Instability of the hedgehog shape for the octet baryon in the chiral quark soliton model

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Akiyama, Satoru ; Futami, Yasuhiko (2003)
  • Related identifiers: doi: 10.1103/PhysRevD.67.074030
  • Subject: High Energy Physics - Phenomenology
    arxiv: Nuclear Theory | High Energy Physics::Phenomenology | High Energy Physics::Lattice | Nuclear Experiment | High Energy Physics::Experiment

In this paper the stability of the hedgehog shape of the chiral soliton is studied for the octet baryon with the SU(3) chiral quark soliton model. The strangeness degrees of freedom are treated by a simplified bound-state approach, which omits the locality of the kaon wave function. The mean field approximation for the flavor rotation is applied to the model. The classical soliton changes shape according to the strangeness. The baryon appears as a rotational band of the combined system of the deformed soliton and the kaon.
  • References (27)
    27 references, page 1 of 3

    [4] T. H. R. Skyrme, Proc. R. Soc. London A260, 127 (1961).

    [5] G. Adkin, C. Nappi, and E. Witten, Nucl. Phys. B228, 552 (1983).

    [6] A. P. Balachandran, F. Lizzi, and V. G. J. Rodgers, Nucl. Phys. B256, 525 (1985).

    [7] E. Guadanini, Nucl. Phys. B236, 35 (1984).

    [8] P. O. Mazur, M. A. Nowak, and M. Praszalowicz, Phys. Lett. 147B, 137,(1984).

    [9] H. Yabu and K. Ando, Nucl. Phys. B301, 601 (1988).

    [10] Y. Nambu and G. Jona-Lasinio, Phys. Rev. 122, 345 (1961); 124, 246 (1961).

    [11] D. Ebert and H. Reinhardt, Nucl. Phys. B271, 188 (1986).

    [12] H. Weigel, R. Alkofer, and H. Reinhardt, Nucl. Phys. B387, 638 (1992).

    [13] D. I. Diakonov, V. Yu. Petrov, and P. V. Pobylitsa, Nucl. Phys. B306, 809 (1988).

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