Analysis of $$\Omega _c(3000)$$ Ω c ( 3000 ) , $$\Omega _c(3050)$$ Ω c ( 3050 ) , $$\Omega _c(3066)$$ Ω c ( 3066 ) , $$\Omega _c(3090)$$ Ω c ( 3090 ) and $$\Omega _c(3119)$$ Ω c ( 3119 ) with QCD sum rules

Study of Ω 0 c and Ω∗0 c

We report results from a study of the charmed double strange baryons Ωc and Ω ∗0 c at Belle. The Ωc is reconstructed using the Ω 0 c → Ω π decay mode, and its mass is measured to be (

( bss ) and Ω 0 c ( css ) with QCD sum rules

In this article, we calculate the masses and the pole residues of the 1 2 + heavy baryons Ω0c(css) and Ω − b (bss) with the QCD sum rules. The numerical values MΩ0c = (2.72 ± 0.18)GeV and Ωb = (6.13 ± 0.12)GeV are in good agreement with the experimental data. PACS number: 14.20.Lq, 14.20.Mr

Ω 0 c ( css ) with QCD sum rules

In this article, we calculate the masses and the pole residues of the 1 2 + heavy baryons Ω0c(css) and Ω − b (bss) with the QCD sum rules. The numerical values Ωc = (2.72 ± 0.18)GeV (or Ωc = (2.71 ± 0.18)GeV) and Ωb = (6.13 ± 0.12)GeV (or M Ω − b = (6.18 ± 0.13)GeV) are in good agreement with the experimental data. PACS number: 14.20.Lq, 14.20.Mr

BELLE-CONF-0851 Study of Ω 0 c and Ω ∗0 c

We report results from a study of the charmed double strange baryons Ωc and Ω ∗0 c at Belle. The Ωc is reconstructed using the Ω 0 c → Ω π decay mode, and its mass is measured to be (

Operators on C(ω α ) which do not preserve C(ω α