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Nonleptonic decay

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Il Nuovo Cimento (1955-1965)

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References

  1. Riazuddin:Nuoro Cimento, in press; hereafter it will be called I.

  2. M. Gell-Mann:Phys. Rev.,125, 1067 (1962); California Institute of Technology Snychrotron Laboratory Report No. CTSL 20 (1961) (unpublished);Y. Ne’eman:Nucl. Phys.,26, 222 (1961);S. Okubo:Prog. Theor. Phys.,27, 969 (1962). Our strangeness-changing vector current is assumed to beF-type. By broken symmetry we mean that the particles concerned have their physical masses related by the Gell-Mann-Okubo formula.

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  3. M. L. Goldberger andS. B. Treiman:Phys. Rev.,110, 1178 (1958).

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  6. Y. Hara:Phys. Rev. Lett.,12, 378 (1964). Hara has considered baryon resonances. An alternative possibility is to introduce a strange pseudovector resonance with onlyD-type coupling to get right signs ofp-wave amplitudes. Such a resonance will not contribute to thes-wave part.

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Author notes

  1. A. H. Zimerman

    Present address: the Instituto de Fisica Teorica, Sao Paulo, Brazil

Authors and Affiliations

  1. Department of Physics and Astronomy, University of Rochester, Rochester, N. Y.

    Riazuddin & A. H. Zimerman

  2. Atomic Energy Centre, Lahore

    Fayyazuddin

Authors
  1. Riazuddin
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  2. A. H. Zimerman
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  3. Fayyazuddin
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Additional information

Work supported by the U. S. Atomic Energy Commission for the first two authors.

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Riazuddin, Zimerman, A.H. & Fayyazuddin Nonleptonic decay. Nuovo Cim 32, 1819–1822 (1964). https://doi.org/10.1007/BF02732815

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  • DOI: https://doi.org/10.1007/BF02732815

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