{"title":"核子和 $Δ$ 重子光谱及其手性动力学强衰变的统一研究","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":"{\"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}","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}
Unified study of nucleon and $Δ$ baryon spectra and their strong decays with chiral dynamics
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.