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Hadron wave functions and form factors can be extracted using four-point correlators. Stochastic techniques are used to estimate the all to all propagators, which are required for the exact calculation of four-point functions. We apply the…

High Energy Physics - Lattice · Physics 2008-11-26 Constantia Alexandrou , Giannis Koutsou

The elementary fragmentation function that describes the process $q\to \pi$ is predicted applying crossing and charge symmetry to the cut diagram of the pion valence quark distribution function. This elementary probability distribution…

High Energy Physics - Phenomenology · Physics 2025-06-23 Roberto Correa da Silveira , Fernando E. Serna , Bruno El-Bennich

We present a preliminary measurement of the Collins asymmetries in the inclusive process e^+e^- --> qqbar --> pi pi X at center-of-mass energy near 10.6 GeV. We use a data sample of 468 fb^(-1) collected by the BABAR experiment, and we…

High Energy Physics - Experiment · Physics 2022-03-02 I. Garzia

The pion electromagnetic form factor at spacelike momentum transfer is calculated in relativistic impulse approximation using the Covariant Spectator Theory. The same dressed quark mass function and the equation for the pion bound-state…

High Energy Physics - Phenomenology · Physics 2014-01-09 Elmar P. Biernat , Franz Gross , M. T. Peña , Alfred Stadler

A calculation of the semi--leptonic decays of the kaon ($K_{l3}$) is presented. The results are direct predictions of a covariant model of the pion and kaon introduced earlier by Ito, Buck, Gross. The weak form factors for $K_{l3}$ are…

High Energy Physics - Phenomenology · Physics 2007-05-23 Andrei Afanasev , W. W. Buck

Holographic QCD provides a unique framework in which to compute QCD observables. In this talk we summarize recent numerical work on computing the pion electromagnetic form factor using an AdS/QCD action that includes both spontaneous and…

High Energy Physics - Phenomenology · Physics 2017-08-23 Herry J. Kwee , Richard F. Lebed

In this work, we investigate the gluon distribution functions for the pion and kaon, in addition to the improved result of the valence-quark ones, in the gauge-invariant nonlocal chiral-quark model (NL$\chi$QM), in which the momentum…

High Energy Physics - Phenomenology · Physics 2023-02-14 Parada T. P. Hutauruk , Seung-il Nam

We present the gluon distribution functions of pion and kaon in small-$x$ and large-$x$ regions, and compare them with the results obtained from lattice QCD and continuum Schwinger function methods. Whether in the small-$x$ region or the…

High Energy Physics - Phenomenology · Physics 2024-05-28 Chengdong Han , Wei Kou , Rong Wang , Xurong Chen

The correct description of the hadron's structure requires understanding how quarks and gluons form the observable hadrons and how they are distributed within them. Two key nonperturbative quantities encapsulate this information: parton…

High Energy Physics - Phenomenology · Physics 2025-12-17 Gustavo B. Bopsin , Bruno El-Bennich , Gastão Krein , Fernando E. Serna , Roberto C. da Silveira

The thesis is devoted to the study of the fragmentation process of polarized quarks, and in particular of the Collins effect used for the extraction of the quark transversity distribution. The aim is to include the spin degree of freedom in…

High Energy Physics - Phenomenology · Physics 2020-04-02 Albi Kerbizi

We present a model calculation of the T-odd transverse momentum dependent (TMD) gluon fragmentation functions for a spin-1/2 hadron. Our model is based on the postulation that a time-like off-shell gluon can fragment into a hadron and a…

High Energy Physics - Phenomenology · Physics 2024-05-21 Xiupeng Xie , Zhun Lu

All the leading-twist parton distribution functions are calculated in a spectator model of the nucleon, using scalar and axial-vector diquarks. Single gluon rescattering is used to generate T-odd distribution functions. Different choices…

High Energy Physics - Phenomenology · Physics 2009-01-14 A. Bacchetta , F. Conti , M. Radici

We review recent developments in the theoretical description of inclusive single-hadron production at next-to-leading order in the parton model of quantum chromodynamics. Fragmentation functions are extracted from fits to data of inclusive…

High Energy Physics - Phenomenology · Physics 2007-05-23 Bernd A. Kniehl

I present a preliminary determination of the Fragmentation Functions (FFs) of unidentified charged hadrons at next-to-leading order in quantum chromodynamics. The analysis is based on hadron production cross section data in single-inclusive…

High Energy Physics - Phenomenology · Physics 2017-09-12 Emanuele R. Nocera

The Collins effect describes the modulation of the hadron production by a transversely polarized quark with the sine of the polar angle, $\varphi$, between the produced hadron's transverse momentum and the quark spin. We employ a quark-jet…

High Energy Physics - Phenomenology · Physics 2012-07-09 Hrayr H. Matevosyan , Anthony W. Thomas , Wolfgang Bentz

A ratio of lattice correlation functions is identified from which the pion form factor can be obtained directly. Preliminary results from quenched Wilson simulations are presented.

