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Related papers: Can We Get Deeper Inside the Pion at the LHC?

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We study the possibility of measuring parity-violating pion-nucleon coupling h_{\pi NN}^{(1)} from \pi^+ electroproton production in the threshold region. We calculate the electron-helicity asymmetry in terms of h_{\pi NN}^{(1)} and the…

Nuclear Theory · Physics 2009-11-06 Jiunn-Wei Chen , Xiangdong Ji

The Drell-Yan massive dilepton production in hadron-hadron collisions provides a unique tool, complementary to Deep Inelastic Scattering, for improving our understanding of hadronic substructure and in particular for testing parton…

High Energy Physics - Phenomenology · Physics 2016-03-15 Eduardo Basso , Claude Bourrely , Roman Pasechnik , Jacques Soffer

In high energy proton-proton collisions, collimated sprays of particles, called jets, result from hard scattered quarks or gluons. Jets are copiously produced in these collisions; however, the dynamic process through which quarks and…

High Energy Physics - Experiment · Physics 2019-05-29 Joseph D. Osborn

We present new sets of pion, kaon, proton and inclusive charged hadron fragmentation functions obtained in NLO combined analyses of single-inclusive hadron production in electron-positron annihilation, proton-proton collisions, and…

High Energy Physics - Phenomenology · Physics 2008-11-26 Daniel de Florian , Rodolfo Sassot , Marco Stratmann

The measurement of primary $\pi^{\pm}$, K$^{\pm}$, p and $\overline{p}$ production at mid-rapidity ($|y| <$ 0.5) in proton-proton collisions at $\sqrt{s} = 7$ TeV performed with ALICE (A Large Ion Collider Experiment) at the Large Hadron…

Nuclear Experiment · Physics 2015-10-13 ALICE Collaboration

A method is presented using helicity cross sections for calculating neutrino-nucleon interactions. The formalism is applied in the calculation of the pion spectra produced by nu_mu and nu_tau beams. The masses of the charged leptons are…

High Energy Physics - Phenomenology · Physics 2008-12-23 E. A. Paschos , Subhendu Rakshit

We report on double-differential inclusive cross-sections of the production of secondary protons, deuterons, and charged pions and kaons, in the interactions with a 5% nuclear interaction length thick stationary beryllium target, of a +8.9…

We consider the charge-odd correlations (COC) in cross sections of processes of production of charged particles. The cases of a muonic pair and pion systems $\pi^{+}\pi^{-},\pi^{+}\pi^{-}\pi^{0}$ are considered in detail for electron-proton…

High Energy Physics - Phenomenology · Physics 2008-11-26 A. I. Ahmadov , Yu. M. Bystritskiy , E. A. Kuraev , E. Zemlyanaya , T. V. Shishkina

We discuss the production of hadrons in polarized lepton nucleon interactions and in the current jet fragmentation region; using the QCD hard scattering formalism we compute the helicity density matrix of the hadron and show how its…

High Energy Physics - Phenomenology · Physics 2009-10-28 M. Anselmino , M. Boglione , J. Hansson , F. Murgia

Knowing the charge of the parton initiating a light-quark jet could be extremely useful both for testing aspects of the Standard Model and for characterizing potential beyond-the-Standard-Model signals. We show that despite the…

High Energy Physics - Phenomenology · Physics 2013-06-17 David Krohn , Tongyan Lin , Matthew D. Schwartz , Wouter J. Waalewijn

The ZEUS inclusive cross-section data from HERA-I, for charged and neutral current processes, taken with $e^+$ and $e^-$ beams, have been used in a new NLO QCD analysis to extract the parton distribution functions (PDFs) of the proton…

High Energy Physics - Phenomenology · Physics 2007-05-23 A. M. Cooper-Sarkar

The double-differential production cross-section of positive pions, $d^2\sigma^{\pi^{+}}/dpd\Omega$, measured in the HARP experiment is presented. The incident particles are 8.9 GeV/c protons directed onto a beryllium target with a nominal…

High Energy Physics - Experiment · Physics 2012-08-27 HARP Collaboration

The precise knowledge of photon pair production rates at the LHC is crucial to estimate the sensitivity to a Higgs boson in the intermediate mass range. This background consists not only of prompt photons but also of fake photons stemming…

High Energy Physics - Phenomenology · Physics 2007-05-23 T. Binoth

The production of charm quark jets in association with electroweak gauge bosons at the LHC can be used as a tool to constrain quark parton distribution functions (PDFs). Motivated by recent measurements at the Tevatron and LHC, we calculate…

High Energy Physics - Phenomenology · Physics 2013-05-30 W. J. Stirling , E. Vryonidou

