Selection Rule for <span class="aps-inline-formula"><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><mi>P</mi></math></span>-Wave Nonleptonic Hyperon Decays as a Consequence of Duality

Mahiko Suzuki

doi:10.1103/PhysRevLett.22.1217

Selection Rule for $P$ -Wave Nonleptonic Hyperon Decays as a Consequence of Duality

Department of Physics, University of Tokyo, Tokyo, Japan

Phys. Rev. Lett. 22, 1217 – Published 2 June, 1969Errata Phys. Rev. Lett. 22, 1413 (1969); Phys. Rev. Lett. 23, 109 (1969)

DOI: https://doi.org/10.1103/PhysRevLett.22.1217

Abstract

A selection rule for $p$ -wave amplitudes of nonleptonic hyperon decays is derived from the duality principle. It predicts $P (Σ_{-}^{-}) = 0$ and $P (Ω^{-} \to Ξ_{π}) = 0$ .

Errata

Selection Rule for $P$ -Wave Nonleptonic Hyperon Decays as a Consequence of Duality

Mahiko Suzuki

Phys. Rev. Lett. 22, 1413 (1969)

Selection Rule for Nonleptonic Hyperon Decays as a Consequence of Duality

Mahiko Suzuki

Phys. Rev. Lett. 23, 109 (1969)

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Selection Rule for $P$ -Wave Nonleptonic Hyperon Decays as a Consequence of Duality

Abstract

Errata

Selection Rule for $P$ -Wave Nonleptonic Hyperon Decays as a Consequence of Duality

Selection Rule for Nonleptonic Hyperon Decays as a Consequence of Duality

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Selection Rule for P-Wave Nonleptonic Hyperon Decays as a Consequence of Duality

Abstract

Errata

Selection Rule for P-Wave Nonleptonic Hyperon Decays as a Consequence of Duality

Selection Rule for Nonleptonic Hyperon Decays as a Consequence of Duality

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Selection Rule for $P$ -Wave Nonleptonic Hyperon Decays as a Consequence of Duality

Selection Rule for $P$ -Wave Nonleptonic Hyperon Decays as a Consequence of Duality