English
Related papers

Related papers: The Gottfried sum rule in an unquenched quark mode…

200 papers

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

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

We discuss the flavor content of the nucleon in an unquenched quark model in which the effects of quark-antiquark pairs (up, down and strange) are taken into account in an explicit form. It is shown that the inclusion of quark-antiquark…

Nuclear Theory · Physics 2009-04-24 R. Bijker , E. Santopinto

In this contribution, we briefly analyze the formalism of the unquenched quark model (UQM) and its application to the description of several observables of hadrons. In the UQM, the effects of $q \bar q$ sea pairs are introduced explicitly…

Nuclear Theory · Physics 2015-09-30 Hugo García Tecocoatzi , Roelof Bijker

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

We present the formalism for a new generation of unquenched quark models 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 via a microscopic, QCD-inspired,…

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

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

We present an unquenched quark model for baryons in which the effects of the quark-antiquark pairs (up, down and strange) are taken into account in an explicit form via a microscopic, QCD-inspired, quark-antiquark creation mechanism. In the…

Nuclear Theory · Physics 2010-01-11 R. Bijker , E. Santopinto

The effects of "quark sea" in determining the flavor structure of the octet baryons have been investigated in the chiral constituent quark model (\chiCQM). The \chiCQM is able to qualitatively generate the requisite amount of quark sea and…

High Energy Physics - Phenomenology · Physics 2014-11-21 Neetika Sharma , Harleen Dahiya

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 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

1) We discuss a sum rule of the tensor structure function $b_1(x)$ for spin-one hadrons along with the Gottfried sum rule. Both sum rules are similar in the sense that they are phenomenological ones based on a naive parton model. As the…

High Energy Physics - Phenomenology · Physics 2016-09-01 S. Kumano

In this contribution, we briefly analyze the formalism of the unquenched quark model (UQM) and its application to the calculation of hadron spectra with self-energy corrections, due to the coupling to the meson-meson continuum. In the UQM,…

High Energy Physics - Phenomenology · Physics 2018-01-03 E. Santopinto , R. Bijker , H. García-Tecocoatzi , J. Ferretti

In this contribution, we discuss the electromagnetic and weak decays of baryons in the unquenched quark model and show that the observed discrepancies between the experimental data and the predictions of the constituent quark model can be…

Nuclear Theory · Physics 2018-09-26 Roelof Bijker , Gustavo Guerrero-Navarro , Emmanuel Ortiz-Pacheco

The sea quark content of the $\Sigma^+$ baryon is investigated using light-cone baryon-meson fluctuation model suggested by Brodsky and Ma. It is found that the $\Sigma^+$ sea is flavour asymmetric ($\dbar > \ubar > \sbar$) and…

High Energy Physics - Phenomenology · Physics 2009-10-31 Fu-Guang Cao , A. I. Signal

We present the formalism for a new generation of unquenched quark models in which quark-antiquark pair effects are taken into account in an explicit form via a microscopic QCD-inspired quark-antiquark creation mechanism. No truncation in…

High Energy Physics - Phenomenology · Physics 2017-08-23 E. Santopinto , R. Bijker

We give a brief summary of the Gottfried sum rule and a flavor asymmetric distribution $\bar u-\bar d$ in the nucleon. First, experimental history of the sum-rule studies is discussed. Second, future prospects for studying the asymmetry at…

High Energy Physics - Phenomenology · Physics 2007-05-23 S. Kumano

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

We compute the light antiquark flavor asymmetry in the proton using the Chiral Quark Model ($\chi_{\rm QM}$). The distribution functions for the light antiquarks $\bar{d}(x)$ and $\bar{u}(x)$ have been extracted with the help of…

High Energy Physics - Phenomenology · Physics 2023-03-22 Shweta Choudhary , Pranjal Srivastava , Harleen Dahiya

We present the last applications of the unquenched quark model (UQM) to the description of flavour asymmetry and strangeness in the proton when baryon-meson components are included. In the meson sector, the UQM is used to calculate the…

Nuclear Theory · Physics 2016-06-22 H. García-Tecocoatzi , R. Bijker , J. Ferretti , E. Santopinto
‹ Prev 1 2 3 10 Next ›