632 research outputs found

    Perturbative and nonperturbative contributions to the strange quark asymmetry in the nucleon

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    There are two mechanisms for the generation of an asymmetry between the strange and anti-strange quark distributions in the nucleon: nonperturbative contributions originating from nucleons fluctuating into virtual baryon-meson pairs such as ΛK\Lambda K and ΣK\Sigma K, and perturbative contributions arising from gluons splitting into strange and anti-strange quark pairs. While the nonperturbative contributions are dominant in the large-xx region, the perturbative contributions are more significant in the small-xx region. We calculate this asymmetry taking into account both nonperturbative and perturbative contributions, thus giving a more accurate evaluation of this asymmetry over the whole domain of xx. We find that the perturbative contributions are generally a few times larger in magnitude than the nonperturbative contributions, which suggests that the best region to detect this asymmetry experimentally is in the region 0.02<x<0.030.02 < x < 0.03. We find that the asymmetry may have more than one node, which is an effect that should be taken into account, e.g. for parameterizations of the strange and anti-strange quark distributions used in global analysis of parton distributions.Comment: 14 pages, 4 figures, figures comparing theoretical calculations with NNPDF global analysis added, accepted for publication in EPJ

    Non-perturbative structure of the polarized nucleon sea

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    We investigate the flavour and quark-antiquark structure of the polarized nucleon by calculating the parton distribution functions of the nucleon sea using the meson cloud model. We find that the SU(2) flavor symmetry in the light antiquark sea and quark-antiquark symmetry in the strange quark sea are broken, {\it i.e.} \Delta\ubar < \Delta \dbar and \Delta s < \Delta \sbar. The polarization of the strange sea is found to be positive, which is in contradiction to previous analyses. We predict a much larger quark-antiquark asymmetry in the polarized strange quark sea than that in the unpolarized strange quark sea. Our results for both polarized light quark sea and polarized strange quark sea are consistent with the recent HERMES data.Comment: RevTex, 17 pages plus 8 PS figure

    Light quark distributions in the proton sea

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    We use the meson cloud model to calculate dˉ(x)uˉ(x)\bar{d}(x) - \bar{u}(x) and dˉ(x)/uˉ(x) \bar{d}(x)/\bar{u}(x) in the proton. We show that a modification of the symmetric, perturbative part of the light quark sea provides better agreement with the ratio $ \bar{d}(x)/\bar{u}(x).Comment: 4 pages, 2 figures, LaTeX. Talk presented at PANIC 9

    The Flavor Asymmetry of the Nucleon Sea

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    We re-examine the effects of anti-symmetry on the anti-quarks in the nucleon sea arising from gluon exchange and pion exchange between confined quarks. While the effect is primarily to suppress anti-down relative to anti-up quarks, this is numerically insignificant for the pion terms.Comment: To appear in Phys. Rev.

    Parton Distributions for the Octet and Decuplet Baryons

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    We calculate the parton distributions for both polarized and unpolarized octet and decuplet baryons, using the MIT bag, dressed by mesons. We show that the hyperfine interaction responsible for the ΔN\Delta - N and Σ0Λ\Sigma^0 - \Lambda splittings leads to large deviations from SU(3) and SU(6) predictions. For the Λ\Lambda we find significant polarized, non-strange parton distributions which lead to a sizable Λ\Lambda polarization in polarized, semi-inclusive epep scattering. We also discuss the flavour symmetry violation arising from the meson-cloud associated with the chiral structure of baryons.Comment: 29 pages, 15 figure

    Omega Meson Cloud and the Proton's Light Anti-Quark Distribution

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    We use the meson cloud model of the nucleon to calculate distribution functions for (dˉuˉ)(\bar {d} - \bar{u}) and dˉ/uˉ \bar{d}/\bar{u} in the proton. Including the effect of the omega meson cloud, with a coupling constant gω2/4π8g_\omega^2/4\pi\approx 8, allows a reasonably good description of the data.Comment: 6 pages, 2 figures, LaTe

    Nucleon Structure Functions from a Chiral Soliton in the Infinite Momentum Frame

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    We study the frame dependence of nucleon structure functions obtained within a chiral soliton model for the nucleon. Employing light cone coordinates and introducing collective coordinates together with their conjugate momenta, translational invariance of the solitonic quark fields (which describe the nucleon as a localized object) is restored. This formulation allows us to perform a Lorentz boost to the infinite momentum frame of the nucleon. The major result is that the Lorentz contraction associated with this boost causes the leading twist contribution to the structure functions to properly vanish when the Bjorken variable xx exceeds unity. Furthermore we demonstrate that for structure functions calculated in the valence quark approximation to the Nambu--Jona--Lasinio chiral soliton model the Lorentz contraction also has significant effects on the structure functions for moderate values of the Bjorken variable xx.Comment: 16 pages, 1 figure, revised version to be published in Int. J. Mod. Phys.

    On the Flavor Structure of the Constituent Quark

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    We discuss the dressing of constituent quarks with a pseudoscalar meson cloud within the effective chiral quark model. SU(3) flavor symmetry breaking effects are included explicitly. Our results are compared with those of the traditional meson cloud approach in which pions are coupled to the nucleon. The pionic dressing of the constituent quarks explains the experimentally observed violation of the Gottfried Sum Rule and leads to an enhanced nonperturbative sea of quark-antiquark pairs in the constituent quark and consequently in the nucleon. We find 2.5 times more pions and 10-15 times more kaons in the nucleon than in the traditional picture.Comment: 7 pages, LaTeX, 4 Postscript figures, to appear in J. Phys.
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