY Tier-2 facilities worldwide and large non-WLCG resource providers. Major contributors of computing resources are listed in Ref. [91]., Measurements of both the inclusive and differential production cross sections of a top-quark-antiquark pair in association with a Z boson (t (t) over barZ) are presented. The measurements are performed by targeting final states with three or four isolated leptons (electrons or muons) and are based on root s = 13 TeV proton-proton collision data with an integrated luminosity of 139 fb(-1), recorded from 2015 to 2018 with the ATLAS detector at the CERN Large Hadron Collider. The inclusive cross section is measured to be a sigma(t (t) over barZ)= 0.99 +/- 0.05 (stat.) +/- 0.08 (syst.) pb, in agreement with the most precise theoretical predictions. The differential measurements are presented as a function of a number of kinematic variables which probe the kinematics of the t (t) over barZ system. Both absolute and normalised differential crosssection measurements are performed at particle and parton levels for specific fiducial volumes and are compared with theoretical predictions at different levels of precision, based on a chi(2)/ndf and p value computation. Overall, good agreement is observed between the unfolded data and the predictions., CERN, ANPCyT, YerPhI, Armenia, Australian Research Council, Conselho Nacional de Desenvolvimento Cientifico e Tecnologico (CNPQ), Fundacao de Amparo a Pesquisa do Estado de Sao Paulo (FAPESP), Natural Sciences and Engineering Research Council of Canada (NSERC), NRC, Canada, Canada Foundation for Innovation, SSTC, Belarus, Ministry of Education, Youth & Sports - Czech Republic Czech Republic Government, Czech Republic Government, DNRF, Denmark, Danish Natural Science Research Council, Centre National de la Recherche Scientifique (CNRS), CEA-DRF/IRFU, France, SRNSFG, Georgia, Federal Ministry of Education & Research (BMBF), HGF, Germany, Max Planck Society, Greek Ministry of Development-GSRT, RGC, China, Hong Kong SAR, China, Israel Science Foundation, Benoziyo Center, Israel, Istituto Nazionale di Fisica Nucleare (INFN), Ministry of Education, Culture, Sports, Science and Technology, Japan (MEXT), Ministry of Education, Culture, Sports, Science and Technology, Japan (MEXT) Japan Society for the Promotion of Science, CNRST, Morocco, Netherlands Organization for Scientific Research (NWO) Netherlands Government, RCN, Norway, Ministry of Science and Higher Education, Poland, NCN, Poland, Portuguese Foundation for Science and Technology European Commission, MNE/IFA, Romania, JINR, MESofRussia, Russian Federation, Ministry of Education, Science & Technological Development, Serbia, MSSR, Slovakia, Slovenian Research Agency - Slovenia, MIZS, Slovenia, DST/NRF, South Africa, Spanish Government, SRC, Sweden, Wallenberg Foundation, Sweden, SERI, Switzerland, Swiss National Science Foundation (SNSF), Cantons of Bern and Geneva, Switzerland, Ministry of Science and Technology, Taiwan, Ministry of Energy & Natural Resources - Turkey, UK Research & Innovation (UKRI) Science & Technology Facilities Council (STFC), DOEandNSF, USA, BCKDF, Canada, CANARIE, Canada, ComputeCanada, Canada, CRC, Canada, IVADO, Canada, Beijing Municipal Science & Technology Commission, COST, France, ERC, France, ERDF, France, Horizon 2020 and Marie Sklodowska-Curie Actions, European Union, France, French National Research Agency (ANR), German Research Foundation (DFG), Alexander von Humboldt Foundation, Thales Group, Aristeia programmes, EU-ESF, Greece, Greek NSRF, Greece, BSF-NSF, Israel, German-Israeli Foundation for Scientific Research and Development, La Caixa Banking Foundation, Spain, CERCA Programme Generalitat de Catalunya, Spain, GenT Programmes Generalitat Valenciana, Spain, Goran Gustafssons Stiftelse, Sweden, Royal Society of London, Leverhulme Trust, BMWFW, Austria, Austrian Science Fund (FWF), Azerbaijan National Academy of Sciences (ANAS), D, Chile, Minciencias, Colombia
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- 2021
16. Invisible Higgs search through vector boson fusion: a deep learning approach
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Partha Konar, Aruna Kumar Nayak, Vishal S. Ngairangbam, and Akanksha Bhardwaj
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Particle physics ,Physics and Astronomy (miscellaneous) ,Event (relativity) ,Physics beyond the Standard Model ,FOS: Physical sciences ,Parton ,lcsh:Astrophysics ,01 natural sciences ,High Energy Physics - Experiment ,Vector boson ,High Energy Physics - Experiment (hep-ex) ,High Energy Physics - Phenomenology (hep-ph) ,0103 physical sciences ,lcsh:QB460-466 ,lcsh:Nuclear and particle physics. Atomic energy. Radioactivity ,010306 general physics ,Engineering (miscellaneous) ,Event reconstruction ,Physics ,010308 nuclear & particles physics ,business.industry ,Deep learning ,High Energy Physics::Phenomenology ,High Energy Physics - Phenomenology ,Higgs boson ,lcsh:QC770-798 ,Artificial intelligence ,business ,Fusion mechanism - Abstract
Vector boson fusion proposed initially as an alternative channel for finding heavy Higgs has now established itself as a crucial search scheme to probe different properties of the Higgs boson or for new physics. We explore the merit of deep-learning entirely from the low-level calorimeter data in the search for invisibly decaying Higgs. Such an effort supersedes decades-old faith in the remarkable event kinematics and radiation pattern as a signature to the absence of any color exchange between incoming partons in the vector boson fusion mechanism. We investigate among different neural network architectures, considering both low-level and high-level input variables as a detailed comparative analysis. To have a consistent comparison with existing techniques, we closely follow a recent experimental study of CMS search on invisible Higgs with 36 fb$^{-1}$ data. We find that sophisticated deep-learning techniques have the impressive capability to improve the bound on invisible branching ratio by a factor of three, utilizing the same amount of data. Without relying on any exclusive event reconstruction, this novel technique can provide the most stringent bounds on the invisible branching ratio of the SM-like Higgs boson. Such an outcome has the ability to constraint many different BSM models severely., Included estimation of pixelwise energy uncertainty, minor changes in text and updated references. Accepted for publication in EPJC
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- 2020
17. Combining single and double parton scatterings in a parton shower
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Baptiste Cabouat and Jonathan R. Gaunt
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Physics ,Nuclear and High Energy Physics ,Particle physics ,010308 nuclear & particles physics ,Scattering ,Subtraction ,Double counting (proof technique) ,FOS: Physical sciences ,Parton ,hep-ph ,Kinematics ,QCD Phenomenology ,01 natural sciences ,Transverse plane ,High Energy Physics - Phenomenology ,High Energy Physics - Phenomenology (hep-ph) ,0103 physical sciences ,lcsh:QC770-798 ,lcsh:Nuclear and particle physics. Atomic energy. Radioactivity ,010306 general physics ,Parton shower ,Nuclear Experiment ,Phenomenological Models ,Boson ,Particle Physics - Phenomenology - Abstract
Double parton scattering (DPS) processes in which there is a perturbative $1\to2$ splitting in both protons overlap with loop corrections to single parton scattering (SPS). Any fundamental theoretical treatment of DPS needs to address this double-counting issue. In this paper, we augment our Monte-Carlo simulation of DPS, dShower, to be able to generate kinematic distributions corresponding to the combination SPS+DPS without double counting. To achieve this, we formulate a fully-differential version of the subtraction scheme introduced in Diehl et al. (JHEP 06 (2017) 083). A shower is attached to the subtraction term, and this is combined with the dShower DPS shower along with the usual SPS shower. We perform a proof-of-concept study of this new algorithm in the context of $\mathrm{Z}^0\mathrm{Z}^0$ production. Once the subtraction term is included, we verify that the results do not depend strongly on the artificial "DPS-SPS demarcation" scale $\nu$. As part of the development of the new algorithm, we improve the kinematics of the $1\to2$ splitting in the DPS shower (and subtraction term), allowing the daughter partons to have a relative transverse momentum. Several reasonable choices for the transverse profile in the $1\to2$ splitting are studied. We find that many kinematic distributions are not strongly affected by the choice, although we do observe some differences in the region where the transverse momenta of both bosons are small., Comment: 46 pages, 18 figures, 1 table
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- 2020
18. Diffractive $$\gamma \gamma $$ γ γ production in pp collisions at the LHC
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D. E. Martins, Victor P. Goncalves, and M. S. Rangel
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Physics ,Particle physics ,Large Hadron Collider ,Physics and Astronomy (miscellaneous) ,hep-ex ,Scattering ,hep-ph ,Parton ,lcsh:Astrophysics ,High Energy Physics - Experiment ,Gamma gamma ,High Energy Physics - Phenomenology ,Distribution function ,Transverse momentum ,lcsh:QB460-466 ,lcsh:QC770-798 ,Invariant mass ,Rapidity ,lcsh:Nuclear and particle physics. Atomic energy. Radioactivity ,Engineering (miscellaneous) ,Particle Physics - Experiment ,Particle Physics - Phenomenology - Abstract
In this letter we estimate the contribution of the double diffractive processes for the diphoton production in $pp$ collisions at the Large Hadron Collider (LHC). The acceptance of the central and forward LHC detectors is taken into account and predictions for the invariant mass, rapidity and, transverse momentum distributions are presented. A comparison with the predictions for the Light -- by -- Light (LbL) scattering and exclusive diphoton production is performed. We demonstrate that the events associated to double diffractive processes can be separated and its study can be used to constrain the behavior of the diffractive parton distribution functions., Comment: 7 pages, 4 figures, 3 tables. Improved version to be published in EPJC. arXiv admin note: text overlap with arXiv:2002.03902
