{"title":"用QCD求和规则分析d波\\(\\Sigma \\)型粲重子态","authors":"Zhi-Gang Wang, Fei Lu, Yang Liu","doi":"10.1140/epjc/s10052-023-11852-w","DOIUrl":null,"url":null,"abstract":"<div><p>We construct the <span>\\(\\Sigma \\)</span>-type currents to investigate the D-wave charmed baryon states with the QCD sum rules systematically. The predicted masses <span>\\(M=3.35^{+0.13}_{-0.18}\\,\\textrm{GeV}\\)</span> (<span>\\(3.33^{+0.13}_{-0.16}\\,\\textrm{GeV}\\)</span>), <span>\\(3.34^{+0.14}_{-0.18}\\,\\textrm{GeV}\\)</span> (<span>\\(3.35^{+0.13}_{-0.16}\\,\\textrm{GeV}\\)</span>) and <span>\\(3.35^{+0.12}_{-0.13}\\, \\textrm{GeV}\\)</span> (<span>\\(3.35^{+0.12}_{-0.14}\\,\\textrm{GeV}\\)</span>) for the <span>\\(\\Omega _c(0,2,{\\frac{1}{2}}^+)\\)</span>, <span>\\(\\Omega _c(0,2,{\\frac{3}{2}}^+)\\)</span> and <span>\\(\\Omega _c(0,2,{\\frac{5}{2}}^+)\\)</span> states are in excellent agreement with the experimental data <span>\\( 3327.1\\pm 1.2 \\text{ MeV }\\)</span> from the LHCb collaboration, and support assigning the <span>\\(\\Omega _c(3327)\\)</span> to be the <span>\\(\\Sigma \\)</span>-type D-wave <span>\\(\\Omega _c\\)</span> state with the spin-parity <span>\\(J^P={\\frac{1}{2}}^+\\)</span>, <span>\\({\\frac{3}{2}}^+\\)</span> or <span>\\({\\frac{5}{2}}^+\\)</span>.</p></div>","PeriodicalId":788,"journal":{"name":"The European Physical Journal C","volume":"83 8","pages":""},"PeriodicalIF":4.2000,"publicationDate":"2023-08-03","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://link.springer.com/content/pdf/10.1140/epjc/s10052-023-11852-w.pdf","citationCount":"1","resultStr":"{\"title\":\"Analysis of the D-wave \\\\(\\\\Sigma \\\\)-type charmed baryon states with the QCD sum rules\",\"authors\":\"Zhi-Gang Wang, Fei Lu, Yang Liu\",\"doi\":\"10.1140/epjc/s10052-023-11852-w\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<div><p>We construct the <span>\\\\(\\\\Sigma \\\\)</span>-type currents to investigate the D-wave charmed baryon states with the QCD sum rules systematically. The predicted masses <span>\\\\(M=3.35^{+0.13}_{-0.18}\\\\,\\\\textrm{GeV}\\\\)</span> (<span>\\\\(3.33^{+0.13}_{-0.16}\\\\,\\\\textrm{GeV}\\\\)</span>), <span>\\\\(3.34^{+0.14}_{-0.18}\\\\,\\\\textrm{GeV}\\\\)</span> (<span>\\\\(3.35^{+0.13}_{-0.16}\\\\,\\\\textrm{GeV}\\\\)</span>) and <span>\\\\(3.35^{+0.12}_{-0.13}\\\\, \\\\textrm{GeV}\\\\)</span> (<span>\\\\(3.35^{+0.12}_{-0.14}\\\\,\\\\textrm{GeV}\\\\)</span>) for the <span>\\\\(\\\\Omega _c(0,2,{\\\\frac{1}{2}}^+)\\\\)</span>, <span>\\\\(\\\\Omega _c(0,2,{\\\\frac{3}{2}}^+)\\\\)</span> and <span>\\\\(\\\\Omega _c(0,2,{\\\\frac{5}{2}}^+)\\\\)</span> states are in excellent agreement with the experimental data <span>\\\\( 3327.1\\\\pm 1.2 \\\\text{ MeV }\\\\)</span> from the LHCb collaboration, and support assigning the <span>\\\\(\\\\Omega _c(3327)\\\\)</span> to be the <span>\\\\(\\\\Sigma \\\\)</span>-type D-wave <span>\\\\(\\\\Omega _c\\\\)</span> state with the spin-parity <span>\\\\(J^P={\\\\frac{1}{2}}^+\\\\)</span>, <span>\\\\({\\\\frac{3}{2}}^+\\\\)</span> or <span>\\\\({\\\\frac{5}{2}}^+\\\\)</span>.