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Related papers: The photon PDF from high-mass Drell-Yan data at th…

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We present the MSHT20qed set of parton distribution functions (PDFs). These are obtained from the MSHT20 global analysis via a refit including QED corrections to the DGLAP evolution at ${\cal O}(\alpha),{\cal O}(\alpha\alpha_S)$ and ${\cal…

High Energy Physics - Phenomenology · Physics 2022-02-16 T. Cridge , L. A. Harland-Lang , A. D. Martin , R. S. Thorne

Parton Density Functions (PDFs) and their uncertainties are extremely important topics for both the Tevatron and the LHC. Experiments at the Tevatron can enhance this knowledge not only by constraining the PDF fits, but also by developing…

High Energy Physics - Phenomenology · Physics 2007-05-23 D Bourilkov , R C Group , M R Whalley

We re-examine the current state of the art for the calculation of photon-initiated processes at the LHC, as formulated in terms of a photon PDF in the proton that may be determined rather precisely from the known proton structure functions.…

High Energy Physics - Phenomenology · Physics 2021-10-06 L. A. Harland-Lang

A search for heavy long-lived multi-charged particles is performed using the ATLAS detector at the LHC. Data with an integrated luminosity of 36.1 fb$^{-1}$ collected in 2015 and 2016 from proton-proton collisions at $\sqrt{s}$ = 13 TeV are…

High Energy Physics - Experiment · Physics 2019-03-27 ATLAS Collaboration

The accurate determination of the Parton Distribution Functions (PDFs) of the proton is an essential ingredient of the Large Hadron Collider (LHC) program. PDF uncertainties impact a wide range of processes, from Higgs boson…

We show that high energy measurements of Drell-Yan at the LHC can serve as electroweak precision tests. Dimension-6 operators, from the Standard Model Effective Field Theory, modify the high energy behavior of electroweak gauge boson…

High Energy Physics - Phenomenology · Physics 2017-06-27 Marco Farina , Giuliano Panico , Duccio Pappadopulo , Joshua T. Ruderman , Riccardo Torre , Andrea Wulzer

In this work we directly fit the QCD dimensional transmutation parameter, ${\Lambda _{\overline {MS} }}$, to experimental data of Drell-Yan (DY) observables. For this purpose we first obtain the evolution of transverse momentum dependent…

High Energy Physics - Phenomenology · Physics 2017-03-22 R. Taghavi , A. Mirjalili

We compute for the first time the lepton-pair rapidity distribution in the photon-mediated Drell-Yan process to next-to-next-to-next-to-leading order (N$^3$LO) in QCD. The calculation is based on the qT-subtraction method, suitably extended…

High Energy Physics - Phenomenology · Physics 2022-02-04 Xuan Chen , Thomas Gehrmann , Nigel Glover , Alexander Huss , Tong-Zhi Yang , Hua Xing Zhu

Massive lepton-pair production, the Drell-Yan process, should be a good source of independent constraints on the gluon density, free from the experimental and theoretical complications of photon isolation that beset studies of prompt photon…

High Energy Physics - Phenomenology · Physics 2007-05-23 E. L. Berger , M. Klasen

Results of a search for the pair production of photon-jets$-$collimated groupings of photons$-$in the ATLAS detector at the Large Hadron Collider are reported. Highly collimated photon-jets can arise from the decay of new, highly boosted…

High Energy Physics - Experiment · Physics 2019-03-14 ATLAS Collaboration

We present the analytic computation of leading high-energy logarithms of the inclusive Drell-Yan and vector boson production cross-section. We also study the phenomenological relevance of the high-energy corrections for Drell-Yan processes…

High Energy Physics - Phenomenology · Physics 2009-06-26 Simone Marzani , Richard D. Ball

We present a systematic comparison of theoretical predictions and various high-precision experimental measurements, specifically of differential cross sections performed by the LHC run II for Drell-Yan gauge boson, top-quark pair,…

The double differential cross sections of the Drell-Yan lepton pair ($\ell^+\ell^-$, dielectron or dimuon) production are measured as functions of the invariant mass $m_{\ell\ell}$, transverse momentum $p_\mathrm{T}(\ell\ell)$, and…

High Energy Physics - Experiment · Physics 2023-07-21 CMS Collaboration

The direct photon spectrum is computed to the highest currently available precision and compared to ATLAS data from 8 TeV collisions at the LHC. The prediction includes threshold resummation at next-to-next-to-next-to-leading logarithmic…

High Energy Physics - Phenomenology · Physics 2016-09-21 Matthew D. Schwartz

We present a detailed study of the charged current Drell-Yan process, which includes the exact O(alpha) electroweak corrections properly matched with leading-log effects due to multiple-photon emission, as required by the experiments at the…

High Energy Physics - Phenomenology · Physics 2009-11-11 C. M. Carloni Calame , G. Montagna , O. Nicrosini , A. Vicini

The effect of full $7$ sets of LHC ATLAS jet cross sections data at $ \sqrt{s} = 7$ TeV on the proton parton distribution functions (PDFs) up to next-to-next-to-next-to-leading order (NNNLO or N3LO) corrections is investigated for the first…

High Energy Physics - Phenomenology · Physics 2020-05-05 A. Vafaee , K. Javidan , A. B. Shokouhi