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- 2020
19. Transverse momentum dependent PDFs at N3LO
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Markus A. Ebert, Bernhard Mistlberger, and Gherardo Vita
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Quark ,Physics ,Quantum chromodynamics ,Nuclear and High Energy Physics ,Particle physics ,Nuclear Theory ,High Energy Physics::Lattice ,High Energy Physics::Phenomenology ,FOS: Physical sciences ,Perturbative QCD ,Parton ,Effective Field Theories ,Gluon ,Nuclear Theory (nucl-th) ,High Energy Physics - Phenomenology ,High Energy Physics - Phenomenology (hep-ph) ,Factorization ,Higgs boson ,lcsh:QC770-798 ,High Energy Physics::Experiment ,lcsh:Nuclear and particle physics. Atomic energy. Radioactivity ,Limit (mathematics) ,Nuclear Experiment - Abstract
We compute the quark and gluon transverse momentum dependent parton distribution functions at next-to-next-to-next-to-leading order (N$^3$LO) in perturbative QCD. Our calculation is based on an expansion of the differential Higgs boson and Drell-Yan production cross sections about their collinear limit. This method allows us to employ cutting edge techniques for the computation of cross sections to extract the universal building blocks in question. The corresponding perturbative matching kernels for all channels are expressed in terms of simple harmonic polylogarithms up to weight five. As a byproduct, we confirm a previous computation of the soft function for transverse momentum factorization at N$^3$LO. Our results are the last missing ingredient to extend the $q_T$ subtraction methods to N$^3$LO and to obtain resummed $q_T$ spectra at N$^3$LL$^\prime$ accuracy both for gluon as well as for quark initiated processes., Comment: 12 pages + appendices, 4 awesome figures, important ancillary files. v2: journal version
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- 2020
20. Leptons in the proton
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Giulia Zanderighi, Luca Buonocore, Paolo Nason, Francesco Tramontano, University of Zurich, Nason, Paolo, Buonocore, L., Nason, P., Tramontano, F., Zanderighi, G., Buonocore, L, Nason, P, Tramontano, F, and Zanderighi, G
- Subjects
Particle physics ,Nuclear and High Energy Physics ,Photon ,Proton ,530 Physics ,Physics beyond the Standard Model ,Hadron ,FOS: Physical sciences ,Parton ,10192 Physics Institute ,01 natural sciences ,High Energy Physics - Experiment ,High Energy Physics - Experiment (hep-ex) ,High Energy Physics - Phenomenology (hep-ph) ,NLO Computations ,0103 physical sciences ,lcsh:Nuclear and particle physics. Atomic energy. Radioactivity ,3106 Nuclear and High Energy Physics ,010306 general physics ,Physics ,Large Hadron Collider ,010308 nuclear & particles physics ,High Energy Physics::Phenomenology ,QCD Phenomenology ,High Energy Physics - Phenomenology ,Standard Model (mathematical formulation) ,NLO Computation ,lcsh:QC770-798 ,High Energy Physics::Experiment ,Lepton - Abstract
As is the case for all light coloured Standard Model particles, also photons and charged leptons appear as constituents in ultrarelativistic hadron beams, and admit a parton density function (PDF). It has been shown recently that the photon PDF can be given in terms of the structure functions and form factors for electron-proton scattering. The same holds for lepton PDFs. In the present work we set up a calculation of the lepton PDFs at next-to-leading order, using the same data input needed in the photon case. A precise knowledge of the lepton densities allows us to study lepton-initiated processes even at a hadron collider, with all possible combinations of same-charge, opposite-charge, same-flavour, different-flavour leptons and leptons-quarks, most of which cannot be realized in any other foreseeable experiment. The lepton densities in the proton are extremely small, so that their contribution to Standard Model processes is generally shadowed by processes initiated by coloured partons. We will show, however, that there are cases where these processes can be relevant, giving rise to rare Standard Model signatures and to new production channels, that can enlarge the discovery potential of New Physics at the LHC and future high energy colliders with hadrons in the initial state., Comment: 43 pages, 14 figures. In V2 we have included a class of subleading O(alpha^2) contributions to the lepton PDFs and motivated this choice. Data in the LHAPDF files have been updated accordingly (see info file). V2 is identical to the published version
- Published
- 2020
21. Z plus jets production via double parton scattering in pA collisions at the LHC
- Author
-
Boris Blok and Federico Alberto Ceccopieri
- Subjects
Physics ,Particle physics ,Large Hadron Collider ,Physics and Astronomy (miscellaneous) ,Scattering ,High Energy Physics::Phenomenology ,Parton ,lcsh:Astrophysics ,Jet (particle physics) ,Measure (mathematics) ,Cross section (physics) ,Transverse plane ,lcsh:QB460-466 ,lcsh:QC770-798 ,lcsh:Nuclear and particle physics. Atomic energy. Radioactivity ,Nuclear Experiment ,Engineering (miscellaneous) ,Nuclear theory - Abstract
We present results on Zjj production via double parton scattering in pA collisions at the LHC. We perform the analysis at leading and next-leading order accuracy with different sets of cuts on jet transverse momenta and accounting for the single parton scattering background. By exploiting the experimental capability to measure the centrality dependence of the cross section, we discuss the feasibility of DPS observation in already collected data at the LHC and in future runs.
- Published
- 2020
22. Sector showers for hadron collisions
- Author
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Helen Brooks, Peter Skands, and Christian T Preuss
- Subjects
Nuclear and High Energy Physics ,Particle physics ,Physics::Instrumentation and Detectors ,Hadron ,FOS: Physical sciences ,Context (language use) ,Parton ,01 natural sciences ,High Energy Physics - Experiment ,Shower ,High Energy Physics - Experiment (hep-ex) ,Operator (computer programming) ,High Energy Physics - Phenomenology (hep-ph) ,0103 physical sciences ,lcsh:Nuclear and particle physics. Atomic energy. Radioactivity ,010306 general physics ,Phenomenological Models ,Physics ,010308 nuclear & particles physics ,High Energy Physics::Phenomenology ,Astrophysics::Instrumentation and Methods for Astrophysics ,QCD Phenomenology ,Helicity ,High Energy Physics - Phenomenology ,Kernel (image processing) ,Bijection ,lcsh:QC770-798 ,High Energy Physics::Experiment - Abstract
In conventional parton showers (including ones based on dipoles/antennae), a given $(\mathrm{Born}+m)$-parton configuration can typically be reached via ${\mathcal O}(m!)$ different "shower histories". In the context of matrix-element-correction and merging procedures, accounting for these histories mandates fairly complex and resource-intensive algorithms. A so far little-explored alternative in the shower context is to divide the branching phase spaces into distinct "sectors", each of which only receives contributions from a single branching kernel. This has a number of consequences including making the shower operator bijective; i.e., each parton configuration now has a single unique "inverse". As a first step towards developing a full-fledged matrix-element-correction and merging procedure based on such showers, we here extend the sector approach for antenna showers to hadron-hadron collisions, including mass and helicity dependence., Comment: 56 pages, 20 figures; added reference in section 2; extend discussion in sections 3.1 and 4.2; corrected typos
- Published
- 2020
23. Analytic double-soft integrated subtraction terms for two massive emitters in a back-to-back kinematics
- Author
-
Maximilian Delto and Wojciech Bizoń
- Subjects
Quantum chromodynamics ,Quark ,Physics ,Nuclear and High Energy Physics ,Particle physics ,Eikonal equation ,High Energy Physics::Phenomenology ,Subtraction ,FOS: Physical sciences ,Context (language use) ,Parton ,QCD Phenomenology ,High Energy Physics - Phenomenology ,High Energy Physics - Phenomenology (hep-ph) ,Pair production ,Phase space ,lcsh:QC770-798 ,ddc:530 ,High Energy Physics::Experiment ,lcsh:Nuclear and particle physics. Atomic energy. Radioactivity - Abstract
We consider the double-soft limit of QCD amplitudes with two massive quarks in a back-to-back kinematics accompanied by two soft partons. We integrate analytically the respective double-soft eikonal functions over the phase space of the two soft partons. Within the context of the nested soft-collinear subtraction scheme, our results may serve as one of the integrated subtraction terms needed for the analytic and fully-differential description of next-to-next-to-leading order (NNLO) QCD corrections to colour-singlet decay into massive partons or to heavy-quark pair production.
- Published
- 2020
24. Two-Jet Correlations in Multijet Events in the Regge Limit of QCD
- Author
-
Maxim Nefedov and Vladimir Saleev
- Subjects
Quantum chromodynamics ,Quark ,Physics ,Nuclear and High Energy Physics ,Particle physics ,Large Hadron Collider ,010308 nuclear & particles physics ,High Energy Physics::Phenomenology ,Parton ,Jet (particle physics) ,01 natural sciences ,Gluon ,0103 physical sciences ,Effective field theory ,High Energy Physics::Experiment ,Perturbation theory (quantum mechanics) ,Nuclear Experiment ,010306 general physics - Abstract
A new method for matching calculations in the leading approximation in the kT-factorization approach with the higher-order contributions of perturbation theory, which appear due to the emission of additional hard partons, is proposed. In the proposed method, azimuthal correlations between the leading and subleading jets in a multijet event are considered. The calculations are carried out within the parton Reggeization approach (PRA) that is based on kT-factorization of hard processes in multi-Regge kinematics, the Kimber–Martin–Ryskin model for nonintegrated parton distribution functions (nPDF), and the effective field theory of Reggeized gluons and quarks proposed by L.N. Lipatov. Theoretical predictions are compared with the CMS collaboration data collected at the Large Hadron Collider at energy $$\sqrt S = 13$$ TeV.
