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The deuteron deep inelastic unpolarized structure function F_2^D is calculated using the Wilson operator product expansion method. The long distance behaviour, related to the deuteron bound state properties, is evaluated using the…

Nuclear Theory · Physics 2010-12-17 J. Paulo Pinto , A. Amorim , F. D. Santos

We propose to measure neutron and deuteron transversity TMDs. The quark transversity distributions of the nucleon are decoupled from the deuteron gluon transversity in the $Q^2$ evolution due to the chiral-odd property in the…

Nuclear Experiment · Physics 2022-05-04 D. Keller

We investigate the structure of constituent quarks and study implications for quark distribution functions of hadrons. Constituent quarks are constructed by dressing bare quarks with Goldstone bosons using the chiral quark model. We…

High Energy Physics - Phenomenology · Physics 2009-10-30 K. Suzuki , W. Weise

The recent high statistics NMC data on the Tin to Carbon structure function ratio seems to indicate, for the first time, a significant $Q^2$ dependence, especially at small values of Bjorken $x$, $x < 0.05$, and $Q^2 > 1 GeV^2$. Pure…

High Energy Physics - Phenomenology · Physics 2007-05-23 D. Indumathi

The class of interference fragmentation functions, arising from interference among different hadron production channels, is reconsidered. Their symmetry properties with respect to chiral transformations allow building spin asymmetries where…

High Energy Physics - Phenomenology · Physics 2017-08-23 M. Radici

We measured the $g_1$ spin structure function of the deuteron at low $Q^{2}$, where QCD can be approximated with chiral perturbation theory ($\chi$PT). The data cover the resonance region, up to an invariant mass of $W\approx1.9$~GeV. The…

Nuclear Experiment · Physics 2022-02-21 K. P. Adhikari , A. Deur , L. El Fassi , H. Kang , S. E. Kuhn , M. Ripani , K. Slifer , X. Zheng , S. Adhikari , Z. Akbar , M. J. Amaryan , H. Avakian , J. Ball , I. Balossino , L. Barion , M. Battaglieri , I. Bedlinskiy , A. S. Biselli , P. Bosted , W. J. Briscoe , J. Brock , S. Bueltmann , V. D. Burkert , F. Thanh Cao , C. Carlin , D. S. Carman , A. Celentano , G. Charles , J. -P. Chen , T. Chetry , S. Choi , G. Ciullo , L. Clark , P. L. Cole , M. Contalbrigo , V. Crede , A. D'Angelo , N. Dashyan , R. De Vita , E. De Sanctis , M. Defurne , C. Djalali , G. E. Dodge , V. Drozdov , R. Dupre , H. Egiyan , A. El Alaoui , L. Elouadrhiri , P. Eugenio , G. Fedotov , A. Filippi , Y. Ghandilyan , G. P. Gilfoyle , E. Golovatch , R. W. Gothe , K. A. Griffioen , M. Guidal , N. Guler , L. Guo , K. Hafidi , H. Hakobyan , C. Hanretty , N. Harrison , M. Hattawy , D. Heddle , K. Hicks , M. Holtrop , C. E. Hyde , Y. Ilieva , D. G. Ireland , E. L. Isupov , D. Jenkins , H. S. Jo , S. C. Johnston , K. Joo , S. Joosten , M. L. Kabir , C. D. Keith , D. Keller , G. Khachatryan , M. Khachatryan , M. Khandaker , W. Kim , A. Klein , F. J. Klein , P. Konczykowski , K. Kovacs , V. Kubarovsky , L. Lanza , P. Lenisa , K. Livingston , E. Long , I . J . D. MacGregor , N. Markov , M. Mayer , B. McKinnon , D. G. Meekins , C. A. Meyer , T. Mineeva , M. Mirazita , V. Mokeev , A Movsisyan , C. Munoz Camacho , P. Nadel-Turonski , G. Niculescu , S. Niccolai , M. Osipenko , A. I. Ostrovidov , M. Paolone , L. Pappalardo , R. Paremuzyan , K. Park , E. Pasyuk , D. Payette , W. Phelps , S. K. Phillips , J. Pierce , O. Pogorelko , J. Poudel , J. W. Price , Y. Prok , D. Protopopescu , B. A. Raue , A. Rizzo , G. Rosner , P. Rossi , F. Sabatie , C. Salgado , R. A. Schumacher , Y. G. Sharabian , T. Shigeyuki , A. Simonyan , Iu. Skorodumina , G. D. Smith , N. Sparveris , D. Sokhan , S. Stepanyan , I. I. Strakovsky , S. Strauch , V. Sulkosky , M. Taiuti , J. A. Tan , M. Ungaro , E. Voutier , X. Wei , L. B. Weinstein , J. Zhang , Z. W. Zhao.

