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Related papers: Sea Contributions and Nucleon Structure

200 papers

We calculate the partonic structure of constituent quark in the Next-to-Leading Order for the first time. The structure of any hadron can be obtained thereafter using a convolution method. Such a procedure is used to generate the structure…

High Energy Physics - Phenomenology · Physics 2007-05-23 Firooz Arash , Ali Naghi Khorramian

Gluon topology makes a potentially important contribution to the spin of the constituent quark.

High Energy Physics - Phenomenology · Physics 2009-10-31 Steven D. Bass

The quark cluster model approach to the baryon-baryon interaction is reviewed and recent application to the charge symmetry breaking in nuclear force is discussed.

High Energy Physics - Phenomenology · Physics 2007-05-23 Makoto Oka

We study the helicity distributions of light flavor quark-antiquark ($q \bar{q}$) pairs in the nucleon sea. The valence quarks are handled by adopting the light-cone SU(6) quark-spectator-diquark model and the sea $q \bar{q}$ pairs are…

High Energy Physics - Phenomenology · Physics 2018-09-12 Mengyun Liu , Bo-Qiang Ma

A gauge invariant method for the investigation of scalar diquark clustering in the nucleon ground state is presented. The method focuses on a comparison of quark distributions in the nucleon with those in the $\Delta$ baryon resonance.…

High Energy Physics - Phenomenology · Physics 2009-10-22 Derek B. Leinweber

The covariant quark model is shown to allow a phenomenological description of the neutron electric form factor, G_E^n(Q^2), in the impulse approximation, provided that the wave function contains minor (~ 3 %) admixtures of the lowest…

Nuclear Theory · Physics 2008-11-26 Q. B. Li , D. O. Riska

An extended chiral constituent quark approach, which embodies higher Fock five-quark components in the baryons wave-functions, is employed to study the sea quark content of the octet baryons. We report on the probabilities of $\bar{u}$,…

High Energy Physics - Phenomenology · Physics 2012-06-18 Chunsheng An , Bijan Saghai

It was found that the isoscalar-scalar and isovector-scalar mesons play significant roles in nuclear matter physics. However, the underlying structures of these resonances are not yet well understood. We construct a three-flavor baryonic…

Nuclear Theory · Physics 2024-04-18 Yao Ma , Yong-Liang Ma

Heavy quark spin symmetry is discussed in the context of single and doubly heavy baryons. A special attention is paid to the constraints/simplifications that this symmetry imposes on the non-relativistic constituent quark model wave…

High Energy Physics - Phenomenology · Physics 2011-05-18 C. Albertus , J. E. Amaro , E. Hernandez , J. Nieves

The comparison of magnetic moments of neutron and proton reveals three possible states of a nucleon each composed of quark plus diquark. In this scheme for the quark content uds there should be three baryons with a different structure:…

High Energy Physics - Phenomenology · Physics 2007-05-23 A. V. Kopylov

This report is based on a ten-week program on "Gluons and the quark sea at high-energies", which took place at the Institute for Nuclear Theory in Seattle in Fall 2010. The principal aim of the program was to develop and sharpen the science…