- Published
- 2020
25. Heavy-light mesons on the light front
- Author
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Pieter Maris, Yang Li, Shuo Tang, and James P. Vary
- Subjects
Physics ,Particle physics ,Physics and Astronomy (miscellaneous) ,Meson ,Nuclear Theory ,High Energy Physics::Lattice ,High Energy Physics::Phenomenology ,FOS: Physical sciences ,Parton ,Observable ,lcsh:Astrophysics ,Pseudoscalar meson ,Nuclear Theory (nucl-th) ,Quantization (physics) ,High Energy Physics - Phenomenology ,Amplitude ,Distribution function ,High Energy Physics - Phenomenology (hep-ph) ,lcsh:QB460-466 ,lcsh:QC770-798 ,High Energy Physics::Experiment ,lcsh:Nuclear and particle physics. Atomic energy. Radioactivity ,Wave function ,Engineering (miscellaneous) - Abstract
We study the heavy-light mesons within basis light-front quantization. The resulting mass spectra of $D$, $D_s$, $B$, and $B_s$ agree reasonably well with experiments. We also predict states which could be measured in the near future. In the light-front formalism, we calculate the light-front wave functions and additional experimental observables, such as parton distribution functions, distribution amplitudes, and decay constants by means of integrations over light-front wave functions. We also provide ratios of decay constants for selected pseudoscalar meson decays ($D_s$ to $D$ and $B_s$ to $B$) as they may prove to be theoretically more robust and more reliably determined in experiments. We find that our ratios are systematically smaller than existing experiment and other approaches by $5-18\%$., 15 pages, 19 figures, 2 tables
- Published
- 2020
26. Diffractive dijet photoproduction at the EIC
- Author
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Vadim Guzey and Michael Klasen
- Subjects
Nuclear and High Energy Physics ,Particle physics ,Nuclear Theory ,FOS: Physical sciences ,Parton ,Kinematics ,01 natural sciences ,High Energy Physics - Experiment ,law.invention ,Nuclear Theory (nucl-th) ,High Energy Physics - Experiment (hep-ex) ,Pomeron ,High Energy Physics - Phenomenology (hep-ph) ,Factorization ,law ,NLO Computations ,0103 physical sciences ,lcsh:Nuclear and particle physics. Atomic energy. Radioactivity ,Nuclear Experiment (nucl-ex) ,010306 general physics ,Collider ,Nuclear Experiment ,Nuclear theory ,Quantum chromodynamics ,Physics ,010308 nuclear & particles physics ,High Energy Physics::Phenomenology ,HERA ,Heavy Ion Phenomenology ,High Energy Physics - Phenomenology ,lcsh:QC770-798 ,High Energy Physics::Experiment - Abstract
We present a first, detailed study of diffractive dijet photoproduction at the recently approved electron-ion collider (EIC) at BNL. Apart from establishing the kinematic reaches for various beam types, energies and kinematic cuts, we make precise predictions at next-to-leading order (NLO) of QCD in the most important kinematic variables. We show that the EIC will provide new and more precise information on the diffractive parton density functions (PDFs) in the pomeron than previously obtained at HERA, illuminate the still disputed mechanism of global vs.\ only resolved-photon factorization breaking, and provide access to a completely new quantity, i.e. nuclear diffractive PDFs., Comment: 20 pages, 10 figures
- Published
- 2020
27. Elliptic Flow of Hadrons via Quark Coalescence Mechanism Using the Boltzmann Transport Equation for Pb+Pb Collision at sNN=2.76 TeV
- Author
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Raghunath Sahoo, Mohammed Younus, Swatantra Kumar Tiwari, and Sushanta Tripathy
- Subjects
Physics ,Quark ,Nuclear and High Energy Physics ,Particle physics ,Nuclear Theory ,High Energy Physics::Phenomenology ,Hadron ,Elliptic flow ,Parton ,Deconfinement ,Boltzmann equation ,Hadronization ,High Energy Physics::Experiment ,Nuclear Experiment ,Relativistic Heavy Ion Collider - Abstract
Elliptic flow of hadrons observed at relativistic heavy ion collision experiments at relativistic heavy ion collider (RHIC) and large hadron collider (LHC) provides us an important signature of possible deconfinement transition from the hadronic phase to partonic phase. However, hadronization processes of deconfined partons back into final hadrons are found to play a vital role in the observed hadronic flow. In the present work, we use a coalescence mechanism also known as recombination (ReCo) to combine quarks into hadrons. To get there, we have used the Boltzmann transport equation in relaxation time approximation to transport the quarks into equilibration and finally to freeze-out the surface, before coalescence takes place. A Boltzmann-Gibbs blast wave (BGBW) function is taken as an equilibrium function to get the final distribution and a power-like function to describe the initial distributions of partons produced in heavy ion collisions. In the present work, we try to estimate the elliptic flow of identified hadrons such as π, K, and p, produced in Pb+Pb collisions at sNN=2.76 TeV at the LHC for different centralities. The elliptic flow (v2) of identified hadrons seems to be described quite well in the available pT range. After the evolution of quarks until freeze-out time has been calculated using BTE-RTA, the approach used in this paper consists of combining two or more quarks to explain the produced hadrons at intermediate momenta regions. The formalism is found to describe the elliptic flow of hadrons produced in Pb+Pb collisions to a large extent.
- Published
- 2020
28. CP-violating Higgs-gauge boson couplings in $$H\nu \bar{\nu }$$ Hνν¯ production at three energy stages of CLIC
- Author
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Haluk Denizli, A. Senol, K. Y. Oyulmaz, O. Karadeniz, BAİBÜ, Fen Edebiyat Fakültesi, Fizik Bölümü, Şenol, Abdulkadir, Denizli, Haluk, and Oyulmaz, Kaan Yüksel
- Subjects
Particle physics ,Physics and Astronomy (miscellaneous) ,Astrophysics::High Energy Astrophysical Phenomena ,Parton ,lcsh:Astrophysics ,01 natural sciences ,Standard Model ,High Energy Physics - Experiment ,0103 physical sciences ,lcsh:QB460-466 ,Effective field theory ,lcsh:Nuclear and particle physics. Atomic energy. Radioactivity ,010306 general physics ,Engineering (miscellaneous) ,Physics ,Gauge boson ,010308 nuclear & particles physics ,Hadronization ,High Energy Physics - Phenomenology ,Higgs boson ,lcsh:QC770-798 ,Production (computer science) ,High Energy Physics::Experiment ,CLIC ,Energy (signal processing) ,Particle Physics - Experiment ,Higgs-gauge Boson Couplings - Abstract
A phenomenological study of CP-violating dimension-six operators via the $e^+e^-\to\nu \bar{\nu} H$ process is performed in a model-independent Standard Model effective field theory framework at all energy stages of CLIC using the updated baseline integrated luminosities. All signal and relevant background events are generated in MadGraph and passed through PYTHIA for parton showering and hadronization at parton level. Detector effects are considered via tuned CLIC detector cards in Delphes. Since we reconstruct the Higgs boson from a pair of b-jets, limits on CP-violating dimension-six couplings are obtained at three $b$-tagging working points: tight, medium and loose defined in the CLIC Delphes card for all three energy stages of CLIC. Our best 95 \% C.L. limits at the loose working point (90 \% b-tagging efficiency) on $\tilde c_{HW}$ and $\tilde c_{HB}$ are $[-7.0\times10^{-3};7.0\times10^{-3}]$ and $[-3.0\times10^{-2};3.0\times10^{-2}]$, respectively at the 3 TeV energy stage of CLIC with an integrated luminosity of 5.0 ab$^{-1}$. Considering a 0.3 \% systematic uncertainty from possible experimental sources worsens the limits on these couplings by a factor of two., Comment: 13 pages, 10 figures
- Published
- 2020
29. Parton and Valon Distributions in the Nuclei
- Author
-
Abolfazl Mirjalili, Javad Sheibani, and S. Atashbar Tehrani
- Subjects
Physics ,Quantum chromodynamics ,Quark ,Particle physics ,Physics and Astronomy (miscellaneous) ,010308 nuclear & particles physics ,General Mathematics ,Nuclear Theory ,EMC effect ,Parton ,Deep inelastic scattering ,01 natural sciences ,Distribution function ,0103 physical sciences ,Bound state ,High Energy Physics::Experiment ,Nuclear Experiment ,010306 general physics ,Nucleon - Abstract
In the valon model a nucleon is assumed to be a bound state of three valence quark clusters (valons). On this base the nucleus structure function which are made from nucleons are analysed. Here in the frame work of perturbative quantum chromodynamics (pQCD) the structure of the valons are described at next to leading-order (NLO) approximation. Using the constituent-quark model, structure function of nucleon is largely investigated in the nuclear medium. For a series of nuclei with the nuclear mass A such that 2 ≤ A ≤ 40 within the kinetic region 0.0001 ≤ x ≤ 0.9 which covers a wide range of x Bjorken variable, the theoretical predications are in good agreement with the existing lepton-nucleus data. A better and fair description of experimental data can be done, considering the shadowing effect for small values of x i.e. x
- Published
- 2020
30. Safe use of jet pull
- Author
-
Chang Wu, Andrew J. Larkoski, and Simone Marzani
- Subjects
