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Related papers: Semi-Inclusive Deep Inelastic Scattering and Besse…

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We study the universality issue of the transverse momentum dependent parton distributions at small-x, by comparing the initial/final state interaction effects in dijet-correlation in pA collisions with those in deep inelastic lepton nucleus…

High Energy Physics - Phenomenology · Physics 2014-11-20 Bo-Wen Xiao , Feng Yuan

Flux-integrated semiexclusive differential cross sections for charged-current quasielastic and neutral-current elastic neutrino scattering on argon are analyzed. The cross sections are calculated using the relativistic distorted-wave…

High Energy Physics - Phenomenology · Physics 2023-04-19 A. V. Butkevich

We shortly review the various methods suggested for determining the transversity function. Among such methods, we consider especially those based on semi-inclusive deep inelastic scattering. In the framework of this kind of reactions, we…

High Energy Physics - Phenomenology · Physics 2009-11-07 Elvio Di Salvo

The T-odd distribution functions contributing to transversity properties of the nucleon and their role in fueling nontrivial contributions to azimuthal asymmetries in semi-inclusive deep inelastic scattering are investigated. We use a…

High Energy Physics - Phenomenology · Physics 2007-05-23 Leonard P. Gamberg , Gary R. Goldstein , Karo A. Oganessyan

To identify some way to measure the quark transversity, this thesis analyzes one-particle and two-particle inclusive deep inelastic scattering, where one and two of the outgoing hadrons are detected in coincidence with the electron. It is…

High Energy Physics - Phenomenology · Physics 2009-09-29 A. Bacchetta

In this literature, we carefully investigate the structure of single- and multi-frequency imaging functions, that are usually employed in inverse scattering problems. Based on patterns of the singular vectors of the Multi-Static Response…

Mathematical Physics · Physics 2013-04-04 Young Deuk Jo , Young Mi Kwon , Joo Young Huh , Won-Kwang Park

The unpolarised transverse momentum dependent distribution and fragmentation functions are extracted from HERMES and COMPASS experimental measurements of SIDIS multiplicities for charged hadron production. The data are grouped into…

High Energy Physics - Phenomenology · Physics 2015-06-18 M. Anselmino , M. Boglione , J. O. Gonzalez H. , S. Melis , A. Prokudin

The role of intrinsic $\bfk_\perp$ in inclusive and semi-inclusive Deep Inelastic Scattering processes ($\ell p \to \ell h X$) is studied with exact kinematics within QCD parton model at leading order; the dependence of the unpolarized…

High Energy Physics - Phenomenology · Physics 2009-11-11 M. Anselmino , M. Boglione , U. D'Alesio , A. Kotzinian , F. Murgia , A. Prokudin

The (anti)neutrino nucleus scattering plays a very important role in probing the hadronic structure as well as the electroweak phenomenologies. To this end, we calculate the jet production semi-inclusive deeply inelastic (anti)neutrino…

High Energy Physics - Phenomenology · Physics 2023-05-31 X. Yang , W. Yang

In this article we review the present understanding of azimuthal and single spin asymmetries for inclusive and semi-inclusive particle production in unpolarized and polarized hadronic collisions at high energy and moderately large…

High Energy Physics - Phenomenology · Physics 2008-12-18 U. D'Alesio , F. Murgia

We analyse the twist-three amplitudes that can give rise to single-spin asymmetries in hadron-hadron scattering; in so doing we bring to light a novel factorisation property. As already known, the requirement of an imaginary part leads to…

High Energy Physics - Phenomenology · Physics 2011-09-13 Philip G. Ratcliffe

The present study seeks to investigate mathematical structures of a multi-frequency subspace migration weighted by the natural logarithmic function for imaging of thin electromagnetic inhomogeneities from measured far-field pattern. To this…

Mathematical Physics · Physics 2014-12-23 Young-Deuk Joh , Won-Kwang Park

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…

High Energy Physics - Phenomenology · Physics 2020-10-28 Markus A. Ebert , Bernhard Mistlberger , Gherardo Vita

The quark spin densities related to generalized parton distributions in impact-parameter space and to transverse-momentum dependent parton distributions are reviewed within a light-cone quark model, with focus on the role of the different…

High Energy Physics - Phenomenology · Physics 2015-05-14 B. Pasquini , S. Boffi , P. Schweitzer

We investigate the twist two gluon distribution functions for spin 1/2 hadrons, emphasizing intrinsic transverse momentum of the gluons. These functions are relevant in leading order in the inverse hard scale in scattering processes such as…

High Energy Physics - Phenomenology · Physics 2009-10-31 P. J. Mulders , J. Rodrigues

The one-loop correction to heavy quark pair back-to-back production in unpolarized semi-inclusive deep inelastic scattering is given in this work in the framework of transverse momentum dependent(TMD) factorization. Both unpolarized and…

