5 research outputs found

    Influence of tensor interactions on masses and decay widths of dibaryons

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    The influence of gluon and Goldstone boson induced tensor interactions on the dibaryon masses and D-wave decay widths has been studied in the quark delocalization, color screening model. The effective S-D wave transition interactions induced by gluon and Goldstone boson exchanges decrease rapidly with increasing strangeness of the channel. The tensor contribution of K and η\eta mesons is negligible in this model. There is no six-quark state in the light flavor world studied so far that can become bound by means of these tensor interactions besides the deuteron. The partial D-wave decay widths of the IJp=1/22+IJ^p={1/2}2^+ NΩ\Omega state to spin 0 and 1 ΛΞ\Lambda\Xi final states are 12.0 keV and 21.9 keV respectively. This is a very narrow dibaryon resonance that might be detectable in relativistic heavy ion reactions by existing RHIC detectors through the reconstruction of the vertex mass of the decay product ΛΞ\Lambda\Xi and by the COMPAS detector at CERN or at JHF in Japan and the FAIR project in Germany in the future.Comment: 19 pages, 5 figure

    An alternative approach to the σ\sigma-meson-exchange in nucleon-nucleon interaction

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    Through a quantitative comparative study of the properties of deuteron and nucleon-nucleon interaction with chiral quark model and quark delocalization color screening model. We show that the σ\sigma-meson exchange used in the chiral quark model can be replaced by quark delocalization and color screening mechanism.Comment: 4 pages, 4 figure

    The d* dibaryon in the extended quark-delocalization, color-screening model

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    The quark-delocalization, color-screening model, extended by inclusion of a one-pion-exchange (OPE) tail, is applied to the study of the deuteron and the d* dibaryon. The results show that the properties of the deuteron (an extended object) are well reproduced, greatly improving the agreement with experimental data as compared to our previous study (without OPE). At the same time, the mass and decay width of the d* (a compact object) are, as expected, not altered significantly.Comment: 9 pages, no figures, LaTeX, subm. to Phys. Rev.
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