Quark ,Nuclear and High Energy Physics ,Particle physics ,media_common.quotation_subject ,Monte Carlo method ,FOS: Physical sciences ,Context (language use) ,Parton ,Jet (particle physics) ,01 natural sciences ,Asymmetry ,High Energy Physics - Phenomenology (hep-ph) ,0103 physical sciences ,Jets ,lcsh:Nuclear and particle physics. Atomic energy. Radioactivity ,010306 general physics ,media_common ,Physics ,Quantum chromodynamics ,010308 nuclear & particles physics ,High Energy Physics::Phenomenology ,QCD Phenomenology ,High Energy Physics - Phenomenology ,Higgs boson ,lcsh:QC770-798 ,High Energy Physics::Experiment - Abstract
Jet pull is an observable designed to probe colour flow between jets. Thus far, a particular projection of the pull vector, the pull angle, has been employed to distinguish colour flow between jets produced by a colour singlet or an octet decay. This is of particular importance in order to separate the decay of a Higgs boson to a pair of bottom quarks from the QCD background. However, the pull angle is not infra-red and collinear (IRC) safe. In this paper we introduce IRC safe projections of the pull vector that exhibit good sensitivity to colour flow, while maintaining calculability. We calculate these distributions to next-to-leading logarithmic accuracy, in the context of the hadronic decay of a Higgs boson, and compare these results to Monte Carlo simulations. This study allows us to define an IRC safe version of the pull angle in terms of asymmetry distributions. Furthermore, because of their sensitivity to wide-angle soft radiation, we anticipate that these asymmetries can play an important role in assessing subleading colour correlations and their modelling in general-purpose Monte Carlo parton showers., 21 pages, 6 figures. Version accepted for publication
- Published
- 2020
31. Prospects for quarkonium studies at the high-luminosity LHC
- Author
-
Melih Arslan Ozcelik, Carlo Flore, Oleg Teryaev, Shohini Bhattacharya, L. Massacrier, Tomas Kasemets, Chris A. Flett, David D'Enterria, Cyrille Marquet, Riccardo Nagar, V. Kartvelishvili, Maxim Nefedov, Miguel G. Echevarria, R. McNulty, Charlotte Van Hulse, Luca Micheletti, Nodoka Yamanaka, Francesco Giovanni Celiberto, Pol Bernard Gossiaux, Hua-Sheng Shao, Thomas Mehen, M. Winn, Bertrand Ducloué, Amy Selvi Tee, Maria Vittoria Garzelli, Cvetan Valeriev Cheshkov, Yiannis Makris, Pieter Taels, Xiaojun Yao, Denys Yen Arrebato Villar, Matteo Rinaldi, Liupan An, Jibo He, Jonathan R. Gaunt, Cédric Mezrag, Darren Price, Florent Scarpa, Emilien Chapon, Kazuhiro Watanabe, Umberto D'Alesio, Jian-Wei Qiu, Yanxi Zhang, Ivan Vitev, Cesar Luiz Da Silva, Sangem Rajesh, Jean-Philippe Lansberg, Jaroslav Adam, Cristian Pisano, Biswarup Paul, E. G. Ferreiro, Maddie Smith, Laboratoire de physique subatomique et des technologies associées (SUBATECH), Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS)-IMT Atlantique (IMT Atlantique), Institut Mines-Télécom [Paris] (IMT)-Institut Mines-Télécom [Paris] (IMT)-Nantes université - UFR des Sciences et des Techniques (Nantes univ - UFR ST), Nantes Université - pôle Sciences et technologie, Nantes Université (Nantes Univ)-Nantes Université (Nantes Univ)-Nantes Université - pôle Sciences et technologie, Nantes Université (Nantes Univ)-Nantes Université (Nantes Univ), Laboratoire de Physique des 2 Infinis Irène Joliot-Curie (IJCLab), Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Université Paris-Saclay-Centre National de la Recherche Scientifique (CNRS), Laboratoire de Physique Théorique et Hautes Energies (LPTHE), Sorbonne Université (SU)-Centre National de la Recherche Scientifique (CNRS), Institut de Recherches sur les lois Fondamentales de l'Univers (IRFU), Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Université Paris-Saclay, Institut de Physique des 2 Infinis de Lyon (IP2I Lyon), Université Claude Bernard Lyon 1 (UCBL), Université de Lyon-Université de Lyon-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS), Centre de Physique Théorique [Palaiseau] (CPHT), École polytechnique (X)-Centre National de la Recherche Scientifique (CNRS), ANR-20-CE31-0015,PrecisOnium,Promouvoir la précision des études de la production de quarkonia(2020), Université de Nantes - UFR des Sciences et des Techniques (UN UFR ST), Université de Nantes (UN)-Université de Nantes (UN)-Centre National de la Recherche Scientifique (CNRS)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-IMT Atlantique Bretagne-Pays de la Loire (IMT Atlantique), Institut Mines-Télécom [Paris] (IMT)-Institut Mines-Télécom [Paris] (IMT), Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Université Claude Bernard Lyon 1 (UCBL), and Université de Lyon-Université de Lyon-Centre National de la Recherche Scientifique (CNRS)
- Subjects
J/psi(3100) ,heavy ion: scattering ,generalized parton distribution ,Nuclear Theory ,Proton ,nucleus nucleus ,parton: distribution function ,Parton ,eta/c(3590) ,nucl-ex ,transverse momentum dependence ,Large Hadron Collider (LHC) ,7. Clean energy ,01 natural sciences ,High Energy Physics - Experiment ,law.invention ,Sivers function ,High Energy Physics - Experiment (hep-ex) ,High Energy Physics - Phenomenology (hep-ph) ,law ,High Luminosity ,[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex] ,parton ,Nuclear Experiment (nucl-ex) ,Quarkonium production ,Nuclear Experiment ,quark gluon: plasma ,Physics ,Large Hadron Collider ,Luminosity (scattering theory) ,hep-ph ,high ,nucleus nucleus: scattering ,Quarkonium ,heavy ion ,High Energy Physics - Phenomenology ,CERN LHC Coll ,Nuclear Physics - Theory ,luminosity: high ,eta/c(2980) ,Particle Physics - Experiment ,quarkonium ,Nuclear and High Energy Physics ,Particle physics ,p p: scattering ,small-x ,CERN Lab ,nucl-th ,[PHYS.NUCL]Physics [physics]/Nuclear Theory [nucl-th] ,collective ,FOS: Physical sciences ,transverse momentum ,[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex] ,Nuclear Theory (nucl-th) ,0103 physical sciences ,Nuclear Physics - Experiment ,luminosity ,010306 general physics ,Collider ,p nucleus: scattering ,quark gluon ,plasma ,Particle Physics - Phenomenology ,010308 nuclear & particles physics ,hep-ex ,High Energy Physics::Phenomenology ,scattering ,nucleus ,gluon ,Gluon ,[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph] ,Quark–gluon plasma ,High Energy Physics::Experiment ,p nucleus ,production - Abstract
Prospects for quarkonium-production studies accessible during the upcoming high-luminosity phases of the CERN Large Hadron Collider operation after 2021 are reviewed. Current experimental and theoretical open issues in the field are assessed together with the potential for future studies in quarkonium-related physics. This will be possible through the exploitation of the huge data samples to be collected in proton-proton, proton-nucleus and nucleus-nucleus collisions, both in the collider and fixed-target modes. Such investigations include, among others, those of: (i) J/psi and Upsilon produced in association with other hard particles; (ii) chi(c,b) and eta(c,b) down to small transverse momenta; (iii) the constraints brought in by quarkonia on gluon PDFs, nuclear PDFs, TMDs, GPDs and GTMDs, as well as on the low-x parton dynamics; (iv) the gluon Sivers effect in polarised-nucleon collisions; (v) the properties of the quark-gluon plasma produced in ultra-relativistic heavy-ion collisions and of collective partonic effects in general; and (vi) double and triple parton scatterings., Comment: Latex, 115 pages, 55 figures, 4 tables. v2: Review published in Progress in Particle and Nuclear Physics
- Published
- 2022
32. Revealing pion and kaon structure via generalised parton distributions
- Author
-
Khépani Raya, Craig D. Roberts, Lei Chang, Zhu-Fang Cui, Jose Rodríguez-Quintero, and Jose-Manuel Morgado
- Subjects
Nuclear and High Energy Physics ,Particle physics ,Continuum Schwinger function methods ,Nuclear Theory ,Meson ,Hadron ,FOS: Physical sciences ,Parton ,High Energy Physics - Experiment ,Nambu-Goldstone modes ,Nuclear Theory (nucl-th) ,High Energy Physics - Experiment (hep-ex) ,High Energy Physics - Lattice ,High Energy Physics - Phenomenology (hep-ph) ,Pion ,Pions and kaons ,Nambu-Goldstone modes-pions and kaons ,22 Física ,Nuclear Experiment (nucl-ex) ,Nuclear Experiment ,Instrumentation ,Physics ,Parton distributions ,High Energy Physics::Phenomenology ,High Energy Physics - Lattice (hep-lat) ,Astronomy and Astrophysics ,Observable ,Strong interactions ,High Energy Physics - Phenomenology ,Distribution function ,Nonperturbative quantum field theory ,Higgs boson ,High Energy Physics::Experiment ,Impact parameter ,Emergence of hadron mass - Abstract
Supported by National Natural Science Foundation of China (12135007, 11805097); Jiangsu Provincial Natural Science Foundation of China (BK20180323); Spanish Ministry of Science and Innovation (MICINN) (PID2019-107844GB-C22); Junta de Andalucia (P18-FR-5057, UHU-1264517); and University of Huelva (EPIT-2019), Clear windows onto emergent hadron mass (EHM) and modulations thereof by Higgs boson interactions are provided by observable measures of pion and kaon structure, many of which are accessible via generalised parton distributions (GPDs). Beginning with algebraic GPD Ansatze, constrained entirely by hadron-scale pi and K valence-parton distribution functions (DFs), in whose forms both EHM and Higgs boson influences are manifest, numerous illustrations are provided. They include the properties of electromagnetic form factors, impact parameter space GPDs, gravitational form factors and associated pressure profiles, and the character and consequences of all-orders evolution. The analyses predict that mass-squared gravitational form factors are stiffer than electromagnetic form factors; reveal that K pressure profiles are tighter than pi profiles, with both mesons sustaining near-core pressures at magnitudes similar to that expected at the core of neutron stars; deliver parameter-free predictions for pi and K valence, glue, and sea GPDs at the resolving scale zeta = 2 GeV; and predict that at this scale the fraction of meson mass-squared carried by glue and sea combined matches that lodged with the valence degrees-of-freedom, with a similar statement holding for mass-squared radii., National Natural Science Foundation of China (NSFC) 12135007 11805097, Natural Science Foundation of Jiangsu Province BK20180323, Spanish Government, European Commission PID2019-107844GB-C22, Junta de Andalucia P18-FR-5057, UHU-1264517 University of Huelva EPIT-2019
