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Related papers: The Quark Distributions in the \Sigma^+ Hyperon

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Within the collective coordinate approach to chiral soliton models we suggest that breaking of SU(3) flavor symmetry mainly resides in the baryon wave-functions while the charge operators have no (or only small) symmetry breaking…

High Energy Physics - Phenomenology · Physics 2007-05-23 H. Weigel

We take into account the sigma meson cloud effect in the meson cloud model to calculate the distributions of light flavor sea quarks in the proton. Our calculation gives a better description of the data for $\bar{d}(x)/\bar{u}(x)$. We also…

High Energy Physics - Phenomenology · Physics 2009-11-10 Feng Huang , Rong-Guang Xu , Bo-Qiang Ma

We study the possible contribution of the nucleon's virtual meson cloud to the sea quark distribution as observed in deep inelastic lepton scattering. We adjust the meson-nucleon cut-offs to the large-x tails of the antiquark distributions,…

High Energy Physics - Phenomenology · Physics 2007-05-23 W. Koepf , L. L. Frankfurt , M. Strikman

Treating baryons as quark + interacting-diquark bound states, a symmetry-preserving formulation of a vector$\,\times\,$vector contact interaction (SCI) is used to deliver an extensive, coherent set of predictions for $\Lambda, \Sigma^0$…

High Energy Physics - Phenomenology · Physics 2025-09-09 Yang Yu , Peng Cheng , Hui-Yu Xing , Daniele Binosi , Craig D. Roberts

The quark flavor and spin distributions in octet baryons are calculated both in the SU(6) quark spectator diquark model and in a perturbative QCD (pQCD) based model. It is shown that the $\Lambda$ has the most significant difference in…

High Energy Physics - Phenomenology · Physics 2009-10-31 Bo-Qiang Ma , Ivan Schmidt , Jian-Jun Yang

The path integral formulation is given to obtain quark and antiquark distribution functions in the nucleon within the flavor SU(3) version of the chiral quark soliton model. The basic model action is a straightforward generalization of the…

High Energy Physics - Phenomenology · Physics 2009-11-07 M. Wakamatsu

Using an SU(3) flavour symmetry breaking expansion in the quark mass, we determine the QCD component of the nucleon, Sigma and Xi mass splittings of the baryon octet due to up-down (and strange) quark mass differences in terms of the kaon…

High Energy Physics - Lattice · Physics 2013-05-30 R. Horsley , J. Najjar , Y. Nakamura , D. Pleiter , P. E. L. Rakow , G. Schierholz , J. M. Zanotti

SU(3) symmetry relations between the octet baryons are introduced in order to connect both the unpolarized and polarized quark distributions of the octet baryons with those of the nucleon. Two different parametrizations of the nucleon quark…

High Energy Physics - Phenomenology · Physics 2009-11-07 Bo-Qiang Ma , Ivan Schmidt , Jacques Soffer , Jian-Jun Yang

We calculate the sea quark distribution of the nucleon in a meson cloud model. The novel feature of our calculation is the implementation of a special piNN form factor recently obtained by Holzwarth and Machleidt. This form factor is hard…

High Energy Physics - Phenomenology · Physics 2008-11-26 R. J. Fries , A. Schaefer

I review some recent developments in the study of quark flavor distributions in the nucleon, including (i) valence quark distributions and the quark-hadron duality prediction for the x -> 1 d/u ratio (ii) sea quark asymmetries and…

High Energy Physics - Phenomenology · Physics 2007-05-23 W. Melnitchouk

A physical model for parton densities in hadrons, based on Gaussian momentum fluctuations of partons and hadronic baryon-meson fluctuations, is presented. The model has previously been shown to describe proton structure function data, and…

High Energy Physics - Phenomenology · Physics 2007-05-23 Johan Alwall

We give a comprehensive review of concepts and numerical calculations for SU(2) and SU(3) baryonic systems which are considered as many body systems composed of three quarks coupled to a polarized Dirac sea by a Nambu--Jona-Lasinio like…

High Energy Physics - Phenomenology · Physics 2007-05-23 Th. Meissner , E. Ruiz Arriola , A. Blotz , K. Goeke

The strange and antistrange quark distributions of the nucleon are less constrained by experimental data than the non-strange quark sea. The combination of light quark sea distributions, $\Delta(x)=\dbar(x)+\ubar(x)-s(x)-\sbar(x)$,…

High Energy Physics - Phenomenology · Physics 2010-08-26 H. Chen , F. -G. Cao , A. I. Signal

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

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

Parton distributions derived from a chiral quark model that generates an excess of down quarks and antiquarks in the proton's sea satisfactorily describe the measured yields of muon pairs produced in proton-nucleus collisions. Comparison of…

High Energy Physics - Phenomenology · Physics 2009-05-05 Estia J. Eichten , Ian Hinchliffe , Chris Quigg

We derive the nucleon non-perturbative sea-quark distributions coming from a composite model involving quarks and hadronic degrees of freedom. The model predicts a definite structured quark-antiquark asymmetry in the nucleon sea.

High Energy Physics - Phenomenology · Physics 2007-05-23 H. R. Christiansen , J. Magnin

We derive a Menta Carlo method to simulate kinetic equilibrium ensemble, and get the same sea-quark flavor asymmetry as the linear equations method in statistical model. In the recent paper, we introduce the spilt factors to indicate the…

High Energy Physics - Phenomenology · Physics 2010-10-27 Bin Zhang , Yong-Jun Zhang

We present a study of the flavour asymmetry of polarized anti-quarks in the nucleon using the meson cloud model. We include contributions both from the vector mesons and the interference terms of pseudoscalar and vector mesons. Employing…

High Energy Physics - Phenomenology · Physics 2009-01-07 Fu-Guang Cao , A. I. Signal

We show that the chiral $SU(n)\otimes SU(n)$ flavor symmetry on the null-plane severely restricts the sea quarks in the baryon octet. It predicts large asymmetry for the light sea quarks $(u,d,s)$, and universality and abundance for the…

High Energy Physics - Phenomenology · Physics 2007-05-23 Susumu Koretune