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Related papers: Quark sea asymmetries of the octet baryons

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The effects of nonperturbatively generated ``quark sea'' have been investigated to determine the flavor structure of the octet baryons. The chiral constituent quark model ($\chi$CQM), which is known to provide a satisfactory explanation of…

High Energy Physics - Phenomenology · Physics 2017-08-23 Harleen Dahiya , Neetika Sharma

The quark flavor distribution functions of the octet baryons ($N$, $\Sigma$, $\Xi$ and $\Lambda$) have been calculated in the chiral constituent quark model ($\chi$CQM). In particular, the valence and sea quark flavor distribution functions…

High Energy Physics - Phenomenology · Physics 2015-06-11 Harleen Dahiya

The flavor asymmetry of the nucleon sea, i.e., the excess of $d\bar{d}$ quark-antiquark pairs over $u\bar{u}$ ones in the proton can be explained by several different models; therefore, it is a challenge to discriminate these models from…

High Energy Physics - Phenomenology · Physics 2010-06-17 Lijing Shao , Yong-Jun Zhang , Bo-Qiang Ma

Sea quark contents of the octet baryons are investigated by employing an extended chiral constituent quark approach, which embodies higher Fock five-quark components in the baryons wave-functions. The well-known flavor asymmetry of the…

High Energy Physics - Phenomenology · Physics 2015-06-04 Chunsheng An , Bijan Saghai

In this contribution, we present the unquenched quark model as an extension of the constituent quark model that includes the effects of sea quarks via a $^{3}P_{0}$ quark-antiquark pair-creation mechanism. Particular attention is paid to…

High Energy Physics - Phenomenology · Physics 2016-09-07 R. Bijker , S. Diaz-Gomez , M. A. Lopez-Ruiz , E. Santopinto

The intrinsic quark-antiquark pairs generated by the minimal energy nonperturbative meson-baryon fluctuations in the nucleon sea provide a consistent framework for understanding a number of empirical anomalies observed in the deep inelastic…

High Energy Physics - Phenomenology · Physics 2008-02-03 B. -Q. Ma , S. J. Brodsky

Chiral constituent quark model with configuration mixing (\chiCQM_{{\rm config}}) is known to provide a satisfactory explanation of the ``proton spin problem'' and related issues. In order to enlarge the scope of \chiCQM_{{\rm config}}, we…

High Energy Physics - Phenomenology · Physics 2008-11-26 Harleen Dahiya , Manmohan Gupta

We have investigated the axial charges of the ground octet baryons within the extended chiral constituent quark model, where all the possible compact five-quark Fock components $qqq(q\bar{q}) (q=u, d, s)$ in the baryons are considered. The…

High Energy Physics - Phenomenology · Physics 2022-06-29 Rui Qi , Jin-Bao Wang , Gang Li , Chun-Sheng An , Cheng-Rong Deng , Ju-Jun Xie

It is now widely recognized that a key to unravel the nonperturbative chiral-dynamics of QCD hidden in the deep-inelastic-scattering observables is the flavor structure of sea-quark distributions in the nucleon. We analyze the flavor…

High Energy Physics - Phenomenology · Physics 2015-06-19 Masashi Wakamatsu

The quark and gluon structure of the proton has been under intense experimental and theoretical investigation for five decades. Even for the distributions of the well-studied valence quarks, challenges such as the value of the down quark to…

Nuclear Experiment · Physics 2019-03-27 D. F. Geesaman , P. E. Reimer

After a pedagogical review of the simple constituent quark model and deep inelastic sum rules, we describe how a quark sea as produced by the emission of internal Goldstone bosons by the valence quarks can account for the observed features…

High Energy Physics - Phenomenology · Physics 2009-10-30 Ling-Fong Li , T. P. Cheng

The flavor asymmetry of the nucleon sea is discussed in an unquenched quark model for baryons in which the effects of quark-antiquark pairs (u anti-u, d anti-d and s anti-s) are taken into account in an explicit form. The inclusion of q…

Nuclear Theory · Physics 2017-11-02 R. Bijker , E. Santopinto

The axial form factor as well as the axial charge of octet baryons are studied in the perturbative chiral quark model (PCQM) with the quark wave functions predetermined by fitting the theoretical results of the proton charge form factor to…

High Energy Physics - Phenomenology · Physics 2015-03-03 X. Y. Liu , K. Khosonthongkee , A. Limphirat , P. Suebka , Y. Yan

We treat the baryon as a composite system made out of a "core" of three quarks (as in the standard quark model) surrounded by a "sea" (of gluons and $q\bar{q}$-pairs) which is specified by its total quantum numbers like flavor, spin and…

High Energy Physics - Phenomenology · Physics 2016-02-08 V. Gupta , R. Huerta , G. Sanchez-Colon

We treat the baryon as a composite system made out of a \lq\lq core" of three quarks (as in the standard quark model) surrounded by a \lq\lq sea" (of gluons and $q\bar{q}$-pairs) which is specified by its total quantum numbers like flavor,…

High Energy Physics - Phenomenology · Physics 2014-11-17 V. Gupta , R. Huerta , G. Sanchez-Colon

We present an unquenched quark model for baryons in which the effects of quark-antiquark pairs (light flavors, u, d and s) are taken into account in an explicit form. The method is illustrated with an application to the flavor asymmetry of…

Nuclear Theory · Physics 2017-11-02 R. Bijker , E. Santopinto

The theoretical foundations of the quantum statistical approach to parton distributions are reviewed together with the phenomenological motivations from a few specific features of Deep Inelastic Scattering data. The chiral properties of QCD…

High Energy Physics - Phenomenology · Physics 2014-02-05 Jacques Soffer , Claude Bourrely , Franco Buccella

We discuss some applications of the unquenched quark model which is an extension of the CQM that includes the effects of sea quarks via a 3P0 quark-antiquark pair-creation mechanism. Particular attention is paid to the electromagnetic…

Nuclear Theory · Physics 2017-12-12 Roelof Bijker , Gustavo Guerrero-Navarro , Emmanuel Ortiz-Pacheco

The chiral quark model with a broken U(3) symmetry gives a simple and unified account for the proton spin and flavor puzzles, as well as the octet baryon magnetic moments.

High Energy Physics - Phenomenology · Physics 2007-05-23 T. P. Cheng , Ling-Fong Li

We discuss the flavor asymmetry of the nucleon in an unquenched quark model for baryons in which the effects of quark-antiquark pairs (u anti-u, d anti-d and s anti-s) are taken into account in an explicit form. It is shown that the…

Nuclear Theory · Physics 2017-11-02 R. Bijker , E. Santopinto
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