High Energy Physics - Lattice · Physics 2014-11-17 Frederic D. R. Bonnet , Robert G. Edwards , George T. Fleming , Randy Lewis , David G. Richards

The azimuthal dependence of hadrons produced in lepton scattering off a polarized hadron probes the quark transverse-spin distributions. In the calculation of the asymmetries, transverse momenta of quarks in the distribution and…

High Energy Physics - Phenomenology · Physics 2011-07-19 R. D. Tangerman , P. J. Mulders

The measurements of the Collins and Sivers asymmetries of identified hadrons produced in deep-inelastic scattering of 160 GeV/c muons on a transversely polarised 6LiD target at COMPASS are presented. The results for charged pions and…

High Energy Physics - Experiment · Physics 2011-11-03 The COMPASS Collaboration , M. Alekseev , V. Yu. Alexakhin , Yu. Alexandrov , G. D. Alexeev , A. Amoroso , A. Arbuzov , B. Badełek , F. Balestra , J. Ball , J. Barth , G. Baum , Y. Bedfer , C. Bernet , R. Bertini , M. Bettinelli , R. Birsa , J. Bisplinghoff , P. Bordalo , F. Bradamante , A. Bravar , A. Bressan , G. Brona , E. Burtin , M. P. Bussa , A. Chapiro , M. Chiosso , A. Cicuttin , M. Colantoni , S. Costa , M. L. Crespo , S. Dalla Torre , T. Dafni , S. Das , S. S. Dasgupta , R. De Masi , N. Dedek , O. Yu. Denisov , L. Dhara , V. Diaz , A. M. Dinkelbach , S. V. Donskov , V. A. Dorofeev , N. Doshita , V. Duic , W. Dünnweber , P. D. Eversheim , A. V. Efremov , W. Eyrich , M. Faessler , V. Falaleev , A. Ferrero , L. Ferrero , M. Finger , M. Finger , H. Fischer , C. Franco , J. Franz , J. M. Friedrich , V. Frolov , R. Garfagnini , F. Gautheron , O. P. Gavrichtchouk , R. Gazda , S. Gerassimov , R. Geyer , M. Giorgi , B. Gobbo , S. Goertz , A. M. Gorin , S. Grabmüller , O. A. Grajek , A. Grasso , B. Grube , R. Gushterski , A. Guskov , F. Haas , J. Hannappel , D. von Harrach , T. Hasegawa , J. Heckmann , S. Hedicke , F. H. Heinsius , R. Hermann , C. Heß , F. Hinterberger , M. von Hodenberg , N. Horikawa , S. Horikawa , N. d'Hose , C. Ilgner , A. I. Ioukaev , S. Ishimoto , O. Ivanov , Yu. Ivanshin , T. Iwata , R. Jahn , A. Janata , P. Jasinski , R. Joosten , N. I. Jouravlev , E. Kabuß , D. Kang , B. Ketzer , G. V. Khaustov , Yu. A. Khokhlov , Yu. Kisselev , F. Klein , K. Klimaszewski , S. Koblitz , J. H. Koivuniemi , V. N. Kolosov , E. V. Komissarov , K. Kondo , K. Königsmann , I. Konorov , V. F. Konstantinov , A. S. Korentchenko , A. Korzenev , A. M. Kotzinian , N. A. Koutchinski , O. Kouznetsov , A. Kral , N. P. Kravchuk , Z. V. Kroumchtein , R. Kuhn , F. Kunne , K. Kurek , M. E. Ladygin , M. Lamanna , J. M. Le Goff , A. A. Lednev , A. Lehmann , S. Levorato , J. Lichtenstadt , T. Liska , I. Ludwig , A. Maggiora , M. Maggiora , A. Magnon , G. K. Mallot , A. Mann , C. Marchand , J. Marroncle , A. Martin , J. Marzec , F. Massmann , T. Matsuda , A. N. Maximov , W. Meyer , A. Mielech , Yu. V. Mikhailov , M. A. Moinester , A. Mutter , A. Nagaytsev , T. Nagel , O. Nähle , J. Nassalski , S. Neliba , F. Nerling , S. Neubert , D. P. Neyret , V. I. Nikolaenko , K. Nikolaev , A. G. Olshevsky , M. Ostrick , A. Padee , P. Pagano , S. Panebianco , R. Panknin , D. Panzieri , S. Paul , B. Pawlukiewicz-Kaminska , D. V. Peshekhonov , V. D. Peshekhonov , G. Piragino , S. Platchkov , J. Pochodzalla , J. Polak , V. A. Polyakov , J. Pretz , S. Procureur , C. Quintans , J. -F. Rajotte , S. Ramos , V. Rapatsky , G. Reicherz , D. Reggiani , A. Richter , F. Robinet , E. Rocco , E. Rondio , A. M. Rozhdestvensky , D. I. Ryabchikov , V. D. Samoylenko , A. Sandacz , H. Santos , M. G. Sapozhnikov , S. Sarkar , I. A. Savin , P. Schiavon , C. Schill , L. Schmitt , P. Schönmeier , W. Schröder , O. Yu. Shevchenko , H. -W. Siebert , L. Silva , L. Sinha , A. N. Sissakian , M. Slunecka , G. I. Smirnov , S. Sosio , F. Sozzi , A. Srnka , F. Stinzing , M. Stolarski , V. P. Sugonyaev , M. Sulc , R. Sulej , V. V. Tchalishev , S. Tessaro , F. Tessarotto , A. Teufel , L. G. Tkatchev , G. Venugopal , M. Virius , N. V. Vlassov , A. Vossen , R. Webb , E. Weise , Q. Weitzel , R. Windmolders , S. Wirth , W. Wiślicki , H. Wollny , K. Zaremba , M. Zavertyaev , E. Zemlyanichkina , J. Zhao , R. Ziegler , A. Zvyagin

Fragmentation functions of pion, kaon, and nucleon are determined by global analyses of hadron-production data in $e^+e^-$ annihilation. It is particularly important that uncertainties of the fragmentation functions are estimated for the…

High Energy Physics - Phenomenology · Physics 2007-09-25 M. Hirai , S. Kumano , T. -H. Nagai , M. Oka , K. Sudoh

A perturbative QCD calculation of heavy flavor quark fragmentation into heavy flavor baryons is developed along the lines of corresponding heavy meson models. The non-perturbative formation of the baryon is accomplished by implementing the…

High Energy Physics - Phenomenology · Physics 2009-10-30 Anatoly D. Adamov , Gary R. Goldstein
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