{"title":"Unified study of nucleon and $Δ$ baryon spectra and their strong decays with chiral dynamics","authors":"Hui-Hua Zhong, Ming-Sheng Liu, Ru-Hui Ni, Mu-Yang Chen, Xian-Hui Zhong, Qiang Zhao","doi":"arxiv-2409.07998","DOIUrl":null,"url":null,"abstract":"In this work we systematically study both the mass spectra and strong decays\nof the nucleon and $\\Delta$ resonances up to the $N=2$ shell within a unified\nquark model framework with chiral dynamics. In this framework we achieve a good\ndescription of the strong decay properties of the well-established nucleon and\n$\\Delta$ resonances. Meanwhile, the mass reversal between $N(1440)1/2^{+}$ as\nthe first radial excitation state and the $1P$-wave nucleon resonances can be\nexplained. We show that the three-body spin-orbit potential arising from the\none-gluon exchange can cause a large configuration mixing between\n$N(1520)3/2^-$ and $N(1700)3/2^-$, and is also responsible for the large\nsplitting between $\\Delta(1600)1/2^-$ and $\\Delta(1700)1/2^-$. Some of these\nbaryon resonances turn to weakly couple to the $N\\pi$, $N\\eta$, $K\\Lambda$, and\n$K\\Sigma$ channels, which may answer the question why they have not been\nestablished in these channels via the $\\pi N$ and $\\gamma N$ scatterings. It\nshows that these ``missing resonances\" may have large potentials to be\nestablished in the $N\\pi\\pi$ final state due to their large decay rates into\neither the $\\Delta(1232)$ or $1P$-wave nucleon resonances via the pionic\ndecays. Further experimental search for their signals in charmonium decays at\nBESIII is thus strongly recommended.","PeriodicalId":501573,"journal":{"name":"arXiv - PHYS - Nuclear Theory","volume":"58 1","pages":""},"PeriodicalIF":0.0000,"publicationDate":"2024-09-12","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"arXiv - PHYS - Nuclear Theory","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/arxiv-2409.07998","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 0
Abstract
In this work we systematically study both the mass spectra and strong decays
of the nucleon and $\Delta$ resonances up to the $N=2$ shell within a unified
quark model framework with chiral dynamics. In this framework we achieve a good
description of the strong decay properties of the well-established nucleon and
$\Delta$ resonances. Meanwhile, the mass reversal between $N(1440)1/2^{+}$ as
the first radial excitation state and the $1P$-wave nucleon resonances can be
explained. We show that the three-body spin-orbit potential arising from the
one-gluon exchange can cause a large configuration mixing between
$N(1520)3/2^-$ and $N(1700)3/2^-$, and is also responsible for the large
splitting between $\Delta(1600)1/2^-$ and $\Delta(1700)1/2^-$. Some of these
baryon resonances turn to weakly couple to the $N\pi$, $N\eta$, $K\Lambda$, and
$K\Sigma$ channels, which may answer the question why they have not been
established in these channels via the $\pi N$ and $\gamma N$ scatterings. It
shows that these ``missing resonances" may have large potentials to be
established in the $N\pi\pi$ final state due to their large decay rates into
either the $\Delta(1232)$ or $1P$-wave nucleon resonances via the pionic
decays. Further experimental search for their signals in charmonium decays at
BESIII is thus strongly recommended.