- Published
- 2022
33. Double parton distributions in the pion in the Nambu–Jona-Lasinio model
- Author
-
Aurore Courtoy, Sergio Scopetta, S. Noguera, and Ministerio de Economía y Competitividad (España)
- Subjects
Quark ,Nuclear and High Energy Physics ,Particle physics ,High Energy Physics::Lattice ,Nuclear Theory ,FOS: Physical sciences ,Parton ,01 natural sciences ,Pion ,High Energy Physics - Phenomenology (hep-ph) ,Nambu–Jona-Lasinio model ,Lattice (order) ,0103 physical sciences ,lcsh:Nuclear and particle physics. Atomic energy. Radioactivity ,010306 general physics ,Nuclear Experiment ,Phenomenological Models ,Deep Inelastic Scattering (Phenomenology) ,Physics ,010308 nuclear & particles physics ,High Energy Physics::Phenomenology ,High Energy Physics - Phenomenology ,Distribution function ,Regularization (physics) ,lcsh:QC770-798 ,High Energy Physics::Experiment ,Non-perturbative - Abstract
Two-parton correlations in the pion, a non perturbative information encoded in double parton distribution functions, are investigated in the Nambu and Jona-Lasinio model. It is found that double parton distribution functions expose novel dynamical information on the structure of the pion, not accessible through one-body parton distributions, as it happens in several estimates for the proton target and in a previous evaluation for the pion, in a light-cone framework. Expressions and predictions are given for double parton distributions corresponding to leading-twist Dirac operators in the quark vertices, and to different regularization methods for the Nambu and Jona-Lasinio model. These results are particularly relevant in view of forthcoming lattice data., 22 pages, 6 figures
- Published
- 2019
34. Scalar-pseudoscalar pair production at the Large Hadron Collider at NLO+NLL accuracy in QCD
- Author
-
Shu-Xiang Li, Yu Zhang, Ren-You Zhang, Ming-Ming Long, He-Yi Li, and Wen-Gan Ma
- Subjects
Quantum chromodynamics ,Physics ,Nuclear and High Energy Physics ,Particle physics ,High Energy Physics::Lattice ,High Energy Physics::Phenomenology ,FOS: Physical sciences ,Astronomy and Astrophysics ,Parton ,Type (model theory) ,High Energy Physics - Phenomenology ,Pair production ,Distribution function ,High Energy Physics - Phenomenology (hep-ph) ,Production (computer science) ,Invariant mass ,High Energy Physics::Experiment ,Resummation ,Nuclear Experiment ,Instrumentation - Abstract
We thoroughly investigate both transverse momentum and threshold resummation effects on scalar-pseudoscalar pair production via quark-antiquark annihilation at the $13~ \text{TeV}$ Large Hadron Collider at QCD NLO+NLL accuracy. A factorization method is introduced to properly supplement the soft-gluon (threshold) resummation contribution from parton distribution functions to the resummed results obtained by the Collins-Soper-Sterman resummation approach. We find that the impact of the threshold-resummation improved PDFs is comparable to the resummation effect of the partonic matrix element and can even predominate in high invariant mass regions. Moreover, the loop-induced gluon-gluon fusion channel in the type-I two-Higgs-doublet model is considered in our calculation. The numerical results show that the electroweak production via quark-antiquark annihilation dominates over the gluon-initiated QCD production by $1 \sim 2$ orders of magnitude., 29 pages, 6 figures
- Published
- 2021
35. Transition distribution amplitudes and hard exclusive reactions with baryon number transfer
- Author
-
Kirill M. Semenov-Tian-Shansky, L. Szymanowski, Bernard Pire, Centre de Physique Théorique [Palaiseau] (CPHT), Centre National de la Recherche Scientifique (CNRS)-École polytechnique (X), National Research Centre 'Kurchatov Institute': Petersburg Nuclear Physics Institute, National Center for Nuclear Research [Warsaw] (NCBJ), and National Center for Nuclear Research (NCBJ)
- Subjects
Particle physics ,Meson ,Distribution (number theory) ,Nuclear Theory ,Structure (category theory) ,FOS: Physical sciences ,General Physics and Astronomy ,Parton ,01 natural sciences ,Interpretation (model theory) ,High Energy Physics - Experiment ,Nuclear Theory (nucl-th) ,High Energy Physics - Experiment (hep-ex) ,High Energy Physics - Phenomenology (hep-ph) ,0103 physical sciences ,010306 general physics ,Nuclear Experiment ,Physics ,010308 nuclear & particles physics ,High Energy Physics::Phenomenology ,3. Good health ,Baryon ,High Energy Physics - Phenomenology ,Amplitude ,[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph] ,High Energy Physics::Experiment ,Baryon number - Abstract
Baryon-to-meson and baryon-to-photon transition distribution amplitudes (TDAs) arise in the collinear factorized description of a class of hard exclusive reactions characterized by the exchange of a non-zero baryon number in the cross channel. These TDAs extend the concepts of generalized parton distributions (GPDs) and baryon distribution amplitudes (DAs). In this review, we discuss the general properties and physical interpretation of baryon-to-meson and baryon-to-photon TDAs. We argue that these non-perturbative objects are a convenient complementary tool to explore the structure of baryons at the partonic level. We present an overview of hard exclusive reactions admitting a description in terms of TDAs. We discuss the first signals from hard exclusive backward meson electroproduction at JLab with the 6 GeV electron beam and explore further experimental opportunities to access TDAs at JLab@12 GeV, PANDA, J-PARC and EIC., 172 pages, 54 figures, 3 tables. Revised version published with Physics Reports
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- 2021
36. Gluon PDF from quark dressing in the nucleon and pion
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Ian C. Cloët, Adam Freese, and Peter C. Tandy
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Quark ,Nuclear and High Energy Physics ,Particle physics ,Nuclear Theory ,High Energy Physics::Lattice ,QC1-999 ,Hadron ,FOS: Physical sciences ,Parton ,01 natural sciences ,Nuclear Theory (nucl-th) ,Pion ,High Energy Physics - Lattice ,High Energy Physics - Phenomenology (hep-ph) ,0103 physical sciences ,Nuclear Experiment (nucl-ex) ,010306 general physics ,Nuclear Experiment ,Quantum chromodynamics ,Physics ,010308 nuclear & particles physics ,High Energy Physics - Lattice (hep-lat) ,High Energy Physics::Phenomenology ,Helicity ,Gluon ,High Energy Physics - Phenomenology ,High Energy Physics::Experiment ,Nucleon - Abstract
Gluon dressing of the light quarks within hadrons is very strong and extremely important in that it dynamically generates most of the observable mass through the breaking of chiral symmetry. The quark and gluon parton densities, $q(x)$ and $g(x)$, are necessarily interrelated since any gluon emission and absorption process, especially dressing of a quark, contributes to $g(x)$ and modifies $q(x)$. Guided by long-established results for the parton-in-parton distributions from a strict 1-loop perturbative analysis of a quark target, we extend the non-perturbative QCD approach based on the Rainbow-Ladder truncation of the Dyson-Schwinger equations to describe the interrelated valence $q_{\rm v}(x)$ and the dressing-gluon $g(x)$ for a hadron at its intrinsic model scale. We employ the pion description from previous DSE work that accounted for the gluon-in-quark effect and introduce a simple model of the nucleon for exploratory purposes. We find typically \mbox{$\langle x \rangle_g \sim 0.20$} for both pion and nucleon at the model scale, and the valence quark helicity contributes 52\% of nucleon spin. We deduce both $q_{\rm v}(x)$ and $g(x)$ from 30 calculated Mellin moments, and after adopting existing data analysis results for $q_{\rm sea}(x)$, we find that NLO scale evolution produces $g(x)$ in good agreement with existing data analysis results for the pion at 1.3 GeV and the nucleon at 5 GeV$^2$. At the scale 2 GeV typical of lattice-QCD calculations, we obtain \mbox{$\langle x \rangle_g^{\rm N} = 0.42$} in good agreement with 0.38 from the average of recent lattice-QCD calculations., Comment: 8 pages, 5 figures. Removed 1 figure, added 1 figure, addded explanatory text, corrected typos, added several new references. This version to be published
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- 2021
37. Gluon parton distribution of the pion from lattice QCD
- Author
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Huey-Wen Lin and Zhouyou Fan
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Quark ,Physics ,Nuclear and High Energy Physics ,Particle physics ,Nuclear Theory ,High Energy Physics::Lattice ,QC1-999 ,High Energy Physics - Lattice (hep-lat) ,High Energy Physics::Phenomenology ,FOS: Physical sciences ,Parton ,Fermion ,Lattice QCD ,Gluon ,Momentum ,Nuclear Theory (nucl-th) ,High Energy Physics - Phenomenology ,Lattice constant ,Pion ,High Energy Physics - Phenomenology (hep-ph) ,High Energy Physics - Lattice ,High Energy Physics::Experiment ,Nuclear Experiment - Abstract