Interaction cross sections and charged pion spectra in p+C interactions at 31 GeV/c were measured with the large acceptance NA61/SHINE spectrometer at the CERN SPS. These data are required to improve predictions of the neutrino flux for the…

High Energy Physics - Experiment · Physics 2015-03-18 N. Abgrall , A. Aduszkiewicz , B. Andrieu , T. Anticic , N. Antoniou , J. Argyriades , A. G. Asryan , B. Baatar , A. Blondel , J. Blumer , M. Bogusz , L. Boldizsar , A. Bravar , W. Brooks , J. Brzychczyk , A. Bubak , S. A. Bunyatov , O. Busygina , T. Cetner , K. -U. Choi , P. Christakoglou , P. Chung , T. Czopowicz , N. Davis , F. Diakonos , S. Di Luise , W. Dominik , J. Dumarchez , R. Engel , A. Ereditato , L. S. Esposito , G. A. Feofilov , Z. Fodor , A. Ferrero , A. Fulop , X. Garrido , M. Gazdzicki , M. Golubeva , K. Grebieszkow , A. Grzeszczuk , F. Guber , H. Hakobyan , T. Hasegawa , S. Igolkin , A. S. Ivanov , Y. Ivanov , A. Ivashkin , K. Kadija , A. Kapoyannis , N. Katrynska , D. Kielczewska , D. Kikola , J. -H. Kim , M. Kirejczyk , J. Kisiel , T. Kobayashi , O. Kochebina , V. I. Kolesnikov , D. Kolev , V. P. Kondratiev , A. Korzenev , S. Kowalski , S. Kuleshov , A. Kurepin , R. Lacey , J. Lagoda , A. Laszlo , V. V. Lyubushkin , M. Mackowiak , Z. Majka , A. I. Malakhov , A. Marchionni , A. Marcinek , I. Maris , V. Marin , T. Matulewicz , V. Matveev , G. L. Melkumov , A. Meregaglia , M. Messina , St. Mrowczynski , S. Murphy , T. Nakadaira , P. A. Naumenko , K. Nishikawa , T. Palczewski , G. Palla , A. D. Panagiotou , W. Peryt , O. Petukhov , R. Planeta , J. Pluta , B. A. Popov , M. Posiadala , S. Pulawski , W. Rauch , M. Ravonel , R. Renfordt , A. Robert , D. Rohrich , E. Rondio , B. Rossi , M. Roth , A. Rubbia , M. Rybczynski , A. Sadovsky , K. Sakashita , T. Sekiguchi , P. Seyboth , M. Shibata , A. N. Sissakian , E. Skrzypczak , M. Slodkowski , A. S. Sorin , P. Staszel , G. Stefanek , J. Stepaniak , C. Strabel , H. Strobele , T. Susa , P. Szaflik , M. Szuba , M. Tada , A. Taranenko , R. Tsenov , R. Ulrich , M. Unger , M. Vassiliou , V. V. Vechernin , G. Vesztergombi , A. Wilczek , Z. Wlodarczyk , A. Wojtaszek , J. -G. Yi , I. -K. Yoo , W. Zipper

Hard, or high transverse momentum, pion photoproduction can be a tool for probing the parton structure of the beam and target. We discuss the perturbative and soft processes that contribute, and show how regions where perturbative processes…

High Energy Physics - Phenomenology · Physics 2007-05-23 Carl E. Carlson

Generalized parton distributions (GPDs) encoding multidimensional information of hadron partonic structure appear as the building blocks in a factorized description of hard exclusive reactions. The nucleon GPDs have been accessed by deeply…

Nuclear Experiment · Physics 2016-07-01 Takahiro Sawada , Wen-Chen Chang , Shunzo Kumano , Jen-Chieh Peng , Shinya Sawada , Kazuhiro Tanaka

This paper presents an analysis at next-to-next-to-leading order in the theory of quantum chromodynamics for the determination of a new set of proton parton distribution functions using diverse measurements in $pp$ collisions at $\sqrt{s} =…

High Energy Physics - Experiment · Physics 2022-05-27 ATLAS Collaboration

LHC collisions can act as a source of photons in the initial state. This mechanism plays an important role in the production of particles with electroweak couplings, and a precise account of photon-initiated (PI) production at the LHC is a…

High Energy Physics - Phenomenology · Physics 2021-06-04 L. A. Harland-Lang

We report on double-differential inclusive cross-sections of the production of secondary protons, charged pions, and deuterons, in the interactions with a 5% nuclear interaction length thick stationary tin target, of proton and pion beams…

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