The ratio g1/F1 has been measured over the range 0.03<x<0.6 and 0.3<Q2<10 (GeV/c)2 using deep-inelastic scattering of polarized electrons from polarized protons and deuterons. We find g1/F1 to be consistent with no Q2-dependence at fixed x…

High Energy Physics - Experiment · Physics 2008-11-26 The E143 Collaboration , K. Abe et al

Transverse spin physics is an important part of the scientific programme of the COMPASS experiment at CERN. The analysis of the data taken with the target polarized orthogonally to the 160 GeV/c muon beam momentum has allowed to measure for…

High Energy Physics - Experiment · Physics 2008-11-26 F. Bradamante

The mass spectra of nucleon resonances with spin 1/2, 3/2, and 5/2 are systematically studied in the constituent quark model with meson-quark coupling, which is inspired by the spontaneous breaking of chiral symmetry of QCD. The meson-quark…

Nuclear Theory · Physics 2009-10-30 H. Kowata , M. Arima , K. Masutani

We explore the physics of the parton-hadron duality in the nucleon structure functions appearing in lepton-nucleon scattering. We stress that the duality allows one to extract the higher-twist matrix elements from data in the resonance…

High Energy Physics - Phenomenology · Physics 2009-10-28 Xiangdong Ji , Peter Unrau

Quark-hadron duality is studied in a systematic way for polarized and unpolarized structure functions, by taking into account all the available data in the resonance region. In both cases, a precise perturbative QCD based analysis of the…

High Energy Physics - Phenomenology · Physics 2009-11-11 A. Fantoni , N. Bianchi , S. Liuti

We review what is currently known about the transverse spin structure of hadrons, in particular from observables that can be analyzed within a collinear framework. These effects have been around for 40 years and represent a critical test of…

High Energy Physics - Phenomenology · Physics 2016-12-21 D. Pitonyak

We report current status of global analyses on nuclear parton distribution functions (NPDFs). The optimum NPDFs are determined by analyzing high-energy nuclear reaction data. Due to limited experimental measurements, antiquark modifications…

High Energy Physics - Phenomenology · Physics 2015-05-27 M. Hirai , S. Kumano , K. Saito

This is a review of recent developments in hadron structure within the framework of Lattice QCD. The main focus is on recent achievements in the evaluation of nucleon quantities, such as the axial charge, electromagnetic form factors, the…

High Energy Physics - Lattice · Physics 2014-11-04 Martha Constantinou

The gravitational form factors for a hadron, the form factors for the hadron matrix element of the QCD energy-momentum tensor, not only describe the coupling of the hadron with a graviton, but also serve as unique quantities for describing…

High Energy Physics - Phenomenology · Physics 2018-08-15 Kazuhiro Tanaka

Sum rules for structure functions and their twist-2 relations have important roles in constraining their magnitudes and $x$ dependencies and in studying higher-twist effects. The Wandzura-Wilczek (WW) relation and the Burkhardt-Cottingham…

High Energy Physics - Phenomenology · Physics 2021-10-13 S. Kumano , Qin-Tao Song

New experimental results on the spin dependent structure functions g_1 and g_2 which are determined from deep-inelastic scattering experiments at CERN, SLAC and DESY are reported. These results are used to evaluate the Bjorken sum rule and…

High Energy Physics - Phenomenology · Physics 2008-02-03 J. Nassalski

Quark-hadron duality is studied in a systematic way for both the unpolarized and polarized structure functions, by taking into account all the available data in the resonance region.In both cases, a detailed perturbative QCD based analysis…

High Energy Physics - Phenomenology · Physics 2009-11-11 A. Fantoni , N. Bianchi , S. Liuti

Partonic structure of constituent quark (or{\it{valon}}) in the Next-to-Leading Order is used to calculate pion structure function. This is a further demonstration of the finding that the constituent quark structure is universal, and once…

High Energy Physics - Phenomenology · Physics 2009-11-10 Firooz Arash

We present experimental results of the first high-precision test of quark-hadron duality in the spin-structure function g_1 of the neutron and $^3$He using a polarized 3He target in the four-momentum-transfer-squared range from 0.7 to 4.0…