The COMPASS Collaboration performed measurements of the Drell-Yan process in 2015 and 2018 using a 190 GeV/c $\pi^{-}$ beam impinging on a transversely polarised ammonia target. Combining the data of both years, we present final results on…

High Energy Physics - Experiment · Physics 2024-01-01 G. D. Alexeev , M. G. Alexeev , C. Alice , A. Amoroso , V. Andrieux , V. Anosov , K. Augsten , W. Augustyniak , C. D. R. Azevedo , B. Badelek , J. Barth , R. Beck , J. Beckers , Y. Bedfer , J. Bernhard , M. Bodlak , F. Bradamante , A. Bressan , W. -C. Chang , C. Chatterjee , M. Chiosso , A. G. Chumakov , S. -U. Chung , A. Cicuttin , P. M. M. Correia , M. L. Crespo , D. D'Ago , S. Dalla Torre , S. S. Dasgupta , S. Dasgupta , F. Delcarro , I. Denisenko , O. Yu. Denisov , S. V. Donskov , N. Doshita , Ch. Dreisbach , W. Dunnweber , R. R. Dusaev , D. Ecker , D. Eremeev , P. Faccioli , M. Faessler , M. Finger , M. Finger , H. Fischer , K. J. Flothner , W. Florian , J. M. Friedrich , V. Frolov , L. G. Garcia Ordonez , F. Gautheron , O. P. Gavrichtchouk , S. Gerassimov , J. Giarra , D. Giordano , A. Grasso , A. Gridin , M. Grosse Perdekamp , B. Grube , M. Gruner , A. Guskov , P. Haas , D. von Harrach , R. Heitz , M. Hoffmann , N. d'Hose , C. -Y. Hsieh , S. Huber , S. Ishimoto , A. Ivanov , T. Iwata , V. Jary , R. Joosten , E. Kabuss , F. Kaspar , A. Kerbizi , B. Ketzer , A. Khatun , G. V. Khaustov , F. Klein , J. H. Koivuniemi , V. N. Kolosov , K. Kondo Horikawa , I. Konorov , V. F. Konstantinov , A. Yu. Korzenev , A. M. Kotzinian , O. M. Kouznetsov , A. Koval , Z. Kral , F. Krinner , F. Kunne , K. Kurek , R. P. Kurjata , A. Kveton , K. Lavickova , S. Levorato , Y. -S. Lian , J. Lichtenstadt , P. -J. Lin , R. Longo , V. E. Lyubovitskij , A. Maggiora , A. Magnon , N. Makke , G. K. Mallot , A. Maltsev , A. Martin , J. Marzec , J. Matousek , T. Matsuda , G. Mattson , C. Menezes Pires , F. Metzger , M. Meyer , W. Meyer , Yu. V. Mikhailov , M. Mikhasenko , E. Mitrofanov , D. Miura , Y. Miyachi , R. Molina , A. Moretti , A. Nagaytsev , D. Neyret , M. Niemiec , J. Novy , W. -D. Nowak , G. Nukazuka , A. G. Olshevsky , M. Ostrick , D. Panzieri , B. Parsamyan , S. Paul , H. Pekeler , J. -C. Peng , M. Pesek , D. V. Peshekhonov , M. Peskova , S. Platchkov , J. Pochodzalla , V. A. Polyakov , M. Quaresma , C. Quintans , G. Reicherz , C. Riedl , D. I. Ryabchikov , A. Rychter , A. Rymbekova , V. D. Samoylenko , A. Sandacz , S. Sarkar , T. Savada , I. A. Savin , G. Sbrizzai , H. Schmieden , A. Selyunin , K. Sharko , L. Sinha , D. Spulbeck , A. Srnka , M. Stolarski , M. Sulc , H. Suzuki , S. Tessaro , F. Tessarotto , A. Thiel , F. Tosello , A. Townsend , T. Triloki , V. Tskhay , B. Valinoti , B. M. Veit , J. F. C. A. Veloso , B. Ventura , A. Vijayakumar , M. Virius , M. Wagner , S. Wallner , K. Zaremba , M. Zavertyaev , M. Zemko , E. Zemlyanichkina , M. Ziembicki

The dilepton decay channels provide clean signatures and are an ideal hunting ground for high mass resonant, like Z', or non-resonant, like contact interactions or extra dimensions, searches at the LHC. The production of high invariant mass…

High Energy Physics - Phenomenology · Physics 2017-01-24 Dimitri Bourilkov

We determine the strong coupling from high-energy data for the Drell-Yan (DY) process and top-quark hadro-production collected at the Large Hadron Collider and the Tevatron combined with the world data on deep-inelastic scattering (DIS) and…

High Energy Physics - Phenomenology · Physics 2025-10-27 S. Alekhin , M. V. Garzelli , S. Moch , O. Zenaiev

We perform the next-to-next-leading-order (NNLO) QCD global fit of PDFs using inclusive charged-lepton and neutrino DIS data down to Q = 1 GeV. We also consider the data on neutrino-nucleon dimuon production, that allows us to disentangle…

High Energy Physics - Phenomenology · Physics 2008-10-28 S. Alekhin , S. Kulagin , R. Petti