We present the first determination of the $x$-dependent pion gluon distribution from lattice QCD using the pseudo-PDF approach. We use lattice ensembles with 2+1+1 flavors of highly improved staggered quarks (HISQ), generated by MILC Collaboration, at two lattice spacings $a\approx 0.12$ and 0.15~fm and three pion masses $M_\pi\approx 220$, 310 and 690 MeV. We use clover fermions for the valence action and momentum smearing to achieve pion boost momentum up to 2.29 GeV. We find that the dependence of the pion gluon parton distribution on lattice spacing and pion mass is mild. We compare our results from the lightest pion mass ensemble with the determination by JAM and xFitter global fits., Comment: 10 pages, 6 figures
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- 2021
38. On matter and pressure distribution in nucleons
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Maryna Oleksiienko, R. Fiore, and László Jenkovszky
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Physics ,Nuclear and High Energy Physics ,Particle physics ,Radiation ,Distribution (number theory) ,Hadron ,Analytic model ,High Energy Physics::Phenomenology ,Nuclear Theory ,FOS: Physical sciences ,Parton ,Stability (probability) ,Atomic and Molecular Physics, and Optics ,High Energy Physics - Phenomenology ,High Energy Physics - Phenomenology (hep-ph) ,Radiology, Nuclear Medicine and imaging ,High Energy Physics::Experiment ,Nucleon ,Nuclear Experiment ,Parametrization - Abstract
Matter and pressure distribution in hadrons are studied in a dual analytic model of generalized parton distributions with complex Regge trajectories. An original parametrization for pressure distribution in the nucleon is proposed ensuring its stability and compatible with the experimental data from the JLab accelerator., 15 pager, 6 figures
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- 2021
39. Testing parton distribution functions with <math><mi>t</mi></math>-channel single-top-quark production
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Tobias Neumann, John M. Campbell, and Zack Sullivan
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Physics ,Particle physics ,Top quark ,Hadron ,Nuclear Theory ,High Energy Physics::Phenomenology ,FOS: Physical sciences ,Parton ,Inelastic scattering ,High Energy Physics - Experiment ,Constraint (information theory) ,Moment (mathematics) ,High Energy Physics - Phenomenology ,High Energy Physics - Experiment (hep-ex) ,Distribution function ,High Energy Physics - Phenomenology (hep-ph) ,Consistency (statistics) ,High Energy Physics::Experiment - Abstract
The production of single top-quarks in the t-channel at hadron colliders imposes strong analytic constraints on parton distribution functions (PDFs) through its double deeply inelastic scattering (DDIS) form. We exploit this to provide novel consistency checks between LO, NLO and NNLO PDF fits and propose to include it as a constraint in future PDF fits. Furthermore, while it is well-known that the b-quark PDF is highly sensitive to the b-quark mass, we show that the treatment of this systematic uncertainty is still incomplete, fragmented or outright missing at the moment. Consequently, we conclude that the b-quark mass uncertainty is the dominant but so far broadly neglected theory uncertainty for this process., Comment: 6 pages, 4 figures; v2: matches published version in PRD
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- 2021
40. Resummation of Super-Leading Logarithms
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Matthias Neubert, Thomas Becher, and Ding Yu Shao
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High Energy Physics - Theory ,Physics ,Particle physics ,Logarithm ,010308 nuclear & particles physics ,Scattering ,530 Physics ,Hadron ,FOS: Physical sciences ,General Physics and Astronomy ,Parton ,Jet (particle physics) ,01 natural sciences ,High Energy Physics - Phenomenology ,High Energy Physics - Phenomenology (hep-ph) ,Amplitude ,High Energy Physics - Theory (hep-th) ,0103 physical sciences ,High Energy Physics::Experiment ,Resummation ,010306 general physics ,Lepton - Abstract
Jet cross sections at high-energy colliders exhibit intricate patterns of logarithmically enhanced higher-order corrections. In particular, so-called non-global logarithms emerge from soft radiation emitted off energetic partons inside jets. While this is a single-logarithmic effect at lepton colliders, at hadron colliders phase factors in the amplitudes lead to double-logarithmic corrections starting at four-loop order. This effect was discovered a long time ago, but not much is known about the higher-order behavior of these terms and their process dependence. We derive, for the first time, the all-order structure of these "super-leading logarithms" for generic $2\to l$ scattering processes at hadron colliders and resum them in closed form., Comment: 6 pages, 2 figures
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- 2021
41. Factorized approach to radiative corrections for inelastic lepton-hadron collisions
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Tiehui Liu, Wally Melnitchouk, Nobuo Sato, and Jian-Wei Qiu
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Physics ,Particle physics ,Nuclear Theory ,Scattering ,Hadron ,High Energy Physics::Phenomenology ,FOS: Physical sciences ,Parton ,Jet (particle physics) ,High Energy Physics - Experiment ,Nuclear Theory (nucl-th) ,High Energy Physics - Experiment (hep-ex) ,High Energy Physics - Phenomenology ,High Energy Physics - Phenomenology (hep-ph) ,Distribution function ,Radiative transfer ,Physics::Accelerator Physics ,High Energy Physics::Experiment ,Nuclear Experiment (nucl-ex) ,Resummation ,Nuclear Experiment ,Lepton - Abstract
We propose a factorized approach to QED radiative corrections for inclusive and semi-inclusive deep-inelastic scattering to systematically account for QED and QCD radiation contributions to both processes on equal footing. This is achieved by utilizing factorization to resum logarithmically enhanced QED radiation into universal lepton distribution and fragmentation (or jet) functions. Numerical simulations suggest that the QED effects induced by the rotational distortion of the hadron transverse momentum, arising from the mismatch between the experimental Breit frame and the true photon-hadron frame, can be as large as 50\% for moderate $Q$, and become increasingly important for large transverse momenta. Our framework provides a uniform treatment of radiative effects for extracting three-dimensional hadron structure from high-energy lepton-hadron scattering at current and future facilities, such as the Electron-Ion Collider., 6 pages, 3 figures, accepted for publication in Phys. Rev. D
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- 2021
42. Matching NNLO predictions to parton showers using N3LL color-singlet transverse momentum resummation in geneva
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Alessandro Gavardi, Stefan Kallweit, Davide Napoletano, Alessandro Broggio, Matthew A. Lim, Luca Rottoli, Riccardo Nagar, Simone Alioli, and Christian Bauer
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Physics ,Particle physics ,Matching (statistics) ,010308 nuclear & particles physics ,0103 physical sciences ,Transverse momentum ,Parton ,Singlet state ,Resummation ,010306 general physics ,01 natural sciences - Published
- 2021
43. Cos(2ϕh) asymmetry in J/ψ production in unpolarized ep collision
- Author
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Mariyah Siddiqah, Asmita Mukherjee, and Raj Kishore
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Quantum chromodynamics ,Physics ,Particle physics ,Proton ,Octet ,media_common.quotation_subject ,Nuclear Theory ,High Energy Physics::Phenomenology ,Parton ,Asymmetry ,Gluon ,Distribution function ,High Energy Physics::Experiment ,Production (computer science) ,Nuclear Experiment ,media_common - Abstract
We present a calculation of the $\mathrm{cos}(2{\ensuremath{\phi}}_{h})$ asymmetry in $J/\ensuremath{\psi}$ production in electron-proton collisions at the future electron-ion collider (EIC), a useful channel to probe the transverse momentum dependent gluon distribution functions also known as gluon transverse momentum dependent parton distributions (TMDs). The dominant subprocess for the $J/\ensuremath{\psi}$ production is the virtual-photon-gluon fusion process ${\ensuremath{\gamma}}^{*}+g\ensuremath{\rightarrow}J/\ensuremath{\psi}+g$. The production of $J/\ensuremath{\psi}$ is calculated in the nonrelativistic quantum chromodynamics framework with the inclusion of both color singlet and color octet contributions. Numerical estimates of the $\mathrm{cos}(2{\ensuremath{\phi}}_{h})$ asymmetry are given in the kinematical region to be accessed by the future EIC. The asymmetry depends on the parametrization of the gluon TMDs, as well as on the long distance matrix elements. We use both Gaussian-type parametrization and the McLerran-Venugopalan model for the TMDs in the kinematical region of small $x$, where the gluons play a dominant role. The asymmetry may be useful to probe the ratio of the linearly-polarized and the unpolarized gluon distribution in the proton.