</p></div>\",\"PeriodicalId\":788,\"journal\":{\"name\":\"The European Physical Journal C\",\"volume\":\"83 8\",\"pages\":\"\"},\"PeriodicalIF\":4.2000,\"publicationDate\":\"2023-08-03\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"https://link.springer.com/content/pdf/10.1140/epjc/s10052-023-11852-w.pdf\",\"citationCount\":\"1\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"The European Physical Journal C\",\"FirstCategoryId\":\"4\",\"ListUrlMain\":\"https://link.springer.com/article/10.1140/epjc/s10052-023-11852-w\",\"RegionNum\":2,\"RegionCategory\":\"物理与天体物理\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q2\",\"JCRName\":\"PHYSICS, PARTICLES & FIELDS\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"The European Physical Journal C","FirstCategoryId":"4","ListUrlMain":"https://link.springer.com/article/10.1140/epjc/s10052-023-11852-w","RegionNum":2,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q2","JCRName":"PHYSICS, PARTICLES & FIELDS","Score":null,"Total":0}
Analysis of the D-wave \(\Sigma \)-type charmed baryon states with the QCD sum rules
We construct the \(\Sigma \)-type currents to investigate the D-wave charmed baryon states with the QCD sum rules systematically. The predicted masses \(M=3.35^{+0.13}_{-0.18}\,\textrm{GeV}\) (\(3.33^{+0.13}_{-0.16}\,\textrm{GeV}\)), \(3.34^{+0.14}_{-0.18}\,\textrm{GeV}\) (\(3.35^{+0.13}_{-0.16}\,\textrm{GeV}\)) and \(3.35^{+0.12}_{-0.13}\, \textrm{GeV}\) (\(3.35^{+0.12}_{-0.14}\,\textrm{GeV}\)) for the \(\Omega _c(0,2,{\frac{1}{2}}^+)\), \(\Omega _c(0,2,{\frac{3}{2}}^+)\) and \(\Omega _c(0,2,{\frac{5}{2}}^+)\) states are in excellent agreement with the experimental data \( 3327.1\pm 1.2 \text{ MeV }\) from the LHCb collaboration, and support assigning the \(\Omega _c(3327)\) to be the \(\Sigma \)-type D-wave \(\Omega _c\) state with the spin-parity \(J^P={\frac{1}{2}}^+\), \({\frac{3}{2}}^+\) or \({\frac{5}{2}}^+\).
期刊介绍:
Experimental Physics I: Accelerator Based High-Energy Physics
Hadron and lepton collider physics
Lepton-nucleon scattering
High-energy nuclear reactions
Standard model precision tests
Search for new physics beyond the standard model
Heavy flavour physics
Neutrino properties
Particle detector developments
Computational methods and analysis tools
Experimental Physics II: Astroparticle Physics
Dark matter searches
High-energy cosmic rays
Double beta decay
Long baseline neutrino experiments
Neutrino astronomy
Axions and other weakly interacting light particles
Gravitational waves and observational cosmology
Particle detector developments
Computational methods and analysis tools
Theoretical Physics I: Phenomenology of the Standard Model and Beyond
Electroweak interactions
Quantum chromo dynamics
Heavy quark physics and quark flavour mixing
Neutrino physics
Phenomenology of astro- and cosmoparticle physics
Meson spectroscopy and non-perturbative QCD
Low-energy effective field theories
Lattice field theory
High temperature QCD and heavy ion physics
Phenomenology of supersymmetric extensions of the SM
Phenomenology of non-supersymmetric extensions of the SM
Model building and alternative models of electroweak symmetry breaking
Flavour physics beyond the SM
Computational algorithms and tools...etc.