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We present a determination of the strong coupling $\alpha_s(m_Z)$ from a global dataset including both fixed-target and collider data from deep-inelastic scattering and a variety of hadronic processes, with a simultaneous determination of…

We present the first computation of next-to-next-to-leading order (NNLO) pure QED and mixed QCD$\otimes$QED corrections to unpolarized and polarized semi-inclusive deep-inelastic scattering (SIDIS). Building on our previous NNLO QCD…

High Energy Physics - Phenomenology · Physics 2025-10-22 Saurav Goyal , Roman N. Lee , Sven-Olaf Moch , Vaibhav Pathak , V. Ravindran

In this paper we present a next-to-next-to-leading order (NNLO) calculation of the process $pp\rightarrow \gamma\gamma$ that we have implemented into the parton level Monte Carlo code MCFM. We do not find agreement with the previous…

High Energy Physics - Phenomenology · Physics 2021-09-15 John M. Campbell , R. Keith Ellis , Ye Li , Ciaran Williams

The HERAPDF2.0 ensemble of parton distribution functions (PDFs) was introduced in 2015. The final stage is presented, a next-to-next-to-leading-order (NNLO) analysis of the HERA data on inclusive deep inelastic $ep$ scattering together with…

High Energy Physics - Experiment · Physics 2021-12-03 H1 , ZEUS Collaborations , : , I. Abt , R. Aggarwal , V. Andreev , M. Arratia , V. Aushev , A. Baghdasaryan , A. Baty , K. Begzsuren , O. Behnke , A. Belousov , A. Bertolin , I. Bloch , V. Boudry , G. Brandt , I. Brock , N. H. Brook , R. Brugnera , A. Bruni , A. Buniatyan , P. J. Bussey , L. Bystritskaya , A. Caldwell , A. J. Campbell , K. B. Cantun Avila , C. D. Catterall , K. Cerny , V. Chekelian , Z. Chen , J. Chwastowski , J. Ciborowski , R. Ciesielski , J. G. Contreras , A. M. Cooper-Sarkar , M. Corradi , L. Cunqueiro Mendez , J. Currie , J. Cvach , J. B. Dainton , K. Daum , R. K. Dementiev , A. Deshpande , C. Diaconu , S. Dusini , G. Eckerlin , S. Egli , E. Elsen , L. Favart , A. Fedotov , J. Feltesse , J. Ferrando , M. Fleischer , A. Fomenko , B. Foster , C. Gal , E. Gallo , D. Gangadharan , A. Garfagnini , J. Gayler , A. Gehrmann-De Ridder , T. Gehrmann , A. Geiser , L. K. Gladilin , E. W. N. Glover , L. Goerlich , N. Gogitidze , Yu. A. Golubkov , M. Gouzevitch , C. Grab , T. Greenshaw , G. Grindhammer , G. Grzelak , C. Gwenlan , D. Haidt , R. C. W. Henderson , J. Hladký , D. Hochman , D. Hoffmann , R. Horisberger , T. Hreus , F. Huber , A. Huss , P. M. Jacobs , M. Jacquet , T. Janssen , N. Z. Jomhari , A. W. Jung , H. Jung , I. Kadenko , M. Kapichine , U. Karshon , J. Katzy , P. Kaur , C. Kiesling , R. Klanner , M. Klein , U. Klein , C. Kleinwort , H. T. Klest , R. Kogler , I. A. Korzhavina , P. Kostka , N. Kovalchuk , J. Kretzschmar , D. Krücker , K. Krüger , M. Kuze , M. P. J. Landon , W. Lange , P. Laycock , S. H. Lee , B. B. Levchenko , S. Levonian , A. Levy , W. Li , J. Lin , K. Lipka , B. List , J. List , B. Lobodzinski , B. Löhr , E. Lohrmann , O. R. Long , A. Longhin , F. Lorkowski , O. Yu. Lukina , I. Makarenko , E. Malinovski , J. Malka , H. -U. Martyn , S. Masciocchi , S. J. Maxfield , A. Mehta , A. B. Meyer , J. Meyer , S. Mikocki , V. M. Mikuni , M. M. Mondal , T. Morgan , A. Morozov , K. Mueller , B. Nachman , K. Nagano , J. D. Nam , Th. Naumann , P. R. Newman , C. Niebuhr , J. Niehues , G. Nowak , J. E. Olsson , Yu. Onishchuk , D. Ozerov , S. Park , C. Pascaud , G. D. Patel , E. Paul , E. Perez , A. Petrukhin , I. Picuric , I. Pidhurskyi , J. Pires , D. Pitzl , R. Polifka , A. Polini , S. Preins , M. Przybycień , A. Quintero , K. Rabbertz , V. Radescu , N. Raicevic , T. Ravdandorj , P. Reimer , E. Rizvi , P. Robmann , R. Roosen , A. Rostovtsev , M. Rotaru , M. Ruspa , D. P. C. Sankey , M. Sauter , E. Sauvan , S. Schmitt , B. A. Schmookler , U. Schneekloth , L. Schoeffel , A. Schöning , T. Schörner-Sadenius , F. Sefkow , I. Selyuzhenkov , M. Shchedrolosiev , L. M. Shcheglova , S. Shushkevich , I. O. Skillicorn , W. Słomiński , A. Solano , Y. Soloviev , P. Sopicki , D. South , V. Spaskov , A. Specka , L. Stanco , M. Steder , N. Stefaniuk , B. Stella , U. Straumann , C. Sun , B. Surrow , M. R. Sutton , T. Sykora , P. D. Thompson , K. Tokushuku , D. Traynor , B. Tseepeldorj , Z. Tu , O. Turkot , T. Tymieniecka , A. Valkárová , C. Vallée , P. Van Mechelen , A. Verbytskyi , W. A. T. Wan Abdullah , D. Wegener , K. Wichmann , M. Wing , E. Wünsch , S. Yamada , Y. Yamazaki , J. Žáček , A. F. Żarnecki , O. Zenaiev , J. Zhang , Z. Zhang , R. Žlebčík , H. Zohrabyan , F. Zomer

