2007/06/30 by L. Ya. Glozman · 1 citation
Physics and Astronomy · #High-Energy Particle Collisions Research #Particle physics theoretical and experimental studies #Quantum Chromodynamics and Particle Interactions #hep-ex #hep-ph #nucl-ex #nucl-th
paper · pdf · doi:10.1103/physrevlett.99.191602
published as Phys.Rev.Lett.99:191602,2007 · 4 pp. A new footnote with an alternative proof of impossibility of parity doublet decay into pi + N is added. To appear in Phys. Rev. Lett
arxiv created 2007/09/25 · openalex publication_date 2007/11/09 · arxiv updated 2009/12/01 · openalex created_date 2025/10/10 · openalex updated_date 2026/07/28
It has been suggested that chiral symmetry is approximately restored in excited hadrons at zero temperature and density (effective symmetry restoration). Using very general chiral symmetry arguments, it is shown that those excited nucleons that are assumed from the spectroscopic patterns to be in approximate chiral multiplets must only weakly decay into the Npi channel, (fN*Npi/fNNpi)(2) << 1. However, those baryons that have no chiral partner must decay strongly with a decay constant comparable with fNNpi. It turns out that for all those well-established excited nucleons which can be classified into chiral doublets the ratio is (fN*Npi/fNNpi)(2) approximately 0.1 or much smaller for the high-spin states. In contrast, the only well-established excited nucleon for which the chiral partner cannot be identified from the spectroscopic data, N(1520), has a decay constant into the Npi channel that is comparable with fNNpi.