Nuclear Theory · Physics 2015-03-19 D. Boer , M. Diehl , R. Milner , R. Venugopalan , W. Vogelsang , A. Accardi , E. Aschenauer , M. Burkardt , R. Ent , V. Guzey , D. Hasch , K. Kumar , M. A. C. Lamont , Y. Li , W. J. Marciano , C. Marquet , F. Sabatie , M. Stratmann , F. Yuan , S. Abeyratne , S. Ahmed , C. Aidala , S. Alekhin , M. Anselmino , H. Avakian , A. Bacchetta , J. Bartels , H. BC , J. Beebe-Wang , S. Belomestnykh , I. Ben-Zvi , G. Beuf , J. Blumlein , M . Blaskiewicz , A. Bogacz , S. J. Brodsky , T. Burton , R. Calaga , X. Chang , I. O. Cherednikov , P. Chevtsov , G. A. Chirilli , C. Ciofi degli Atti , I. C. Cloet , A. Cooper-Sarkar , R. Debbe , Ya. Derbenev , A. Deshpande , F. Dominguez , A. Dumitru , R. Dupre , B. Erdelyi , C. Faroughy , S. Fazio , A. Fedotov , J. R. Forshaw , R. Geraud , K. Gallmeister , L. Gamberg , J. -H. Gao , D. Gassner , F. Gelis , G. P. Gilfoyle , G. Goldstein , K. Golec-Biernat , V. P. Goncalves , M. Gonderinger , M. Guzzi , P. Hagler , H. Hahn , L. Hammons , Y. Hao , P. He , T. Horn , W. A. Horowitz , M. Huang , A. Hutton , B. Jager , W. Jackson , A. Jain , E. C. Johnson , Z. -B. Kang , L. P. Kaptari , D. Kayran , J. Kewisch , Y. Koike , A. Kondratenko , B. Z. Kopeliovich , Y. V. Kovchegov , G. Krafft , P. Kroll , S. Kumano , K. Kumericki , T. Lappi , T. Lautenschlager , R. Li , Z. -T. Liang , V. N. Litvinenko , S. Liuti , Y. Luo , D. Muller , G. Mahler , A. Majumder , S. Manikonda , F. Marhauser , G. McIntyre , M. Meskauskas , W. Meng , A. Metz , C. B. Mezzetti , G. A. Miller , M. Minty , S. -O. Moch , V. Morozov , U. Mosel , L. Motyka , H. Moutarde , P. J. Mulders , B. Musch , P. Nadel-Turonski , P. Nadolsky , F. Olness , P. N. Ostrumov , B. Parker , B. Pasquini , K. Passek-Kumericki , A. Pikin , F. Pilat , B. Pire , H. Pirner , C. Pisano , E. Pozdeyev , A. Prokudin , V. Ptitsyn , X. Qian , J. -W. Qiu , M. Radici , A. Radyushkin , T. Rao , R. Rimmer , F. Ringer , S. Riordan , T. Rogers , J. Rojo , T. Roser , R. Sandapen , R. Sassot , T. Satogata , H. Sayed , A. Schafer , G. Schnell , P. Schweitzer , B. Sheehy , J. Skaritka , G. Soyez , M. Spata , H. Spiesberger , A. M. Stasto , N. G. Stefanis , M. Strikman , M. Sullivan , L. Szymanowski , K. Tanaka , S. Taneja , S. Tepikian , B. Terzic , Y. Than , T. Toll , D. Trbojevic , E. Tsentalovich , N. Tsoupas , K. Tuchin , J. Tuozzolo , T. Ullrich , A. Vossen , S. Wallon , G. Wang , H. Wang , X. -N. Wang , S. Webb , C. Weiss , Q. Wu , B. -W. Xiao , W. Xu , B. Yunn , A. Zelenski , Y. Zhang , J. Zhou , P. Zurita

In the model every quark or lepton is identified with a quartet of four "more elementary" particles. One particle in a quartet is a massive spin-0 boson and other three particles are massless spin-1/2 fermions.

High Energy Physics - Phenomenology · Physics 2007-05-23 N. G. Marchuk

Here we study the quark orbital angular momentum of the ground octet baryons employing an extended chiral constituent quark model, within which the baryon wave functions are taken to be superposition of the traditional $qqq$ and the…

High Energy Physics - Phenomenology · Physics 2023-03-01 Jing-Feng Li , Cheng Chen , Gang Li , Chun-Sheng An , Cheng-Rong Deng , Ju-Jun Xie

Nontrivial $q \bar q$ sea effects have their origin in the low-$Q^2$ dynamics of strong QCD. We present here a quark model calculation of the contribution of $s \bar s$ pairs arising from a {\it complete} set of OZI-allowed strong $Y^*K^*$…

High Energy Physics - Phenomenology · Physics 2010-04-06 Paul Geiger , Nathan Isgur

We investigate the spin structure of the nucleon in an extended Jaffe-Lipkin quark model. In addition to the conventional $3q$ structure, different $(3q)(Q\bar{Q})$ admixtures in the nucleon wavefunction are also taken into account. The…

High Energy Physics - Phenomenology · Physics 2007-05-23 Bo-Qiang Ma , Ivan Schmidt , Jian-Jun Yang

Besides the ordinary hadrons, QCD allows the existence of states in which excitations of the gluonic field can play the role of valence particles, either alone in a glueball, or coupled to quarks in a hybrid. So, hybrid baryons, made of…

High Energy Physics - Phenomenology · Physics 2024-09-04 Lorenzo Cimino , Cintia T. Willemyns , Claude Semay

Using generalized Sehgal equations for magnetic moments of baryon octet and taking into account $\Sigma^{0}-\Lambda$ mixing and two particle corrections to independent quark contributions we obtain very good fit using experimental values…

High Energy Physics - Phenomenology · Physics 2009-11-10 J. Bartelski , S. Tatur

The meson-cloud model of the nucleon consisting of a system of three valence quarks surrounded by a meson cloud is applied to study the electroweak structure of the proton and neutron. The electroweak nucleon form factors are calculated…

High Energy Physics - Phenomenology · Physics 2015-05-13 B. Pasquini , S. Boffi

Parton distribution and correlation functions describe the relation between a hadron and the quarks and gluons (or collectively, the partons) within it, and carry rich information on hadron's partonic structure that cannot be calculated by…

High Energy Physics - Phenomenology · Physics 2020-01-08 Jian-Wei Qiu

Light-baryon resonances (with u,d, and s quarks in the SU(3) classification) fall on Regge trajectories. When their squared masses are plotted against the intrinsic orbital angular momenta {\rm L}, $\Delta^*$'s with even and odd parity can…

Nuclear Experiment · Physics 2017-08-23 E. Klempt