{"title":"The benchmark mode \\(\\Omega _c \\rightarrow \\Omega ^-\\pi ^+\\) and its related processes","authors":"Shuge Zeng, Fanrong Xu, Yu Gu","doi":"10.1140/epjc/s10052-025-13886-8","DOIUrl":null,"url":null,"abstract":"<div><p>The benchmark mode <span>\\(\\Omega _c^0\\rightarrow \\Omega ^- \\pi ^+\\)</span>, which receives purely factorization contribution, is of great importance among all the decay channels of <span>\\(\\Omega _c^0\\)</span> decays. In this work, within the framework of non-relativistic quark model (NRQM), we calculate all the 6 baryon transition form factors involving <span>\\(\\frac{1}{2} ^+\\rightarrow \\frac{3}{2} ^+\\)</span> decays. The absolute branching fractions of non-leptonic decays <span>\\(\\Omega _c^0\\rightarrow \\Omega ^- \\pi ^+\\)</span>, <span>\\(\\Omega _c^0\\rightarrow \\Omega ^- \\rho ^+\\)</span> and <span>\\(\\Omega _c^0\\rightarrow \\Xi ^- \\pi ^+\\)</span> as well as semi-leptonic decays <span>\\(\\Omega _c^0\\rightarrow \\Omega ^- \\ell ^+ \\nu _{\\ell } \\; (\\ell =e,\\mu )\\)</span> are calculated although they cannot be measured directly by current experiment. Based on the prediction <span>\\(\\mathcal {B}(\\Omega _c^0\\rightarrow \\Omega ^-\\pi ^+)=(3.43{\\pm 0.48})\\%\\)</span> in our work, we further predict the ratios between interested modes and the benchmark mode, giving <span>\\(R(\\Xi ^-\\pi ^+)=0.16\\pm {0.06}\\)</span>, <span>\\(R(\\Omega ^-\\rho ^+)=5.33{\\pm 0.94}\\)</span>, <span>\\(R(\\Omega ^- e^+\\nu _e)=1.18{\\pm 0.22}\\)</span> and <span>\\(R(\\Omega ^- \\mu ^+\\nu _\\mu )=1.11{\\pm 0.20}\\)</span>. The predictions on <span>\\(\\Omega _c^0\\rightarrow \\Xi ^-\\pi ^+\\)</span> and <span>\\(\\Omega _c^0\\rightarrow \\Omega ^- e^+\\nu \\)</span> agree well with recent measured ratios reported by LHCb in 2023 and ALICE in 2024, respectively.</p></div>","PeriodicalId":788,"journal":{"name":"The European Physical Journal C","volume":"85 2","pages":""},"PeriodicalIF":4.2000,"publicationDate":"2025-02-14","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://link.springer.com/content/pdf/10.1140/epjc/s10052-025-13886-8.pdf","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"The European Physical Journal C","FirstCategoryId":"4","ListUrlMain":"https://link.springer.com/article/10.1140/epjc/s10052-025-13886-8","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}
引用次数: 0
Abstract
The benchmark mode \(\Omega _c^0\rightarrow \Omega ^- \pi ^+\), which receives purely factorization contribution, is of great importance among all the decay channels of \(\Omega _c^0\) decays. In this work, within the framework of non-relativistic quark model (NRQM), we calculate all the 6 baryon transition form factors involving \(\frac{1}{2} ^+\rightarrow \frac{3}{2} ^+\) decays. The absolute branching fractions of non-leptonic decays \(\Omega _c^0\rightarrow \Omega ^- \pi ^+\), \(\Omega _c^0\rightarrow \Omega ^- \rho ^+\) and \(\Omega _c^0\rightarrow \Xi ^- \pi ^+\) as well as semi-leptonic decays \(\Omega _c^0\rightarrow \Omega ^- \ell ^+ \nu _{\ell } \; (\ell =e,\mu )\) are calculated although they cannot be measured directly by current experiment. Based on the prediction \(\mathcal {B}(\Omega _c^0\rightarrow \Omega ^-\pi ^+)=(3.43{\pm 0.48})\%\) in our work, we further predict the ratios between interested modes and the benchmark mode, giving \(R(\Xi ^-\pi ^+)=0.16\pm {0.06}\), \(R(\Omega ^-\rho ^+)=5.33{\pm 0.94}\), \(R(\Omega ^- e^+\nu _e)=1.18{\pm 0.22}\) and \(R(\Omega ^- \mu ^+\nu _\mu )=1.11{\pm 0.20}\). The predictions on \(\Omega _c^0\rightarrow \Xi ^-\pi ^+\) and \(\Omega _c^0\rightarrow \Omega ^- e^+\nu \) agree well with recent measured ratios reported by LHCb in 2023 and ALICE in 2024, respectively.
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.