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      Nonrigid chiral soliton for the octet and decuplet baryons

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          Abstract

          Systematic treatment of the collective rotation of the nonrigid chiral soliton is developed in the SU(3) chiral quark soliton model and applied to the octet and decuplet baryons. The strangeness degrees of freedom are treated by a simplified bound-state approach which omits the locality of the kaon wave function. Then, the flavor rotation is divided into the isospin rotation and the emission and absorption of the kaon. The kaon Hamiltonian is diagonalized by the Hartree approximation. The soliton changes the shape according to the strangeness. The baryons appear as the rotational bands of the combined system of the soliton and the kaon.

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          Author and article information

          Journal
          01 October 2003
          Article
          10.1103/PhysRevD.69.014001
          hep-ph/0310015
          5ab0d267-aeea-4e86-9e0d-a8254271a797
          History
          Custom metadata
          Phys.Rev. D69 (2004) 014001
          11 pages(LaTex), 1 figures(eps)
          hep-ph

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