In this review, we discuss the results on the parton-to-pion fragmentation functions obtained in a combined NLO fit to data of single-inclusive hadron production in electron-positron annihilation, proton-proton collisions, and…

High Energy Physics - Phenomenology · Physics 2016-11-23 R. J. Hernández-Pinto , M. Epele , D. de Florian , R. Sassot , M. Stratmann

An analytical solution based on the Laplace transformation technique for the DGLAP evolution equations is presented at next-to-leading order accuracy in perturbative QCD. This technique is also applied to extract the analytical solution for…

High Energy Physics - Phenomenology · Physics 2017-03-09 Hamzeh Khanpour , Abolfazl Mirjalili , S. Atashbar Tehrani

In this paper, we employ the nonrelativistic QCD factorization to conduct a comprehensive examination of the $Z$ boson decay into a pair of $\Upsilon$ mesons, achieving accuracy at the next-to-leading-order (NLO) in $\alpha_s$. Our…

High Energy Physics - Phenomenology · Physics 2024-08-27 Cong Li , Ying-Zhao Jiang , Zhan Sun

We define a general scheme for the evolution of fragmentation functions which resums both soft gluon logarithms and mass singularities in a consistent manner and to any order, and requires no additional theoretical assumptions. Using the…

High Energy Physics - Phenomenology · Physics 2010-03-25 S. Albino , B. A. Kniehl , G. Kramer , W. Ochs

In this paper I show that it is possible to use Regge theory to constrain the initial parton distribution functions of a global DGLAP fit. In this approach, both quarks and gluons have the same high-energy behaviour which may also be used…

