1992Physical review. D. Particles, fields, gravitation, and cosmology/Physical review. D. Particles and fieldsRequires access

The η -baryon octet

S. F. Tuan

Open publisher page 2 citations

Abstract

The recent tantalizing experimental support for an $\ensuremath{\eta}$-baryon ${J}^{P}={\frac{1}{2}}^{\ensuremath{-}}$ unmixed octet challenges conventional model wisdom. The establishment of the $\ensuremath{\Xi}(1868)$ member of the $\ensuremath{\eta}$ octet will give strong affirmation that the negative-parity baryon mass spectrum could be mixing-free.

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What this paper is about

The recent tantalizing experimental support for an $\ensuremath{\eta}$-baryon ${J}^{P}={\frac{1}{2}}^{\ensuremath{-}}$ unmixed octet challenges conventional model wisdom. The establishment of the $\ensuremath{\Xi}(1868)$ member of the $\ensuremath{\eta}$ octet will give strong affirmation that the negative-parity baryon mass spectrum could be mixing-free.

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Available abstract

The recent tantalizing experimental support for an $\ensuremath{\eta}$-baryon ${J}^{P}={\frac{1}{2}}^{\ensuremath{-}}$ unmixed octet challenges conventional model wisdom. The establishment of the $\ensuremath{\Xi}(1868)$ member of the $\ensuremath{\eta}$ octet will give strong affirmation that the negative-parity baryon mass spectrum could be mixing-free.

Key concepts: Octet, Baryon, Physics, Particle physics, Parity (physics), Mixing (physics), Hyperon, Nuclear physics

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