Quasi-two-body decays of nonstrange baryons.

New Baryons in the and ! Channels

The decays of excited nonstrange baryons into the final states ∆η and ∆ω are examined in a relativized quark pair creation model. The wavefunctions and parameters of the model are fixed by previous calculations of Nπ and Nππ, etc., decays through various quasi-two body channels including Nη and Nω. Our results show that the combination of thresholds just below the region of interest and the iso...

Strange Decays of Nonstrange Baryons

The strong decays of excited nonstrange baryons into the final states ΛK, ΣK, and for the first time into Λ(1405)K, Λ(1520)K, Σ(1385)K, ΛK∗, and ΣK∗, are examined in a relativized quark pair creation model. The wave functions and parameters of the model are fixed by previous calculations of Nπ and Nππ, etc., decays. Our results show that it should be possible to discover several new negative pa...

Strong Decays of Nonstrange Q I Introduction Ii Method of Calculation

We study strong decays of nonstrange baryons by making use of the algebraic approach to hadron structure. Within this framework we derive closed expressions for decay widths in an elementary-meson emission model and use these to analyze the experimental data for N A large amount of experimental data was accumulated in the 1960's and 1970's on the spectroscopy of light hadrons. These data led fi...

ar X iv : n uc l - th / 9 60 80 57 v 2 1 8 N ov 1 99 6 Strong decays of nonstrange q 3 baryons

A SU ( 4 ) ⊗ O ( 3 ) scheme for nonstrange baryons

A SU (4) ⊗ O(3) scheme for nonstrange baryons Abstract. We show that nonstrange baryon resonances can be classified according to multiplets of SU (4)⊗ O(3). We identify spectral regularities and degeneracies that allow us to predict the high spin spectrum from 2 to 3 GeV.