High Energy Physics - Phenomenology · Physics 2017-12-06 Guang-Peng Zhang

Within the framework of a generalized factorization, semi-inclusive deeply inelastic scattering (SIDIS) cross sections can be expressed as a series of products of collinear hard parts and transverse-momentum-dependent (TMD) parton…

High Energy Physics - Phenomenology · Physics 2014-11-20 Jian-Hua Gao , Zuo-tang Liang , Xin-Nian Wang

We give a general overview of the role and interpretation of fragmentation functions in hard processes. Transverse momentum dependence gives rise to time-reversal odd fragmentation functions contributing at leading order. Final state…

High Energy Physics - Phenomenology · Physics 2007-05-23 A. Bianconi , S. Boffi , R. Jakob , M. Radici

The Collins fragmentation function is extracted from HERMES data on azimuthal single spin asymmetries in semi-inclusive deeply inelastic scattering, and BELLE data on azimuthal asymmetries in electron positron annihilations. A Gaussian…

High Energy Physics - Phenomenology · Physics 2008-11-26 A. V. Efremov , K. Goeke , P. Schweitzer

In 2022, the COMPASS collaboration performed semi-inclusive measurements of deep-inelastic muon-scattering on a transversely polarised deuteron (6LiD) target. From these data, transverse-spin-dependent dihadron asymmetries are extracted…

High Energy Physics - Experiment · Physics 2025-12-30 G. D. Alexeev , M. G. Alexeev , C. Alice , A. Amoroso , V. Andrieux , V. Anosov , S. Asatryan , K. Augsten , W. Augustyniak , C. D. R. Azevedo , B. Badelek , R. Beck , J. Beckers , Y. Bedfer , V. Benesova , J. Bernhard , F. Bradamante , A. Bressan , W. -C . Chang , C. Chatterjee , M. Chiosso , S. -U. Chung , A. Cicuttin , M. L. Crespo , D. D'Ago , S. Dalla Torre , S. S. Dasgupta , S. Dasgupta , M. Dehpour , F. Delcarro , I. Denisenko , O. Yu. Denisov , S. V. Donskov , N. Doshita , Ch. Dreisbach , W. Dün nweber , R. R. Dusaev , D. Ecker , P. Faccioli , M. Faessler , M. Finger , M. Finger , H. Fischer , K. J. Flöthner , W. Florian , J. M. Friedrich , V. Frolov , L. G. Garcia Ordòñez , O. P. Gavrichtchouk , S. Gerassimov , J. Giarra , D. Giordan o , A. Grasso , A. Gridin , M. Grosse Perdekamp , B. Grube , M. Grüner , A. Guskov , P. Haas , D. von Harrach , M. Hoffmann , A. Hoghmrtsyan , N. d'Hose , C. -Y. Hsieh , S. Ishimoto , A. Ivanov , T. Iwata , V. Jary , E. Jelinkova , R. Joosten , E. Kabuß , F. Kaspar , A. Kerbizi , B. Ketzer , G. V. Khaustov , T. Klasek , J. H. Koivuniemi , V. N. Kolosov , K. Kondo Horikawa , I. Konorov , A. Yu. Korzenev , A. M. Kotzinian , O. M. Kouznetsov , A. Koval , 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 , N. Makke , G. K. Mallot , A. Maltsev , A. Martin , H. Marukyan , J. Marzec , J. Matoušek , T. Matsuda , C. Menezes Pires , F. Metzge r , W. Meyer , M. Mikhasenko , E. Mitrofanov , D. Miura , Y. Miyachi , R. Molina , A. Movsisian , A. Moretti , A. Nagaytsev , D. Neyret , M. Niemiec , J. Nový , W. -D. Nowak , G. Nukazuka , A. G. Olshevsky , M. Ostrick , D. Panzieri , B. Parsamyan , S. P aul , H. Pekeler , J. -C. Peng , M. Pešek , D. V. Peshekhonov , M. Pešková , S. Platchkov , J. Pochodzalla , V. A. Polyakov , P. Pucci , C. Quintans , G. Reicherz , C. Riedl , D. I. Ryabchikov , A. Rychter , A. Rymbekova , V. D. Samoylenko , A. S andacz , S. Sarkar , I. A. Savin , G. Sbrizzai , H. Schmieden , A. Selyunin , S. Seriubin , L. Sinha , D. Spülbeck , A. Srnka , M. Stolarski , M. Sulc , H. Suzuki , S. Tessaro , F. Tessarotto , A. Thiel , F. Tosello , A. Townsend , V. Tskhay , B. Valino ti , B. M. Veit , J. F. C. A. Veloso , A. Vijayakumar , M. Virius , M. Wagner , S. Wallner , K. Zaremba , M. Zavertyaev , M. Zemko , E. Zemlyanichkina , M. Ziembicki