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- 2021
44. Measurement of the charge asymmetry of electrons from the decays of W bosons produced in pp¯ collisions at s=1.96 TeV
- Author
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M. Kurata, Andrew Ivanov, Daniela Bortoletto, P. E. Karchin, A. Castro, V. Thukral, D. Goldin, G. Piacentino, M. Kambeitz, J. Keung, A. Mukherjee, Pavol Bartos, G. Manca, T. A. Schwarz, Monica D'Onofrio, M. Rescigno, Justin Pilot, Rainer Wallny, Mario Campanelli, V. V. Glagolev, H. Gerberich, G. Chlachidze, B. Auerbach, S. Donati, R. F. Harr, K. R. Bland, Kenichi Hatakeyama, D. Tonelli, T. Yang, Y. C. Yang, C. Paus, M. Franklin, Chris Hays, A. Semenov, Mark Kruse, Alison Lister, C. Plager, J. Nett, Stefano Giagu, J. D. Lewis, Hirokazu Miyake, S. Amerio, Alberto Annovi, T. Tomura, Jian Tang, P. Garosi, I. Redondo Fernández, O. Norniella, R. Vilar, C. M. Ginsburg, J. E. Kim, S. H. Kim, K. K. Joo, Scott Wilbur, Nicola D'Ascenzo, J. A. Appel, M. J. Shochet, A. Hocker, J. S. Conway, M. Iori, C. Pagliarone, T. Rodriguez, Javier Cuevas, Hong Ye Song, A. Simonenko, G. Pauletta, V. A. Giakoumopoulou, Virgil E Barnes, G. Volpi, Gervasio Gomez, D. W. Jang, V. Papadimitriou, J. C. Freeman, P. F. Shepard, S. H. Oh, P. J. Bussey, D. Waters, B. Di Ruzza, A. Ruiz, Adrian Buzatu, Y. Nagai, D. J. Cox, C. Galloni, T. Nigmanov, M. Gold, Koji Yamamoto, Ulrich Husemann, A. Manousakis-Katsikakis, N. Moggi, P. K. Teng, Matthew Jones, D. Yamato, A. Savoy-Navarro, Yuji Sudo, Andrew Beretvas, Giuseppe Latino, D. Mietlicki, Jonathan L. Rosner, T. Miao, D. Chokheli, G. Punzi, Itsuo Nakano, I. Yu, Alan Garfinkel, Marcelo Vogel, Fabrizio Margaroli, J. R. Smith, P. Schlabach, P. Totaro, B. Jayatilaka, Henry J. Frisch, K. Gibson, Matteo Cremonesi, Fumihiko Ukegawa, Xin Wu, Th. Müller, K. Sliwa, J. N. Bellinger, Y. D. Oh, G. Flanagan, D. Torretta, Viviana Cavaliere, T. Wright, T. Aaltonen, L. Ristori, Y. Takeuchi, W.F. Badgett, Peter Wagner, W. Ashmanskas, S. Lockwitz, Sudhir Malik, M. Vidal, Marco Trovato, H. S. Budd, W. Parker, L. Brigliadori, Keunchang Cho, A. Elagin, A. Bocci, Jay Dittmann, Stephan Lammel, E. J. Jeon, T. Kuhr, F. Canelli, K. Takemasa, V. Saveliev, S. Moed, Kiminori Kondo, M. J. Kim, M. M. Deninno, D. H. Kim, A. Loginov, A. B. Wicklund, Erik Brücken, E. E. Schmidt, A. Cerri, D. Stentz, H. S. Kim, W. Ketchum, E. Thomson, J. Antos, Prabhakar Palni, C. Mesropian, S. Y. Noh, Kazuhiko Hara, S. Carrillo, E. Gramellini, Giovanni Bellettini, M. E. Mattson, S. R. Hahn, E. Palencia, F. Vázquez, A. Di Canto, Maxim Goncharov, J. Asaadi, E. James, Naoki Kimura, A. Kasmi, V. Vecchio, L. Demortier, O. Gonzalez Lopez, S. Leo, A. Mazzacane, J. Vizán, Luca Scodellaro, V. Rusu, M. Lancaster, S. Torre, Fedor Prokoshin, Sandra Leone, A. R. Clark, P. Giromini, Koji Sato, Anna Zanetti, Chen Zhou, J. Lueck, Peter Wittich, P. B. Renton, M. Mussini, Stefano Camarda, T. Harrington-Taber, Y. Zeng, K. Matera, T. Okusawa, L. Pondrom, S. Z. Shalhout, A. Mitra, W. C. Wester, R. Forrest, Y. Seiya, R. McNulty, M. Hare, A. Sukhanov, Sally Seidel, Federico Sforza, Manfred Paulini, G.V. Velev, D. Cruz, W. K. Sakumoto, M. H. Kirby, Elisabetta Pianori, Jane Nachtman, S. Wolbers, A. Pranko, Kevin Burkett, M. Tecchio, James Russ, Kohei Yorita, Stefano Zucchelli, Maxwell Chertok, Caterina Vernieri, Kai Yi, J. Huston, Luigi Marchese, H. Wolfmeister, Y. Sakurai, Michal Kreps, C. Grosso-Pilcher, Y. K. Kim, D. Lucchesi, J. Lys, R. Roser, Ryan Christopher Edgar, P. Murat, T. Liu, M. Shimojima, Fabrizio Scuri, A. Driutti, John Strologas, Lucio Cerrito, L. Nodulman, P. Marino, F. Devoto, Ziqing Hong, Roger Moore, Paul Wilson, Duncan Carlsmith, F. Ptohos, H. H. Williams, Q. Liu, L. B. Oakes, M. J. Morello, F. D. Snider, R. St. Denis, K. Ebina, A. Boveia, J. Y. Han, J. Boudreau, G. P. Yeh, G. Introzzi, A. Robson, R. Orava, A. Anastassov, Christopher Clarke, Walter Hopkins, G. Lungu, A. Napier, Rodolfo Carosi, S. M. Wang, A. T. Laasanen, C. A. Cox, T. Bae, R. D. Field, K. Potamianos, A. Artikov, F. Azfar, Tomoko Yoshida, Sergo Jindariani, U. K. Yang, T. J. Phillips, S. B. Kim, J. S. H. Lee, A. Isgrò, J. Kroll, R. Culbertson, F. Happacher, Matthew Herndon, Andrea Di Luca, J. Budagov, A. Bhatti, S. Rolli, Benjamin Kilminster, Barry Blumenfeld, Roman Lysak, I. Suslov, Sinead Farrington, S. Uozumi, K. Goulianos, Manfredi Ronzani, Aristotle Calamba, S. Poprocki, D. J. Kong, C. Vellidis, J. P. Fernández Ramos, P. de Barbaro, B. Carls, V. Sorin, Franco Bedeschi, P. Lukens, A. Bodek, D. Toback, M. Stancari, Yongsun Kim, A. Golossanov, M. Corbo, Y. C. Chen, S. Tokar, L. Santi, Giorgio Chiarelli, Emanuele Michielin, Mahmoud I. Hussein, Patrizia Barria, B. A. Barnett, T. R. Junk, Teruki Kamon, P. Mazzanti, Bruno Casal, D. Cauz, P. Mehtala, E. Gerchtein, J. Yoh, S. Y. Jun, Matteo Bauce, Antonio Limosani, Robin Erbacher, M. Datta, W-M. Yao, A. T. Goshaw, C. S. Moon, M. Cordelli, G. Busetto, Brian L Winer, D. Glenzinski, S. R. Hou, S. Errede, R. Madrak, J. Naganoma, Giorgio Apollinari, F. Rimondi, Tetsuo Arisawa, B. Esham, D. P. Benjamin, Joachim Heinrich, A. K. Mehta, G. B. Yu, S. Behari, Y. Funakoshi, Y. Kato, J. Guimaraes Da Costa, K. T. Pitts, I. V. Gorelov, Zhenbin Wu, K. Tollefson, Pierfrancesco Butti, A. V. Kotwal, I. Shreyber-Tecker, D. Amidei, Jacobo Konigsberg, Elliot Lipeles, R. E. Hughes, Daniel Whiteson, F. Ruffini, A. Aurisano, J. S. Wilson, N. Giokaris, J. Thom, Kevin Lannon, M. D'Errico, M. E. Convery, Guillelmo Gomez-Ceballos, L. Ortolan, Paul Lujan, Massimo Casarsa, M. Dorigo, P. Catastini, C. Bromberg, A. Barbaro-Galtieri, T. G. Shears, H. S. Lee, and Paolo Maestro
- Subjects
Physics ,Particle physics ,Proton ,010308 nuclear & particles physics ,media_common.quotation_subject ,High Energy Physics::Phenomenology ,Tevatron ,Parton ,7. Clean energy ,01 natural sciences ,Asymmetry ,law.invention ,law ,Pseudorapidity ,0103 physical sciences ,Physics::Accelerator Physics ,High Energy Physics::Experiment ,Fermilab ,Nuclear Experiment ,010306 general physics ,Collider ,Collider Detector at Fermilab ,media_common - Abstract
At the Fermilab Tevatron proton-antiproton ($p\bar{p}$) collider, high-mass electron-neutrino ($e\nu$) pairs are produced predominantly in the process $p \bar{p} \rightarrow W(\rightarrow e\nu) + X$. The asymmetry of the electron and positron yield as a function of their pseudorapidity constrain the slope of the ratio of the $u$- to $d$-quark parton distributions versus the fraction of the proton momentum carried by the quarks. This paper reports on the measurement of the electron-charge asymmetry using the full data set recorded by the Collider Detector at Fermilab in 2001--2011 and corresponding to 9.1~fb$^{-1}$ of integrated luminosity. The measurement significantly improves the precision of the Tevatron constraints on the parton-distribution functions of the proton. Numerical tables of the measurement are provided.
