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      Parity of Anti-Decuplet Baryons Revisited from Chiral Soliton Models

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          Abstract

          We recalculate masses and widths of anti-decuplet baryons in the case of positive parity from chiral soliton models, provided that the member \(\Xi_{3/2}\) of the anti-decuplet has a mass 1.86 GeV as reported recently. Calculations show that there are no convincing candidates for the nonexotic members of the anti-decuplet available in the baryon listings. Up to the leading order of \(m_s\) and 1/\(N_c\), the width formula for the decay of the anti-decuplet baryons to the octet depends only on SU(3) symmetry model-independently, except the coupling constant. Similarly we give a width formula for the decay of negative parity baryons belong to certain SU(3) baryon multiplet by pure symmetry consideration. By this formula, we find that if we have an anti-decuplet with negative parity and that the masses are the same as those given by chiral soltion models, the identification of N(1650) as \(N_{\bar{10}}\) are inconsistent with experiments for \(N(1650)\to N\pi\) while the widths agree with other two decay channels involving strangeness. And \(\Sigma(1750)\) seems to be a reasonable candidate for \(\Sigma_{\bar{10}}\).

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          Nonstrange and other unitarity partners of the exotic Theta+ baryon

          Given presently known empirical information about the exotic Theta+ baryon, we analyze possible properties of its SU(3)F partners, paying special attention to the nonstrange member of the antidecuplet N*. The modified PWA analysis presents two candidate masses, 1680 MeV and 1730 MeV. In both cases the N* should be highly inelastic. The theoretical analysis, based on the soliton picture and assumption of Gamma(Theta+) < 5 MeV, shows that most probably Gamma(N*) < 30 MeV. Similar analysis for Xi3/2 predicts its width to be not more than about 10 MeV. Our results suggest several directions for experimental studies that may clarify properties of the antidecuplet baryons, and structure of their mixing with other baryons.
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            Exotic baryon multiplets at large number of colours

            We generalize the usual octet, decuplet and exotic antidecuplet and higher baryon multiplets to any number of colours Nc. We show that the multiplets fall into a sequence of bands with O(1/Nc) splittings inside the band and O(1)splittings between the bands characterized by "exoticness", that is the number of extra quark-antiquark pairs needed to compose the multiplet. Each time one adds a pair the baryon mass is increased by the same constant which can be interpreted as a mass of a quark-antiquark pair. At the same time, we prove that masses of exotic rotational multiplets are reliably determined at large Nc from collective quantization of chiral solitons.
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              The 27-plet Baryons from Chiral Soliton Models

              We use the perturbation method to calculate the masses and widths for 27-plet baryons with spin 3/2 from chiral soliton models. According to the masses and quantum numbers, we find all the candidates for non-exotic members of 27-plet. The calculation of the widths shows that these candidates manifest an approximate symmetry of the 27 representation of the SU(3) group, and the quantum numbers of \(\Xi(1950)\) seem to be \(I(J^P)={1/2}({3/2}^+)\). Up to leading order of the strange quark mass, we find that the exotic members have widths much larger than those of the anti-decuplet members.
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                Author and article information

                Journal
                25 November 2003
                2004-07-19
                Article
                10.1103/PhysRevD.70.097503
                hep-ph/0311331
                c754d776-eab2-42ab-a1bb-175ed9986a60
                History
                Custom metadata
                Phys.Rev.D70:097503,2004
                4 pages in revtex format, version for journal publication. Arguments revised, with conclusion unchanged
                hep-ph hep-ex nucl-ex nucl-th

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