High Energy Physics - Phenomenology · Physics 2014-11-17 Gregory Soyez

The effects of the first nonlinear corrections to the DGLAP evolution equations are studied by using the recent HERA data for the structure function $F_2(x,Q^2)$ of the free proton and the parton distributions from CTEQ5L and CTEQ6L as a…

High Energy Physics - Phenomenology · Physics 2014-11-17 K. J. Eskola , H. Honkanen , V. J. Kolhinen , Jianwei Qiu , C. A. Salgado

Parton distribution functions (PDFs) with QED corrections extracted from the QED$\otimes$QCD DGLAP evolution equations in the framework of "valon" model. Our results for the PDFs with QED corrections in this phenomenological model are in…

High Energy Physics - Phenomenology · Physics 2017-10-25 Marzieh Mottaghizadeh , Fatemeh Taghavi Shahri , Parvin Eslami

The most recent H1 and ZEUS data for diffractive structure functions are analyzed under three different theoretical approaches. This includes the Pomeron Structure Function (PSF) framework, Bartels-Ellis-Kowalski-Wusthoff (BEKW) color…

High Energy Physics - Phenomenology · Physics 2007-05-23 S. Sapeta

We use the known soft and collinear limits of tree- and one-loop scattering amplitudes -- computed over a decade ago -- to explicitly construct a subtraction scheme for next-to-next-to-leading order (NNLO) computations. Our approach…

High Energy Physics - Phenomenology · Physics 2015-06-03 Radja Boughezal , Kirill Melnikov , Frank Petriello

We perform a global fit of parton distribution functions (PDFs) together with the strong coupling constant $\alpha_s$ and the quark masses $m_c$, $m_b$ and $m_t$ at next-to-leading order (NLO) in QCD. The analysis applies the…

High Energy Physics - Phenomenology · Physics 2018-09-10 S. Alekhin , J. Blümlein , S. Moch

We discuss interplay between the high-twist (HT) terms in the operator-product expansion and the next-to-next-to-leading-order (NNLO) QCD corrections to the deep-inelastic-scattering structure functions in analysis of the high-precision…

High Energy Physics - Phenomenology · Physics 2007-05-23 S. Alekhin

We discuss the next-to-next-to-leading order (NNLO) QCD corrections to Z boson production in association with a jet including all partonic channels at all color levels and including the leptonic decay of the Z boson. We focus on the…

High Energy Physics - Phenomenology · Physics 2016-05-12 A. Gehrmann-De Ridder , T. Gehrmann , E. W. N. Glover , A. Huss , T. A. Morgan

In order to obtain polarised parton densities we have made next to leading order QCD fit using experimental data on deep inelastic structure functions on nucleons. This fit is compared with the updated fit to coresponding spin asymmetries.…

High Energy Physics - Phenomenology · Physics 2009-11-07 Jan Bartelski , Stanislaw Tatur

We present the first calculation of next-to-leading order (NLO) factorized QED contributions to the short-distance hard coefficients of inclusive lepton-hadron deep inelastic scattering (DIS) in a joint QCD and QED factorization approach.…

High Energy Physics - Phenomenology · Physics 2024-08-19 Justin Cammarota , Jian-Wei Qiu , Kazuhiro Watanabe , Jia-Yue Zhang

The supersymmetric evolution of the fragmentation functions (or timelike evolution) within N=1 $QCD$ is discussed and predictions for the fragmentation functions of the theory (into final protons) are given. We use a backward running of the…

High Energy Physics - Phenomenology · Physics 2014-11-17 Claudio Coriano' , Alon E. Faraggi

We extract polarized parton distribution functions (PPDFs), referred to as "KTA17," together with the highly correlated strong coupling $\alpha_s$ from recent and up-to-date $g_1$ and $g_2$ polarized structure functions world data at…

High Energy Physics - Phenomenology · Physics 2017-04-07 Hamzeh Khanpour , Sara Taheri Monfared , S. Atashbar Tehrani