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- 2021
45. Matching N3LO QCD calculations to parton showers
- Author
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Stefan Prestel
- Subjects
Physics ,Quantum chromodynamics ,Nuclear and High Energy Physics ,Matching (statistics) ,Particle physics ,FOS: Physical sciences ,Parton ,QC770-798 ,High Energy Physics - Phenomenology ,Alpha (programming language) ,High Energy Physics - Phenomenology (hep-ph) ,Nuclear and particle physics. Atomic energy. Radioactivity ,Perturbative QCD ,High Energy Physics::Experiment ,Resummation ,Differential (infinitesimal) ,Event (particle physics) ,Lepton ,Event generator - Abstract
The search for new interactions and particles in high-energy collider physics relies on precise background predictions. This has led to many advances in combining precise fixed-order cross-section calculations with detailed event generator simulations. In recent years, fixed-order QCD calculations of inclusive cross sections at N3LO precision have emerged, followed by an impressive progress at producing differential results. Once differential results become publicly available, it would be prudent to embed these into event generators to allow the community to leverage these advances. This note offers some concrete thoughts on ME+PS matching at third order in QCD. As a method for testing these thoughts, a toy calculation of $e^+e^-\rightarrow u \bar u$ at $\mathcal{O}(\alpha_s^3)$ is constructed, and combined with an event generator through unitary matching. The toy implementation may serve also as blueprint for high-precision QCD predictions at future lepton colliders. As a byproduct of the N3LO matching formula, a new NNLO+PS formula for processes with "additional" jets is obtained., Comment: 19 pages main text + detailed appendices
- Published
- 2021
46. Spin asymmetries in electron-jet production at the future electron ion collider
- Author
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Ding Yu Shao, F. Zhao, Zhong-Bo Kang, and Kyle Lee
- Subjects
Nuclear and High Energy Physics ,Particle physics ,Nuclear Theory ,FOS: Physical sciences ,Parton ,Electron ,QC770-798 ,law.invention ,High Energy Physics - Experiment ,Nuclear Theory (nucl-th) ,High Energy Physics - Experiment (hep-ex) ,High Energy Physics - Phenomenology (hep-ph) ,law ,Nuclear and particle physics. Atomic energy. Radioactivity ,Jets ,Nuclear Experiment (nucl-ex) ,Collider ,Nuclear Experiment ,Spin-½ ,Physics ,Jet (fluid) ,Scattering ,High Energy Physics::Phenomenology ,HERA ,QCD Phenomenology ,High Energy Physics - Phenomenology ,Distribution function ,High Energy Physics::Experiment - Abstract
We study all the possible spin asymmetries that can arise in back-to-back electron-jet production, $ep\rightarrow e+\text{jet}+X$, as well as the associated jet fragmentation process, $ep\rightarrow e+ \text{jet} (h)+X$, in electron-proton collisions. We derive the factorization formalism for these spin asymmetries and perform the corresponding phenomenology for the kinematics relevant to the future electron ion collider. In the case of unpolarized electron-proton scattering, we also give predictions for azimuthal asymmetries for the HERA experiment. This demonstrates that electron-jet production is an outstanding process for probing unpolarized and polarized transverse momentum dependent parton distribution functions and fragmentation functions., 46 pages, 10 figures, 5 tables
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- 2021
47. Three-photon productions within the $$k_t$$ <math> <msub> <mi>k</mi> <mi>t</mi> </msub> </math> -factorization at the LHC
- Author
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Somayeh Rezaie, Ramin Kord Valeshabadi, and M. Modarres
- Subjects
Physics ,Particle physics ,Photon ,Large Hadron Collider ,Physics and Astronomy (miscellaneous) ,Parton ,QC770-798 ,Astrophysics ,QB460-466 ,Distribution function ,Cover (topology) ,Factorization ,Nuclear and particle physics. Atomic energy. Radioactivity ,Production (computer science) ,Engineering (miscellaneous) ,Event generator - Abstract
Recently, the ATLAS data of isolated three-photon production showed that the next-to-leading order (NLO) collinear factorization is not enough to describe experimental data. Therefore, one needs to calculate the cross section beyond the NLO, and as showed later, these data can be well described by the NNLO calculation within the collinear factorization framework. However, it is shown that the $$k_t$$ k t -factorization can be quite successful in describing exclusive and high energy collision processes, henceforth we decided to calculate isolated three-photon production within this framework. In this work we use the Martin, Ryskin, and Watt unintegrated parton distribution functions (MRW UPDFs) at LO and NLO levels, in addition to parton branching (PB) UPDFs in order to calculate cross section which we utilize the KATIE parton level event generator. It will be shown that in contrast to collinear factorization, the $$k_t$$ k t -factorization can describe quiet well the three-photon production ATLAS data. Interestingly our results using the NLO-MRW and PB UPDFs can cover the data within their uncertainty bands, similar to the NNLO collinear results.
- Published
- 2021
48. Nucleon Tomography and Generalized Parton Distribution at Physical Pion Mass from Lattice QCD
- Author
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Huey-Wen Lin
- Subjects
Physics ,Quark ,Particle physics ,Isovector ,Nuclear Theory ,High Energy Physics::Lattice ,High Energy Physics - Lattice (hep-lat) ,FOS: Physical sciences ,General Physics and Astronomy ,Parton ,Lattice QCD ,Nuclear Theory (nucl-th) ,Renormalization ,High Energy Physics - Phenomenology ,High Energy Physics - Phenomenology (hep-ph) ,Pion ,High Energy Physics - Lattice ,High Energy Physics::Experiment ,Nucleon ,Minimal subtraction scheme ,Nuclear Experiment - Abstract
We present the first lattice calculation of the nucleon isovector unpolarized generalized parton distribution (GPD) at the physical pion mass using a lattice ensemble with 2+1+1 flavors of highly improved staggered quarks (HISQ) generated by MILC Collaboration, with lattice spacing $a\approx 0.09$~fm and volume $64^3\times 96$. We use momentum-smeared sources to improve the signal at nucleon boost momentum $P_z \approx 2.2$ GeV, and report results at nonzero momentum transfers in $[0.2,1.0]\text{ GeV}^2$. Nonperturbative renormalization in RI/MOM scheme is used to obtain the quasi-distribution before matching to the lightcone GPDs. The three-dimensional distributions $H(x,Q^2)$ and $E(x,Q^2)$ at $\xi=0$ are presented, along with the three-dimensional nucleon tomography and impact-parameter--dependent distribution for selected Bjorken $x$ at $\mu=3$ GeV in $\overline{\text{MS}}$ scheme., Comment: Typos fixed. Removed data using twisted-boundary conditions
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- 2021
49. Relations between generalized parton distributions and transverse momentum dependent parton distributions
- Author
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Dipankar Chakrabarti, Poonam Choudhary, Bheemsehan Gurjar, Asmita Mukherjee, and Pulak Talukdar
- Subjects
Quantum chromodynamics ,Physics ,Quark ,Angular momentum ,Particle physics ,High Energy Physics::Lattice ,High Energy Physics::Phenomenology ,Structure (category theory) ,FOS: Physical sciences ,Parton ,Function (mathematics) ,High Energy Physics - Phenomenology ,High Energy Physics - Phenomenology (hep-ph) ,Transverse momentum ,High Energy Physics::Experiment ,Nuclear Experiment - Abstract
We investigate the relations between transverse momentum dependent parton distributions (TMDs) and generalized parton distributions (GPDs) in a light-front quark-diquark model motivated by soft wall AdS/QCD. Many relations are found to have similar structure in different models. It is found that a relation between the Sivers function and the GPD $E_q$ can be obtained in this model in terms of a lensing function. The quark orbital angular momentum is calculated and the results are compared with the results in other similar models. Implications of the results are discussed. Relations among different TMDs in the model are also presented., minor changes, errors in some references are corrected
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- 2021
50. Bayesian Monte Carlo extraction of the sea asymmetry with SeaQuest and STAR data
- Author
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Wolodymyr Melnitchouk, Christopher Cocuzza, Nobuo Sato, and Andreas Metz
- Subjects
Quantum chromodynamics ,Physics ,Particle physics ,Nuclear Theory ,High Energy Physics::Lattice ,Star (game theory) ,media_common.quotation_subject ,High Energy Physics::Phenomenology ,Monte Carlo method ,FOS: Physical sciences ,Parton ,Asymmetry ,High Energy Physics - Experiment ,Nuclear Theory (nucl-th) ,High Energy Physics - Experiment (hep-ex) ,High Energy Physics - Phenomenology ,High Energy Physics - Phenomenology (hep-ph) ,High Energy Physics::Experiment ,Production (computer science) ,Fermilab ,Nuclear Experiment ,Chiral symmetry breaking ,media_common - Abstract
We perform a global QCD analysis of unpolarized parton distributions within a Bayesian Monte Carlo framework, including the new $W$-lepton production data from the STAR Collaboration at RHIC and Drell-Yan di-muon data from the SeaQuest experiment at Fermilab. We assess the impact of these two new measurements on the light antiquark sea in the proton, and the $\bar{d}-\bar{u}$ asymmetry in particular. The SeaQuest data are found to significantly reduce the uncertainty on the $\bar{d}/\bar{u}$ ratio at large parton momentum fractions $x$, strongly favoring an enhanced $\bar{d}$ sea up to $x \approx 0.4$, in general agreement with nonperturbative calculations based on chiral symmetry breaking in QCD., 10 pages, 8 figures
- Published
- 2021
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