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Related papers: Investigation on the $\Omega(2012)$ from QCD sum r…

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We investigate the recently observed $\Omega(2012)$ baryon using QCD sum rules. By constructing $P$-wave $\Omega$ baryon currents and performing spin projection and parity projection, we obtain the masses of the $J^P = 1/2^-$ and $3/2^-$…

High Energy Physics - Phenomenology · Physics 2024-10-01 Niu Su , Hua-Xing Chen , Philipp Gubler , Atsushi Hosaka

Using the QCD sum rule method, we investigate the mass splitting for the spin-orbit partner states of the $\Omega(2012)$ baryon assuming that it is a $P$-wave excitation with $J^P=3/2^-$. This study is an extension of the previous work [1]…

High Energy Physics - Phenomenology · Physics 2025-10-03 Niu Su , Hua-Xing Chen , Philipp Gubler , Atsushi Hosaka

Very recently Belle Collaboration reported observation of a narrow state called $\Omega(2012)$ with mass $2012.4 \pm 0.7$~(stat)~$\pm 0.6$(syst)~MeV and width $6.4^{+2.5}_{-2.0}$~(stat)~$\pm 1.6$~(syst)~MeV. We calculate the mass and…

High Energy Physics - Phenomenology · Physics 2018-08-01 T. M. Aliev , K. Azizi , Y. Sarac , H. Sundu

Inspired by the newly observed $\Omega(2012)$ state at Belle II, we investigate the two-body strong decays of $\Omega$ baryons up to $N=2$ shell within the chiral quark model. Our results indicate that: (i) the newly observed $\Omega(2012)$…

High Energy Physics - Phenomenology · Physics 2018-08-08 Li-Ye Xiao , Xian-Hui Zhong

We calculate the mass and residue of the newly observed $\Omega_c(3000)$ and $\Omega_c(3066)$ states with quantum numbers $J^P = \frac{1}{2}^{-}$ and $\frac{3}{2}^{-}$ within QCD sum rules. Our predictions on masses are in good agreement…

High Energy Physics - Phenomenology · Physics 2020-01-29 T. M. Aliev , S. Bilmis , M. Savci

The present study provides spectroscopic investigations of spin-$\frac{3}{2}$ $\Lambda$ baryons with both positive and negative parities. The analysis mainly focuses on three states, namely $1P$, $2P$, and $2S$, and corresponding masses are…

High Energy Physics - Phenomenology · Physics 2024-04-15 K. Azizi , Y. Sarac , H. Sundu

The masses of the flavor octet and singlet baryons with negative parity and spin 1/2 are calculated using the QCD sum rule. We find that the chiral symmetry breaking vacuum condensates cause the mass splitting of the positive and negative…

High Energy Physics - Phenomenology · Physics 2008-02-03 D. Jido , M. Oka

The masses and residues of the radially excited heavy $\Omega_c^{0}$ and $ \Omega_b^{-}$ baryons with spin-parity $J^{P}=\frac{1}{2}^{+}$ and $J^{P}= \frac{3}{2}^{+}$ are calculated by means of QCD two-point sum rule method using the…

High Energy Physics - Phenomenology · Physics 2017-09-13 S. S. Agaev , K. Azizi , H. Sundu

Recently, a new excited baryon state, $\Omega(2012)$, was observed in the invariant mass spectra of $K^-\Xi^0$ and $K^0_S \Xi^-$ by the Belle Collaboration. This state has a narrow width ($\sim 6$ MeV) compared to other baryon states with a…

High Energy Physics - Phenomenology · Physics 2024-06-26 Ju-Jun Xie , Li-Sheng Geng

The mass and pole residue of the ground and first radially excited $ \Omega_c^{0}$ states with spin-parities $J^{P}=1/2^{+},\,3/2^{+}$, as well as P-wave $\Omega_c^{0}$ with $J^{P}=1/2^{-},\,3/2^{-}$ are calculated by means of the two-point…

High Energy Physics - Phenomenology · Physics 2017-06-28 S. S. Agaev , K. Azizi , H. Sundu

We present an exploratory lattice QCD analysis of the $ \Omega $-baryon spectrum. Using smeared three-quark operators in a correlation matrix analysis, we report masses for the ground, first and second excited states of the $ J^P =…

High Energy Physics - Lattice · Physics 2024-08-30 Liam Hockley , Waseem Kamleh , Derek Leinweber , Anthony Thomas

We extend our previous analysis on the mass of the recently discovered $\Omega(2012)$ state by investigation of its strong decays and calculation of its width employing the method of light cone QCD sum rule. Considering two possibilities…

High Energy Physics - Phenomenology · Physics 2018-11-14 T. M. Aliev , K. Azizi , Y. Sarac , H. Sundu

We construct the $\Sigma$-type currents to investigate the D-wave charmed baryon states with the QCD sum rules systematically. The predicted masses $M=3.35^{+0.13}_{-0.18}\,\rm{GeV}$ ($3.33^{+0.13}_{-0.16}\,\rm{GeV}$),…

High Energy Physics - Phenomenology · Physics 2023-08-04 Zhi-Gang Wang , Fei Lu , Yang Liu

We present the ground and excited state spectra of $\Omega^{0}_{c}$ baryons with spin up to 7/2 from lattice quantum chromodynamics with dynamical quark fields. Based on our lattice results, we predict the quantum numbers of five…

High Energy Physics - Phenomenology · Physics 2017-08-02 M. Padmanath , Nilmani Mathur

In this article, we distinguish the contributions of the positive parity and negative parity $\Omega_c$ states, study the masses and pole residues of the 1S, 1P, 2S and 2P $\Omega_c$ states with the spin $J=\frac{1}{2}$ and $\frac{3}{2}$…

High Energy Physics - Phenomenology · Physics 2017-12-11 Zhi-Gang Wang , Xing-Ning Wei , Ze-Hui Yan

Masses and couplings of the negative parity excited baryons are studied in the QCD sum rule. Separation of the negative-parity spectrum is proposed and is applied to the flavor octet and singlet baryons. We find that the quark condensate is…

High Energy Physics - Phenomenology · Physics 2015-06-25 M. Oka , D. Jido , A. Hosaka

The QCD sum rule method is formulated for the strangeness +1 pentaquark baryon with isospin I=0 and spin-parity J^P = 3/2^\pm. The spin-3/2 states are considered to be narrower than the spin-1/2 ones, and thus may provide a natural…

High Energy Physics - Phenomenology · Physics 2014-11-18 P. Gubler , D. Jido , T. Kojo , T. Nishikawa , M. Oka

We use the QCD sum rule approach to calculate the masses of the Lambda_Q and Sigma_Q baryons to the Lambda_{QCD}/m_Q order within the framework of heavy quark effective theory. We compare the direct approach and the covariant approach to…

High Energy Physics - Phenomenology · Physics 2009-11-07 Dao-Wei Wang , Ming-Qiu Huang , Cheng-Zu Li

The strong coupling constants of newly observed $\Omega_c^0$ baryons with spin $J = \frac{1}{2}$ and $J = \frac{3}{2}$ decaying into $\Xi_c^{+} K^{-}$ are estimated within light cone QCD sum rules. The calculations are performed within two…

High Energy Physics - Phenomenology · Physics 2018-05-09 T. M. Aliev , S. Bilmis , M. Savci

We investigate the mass and strong decay properties of the $\Omega(2012)$ resonance using QCD sum rules, assuming it to be an S-wave $\Xi(1530)\bar{K}$ molecular pentaquark state with $I(J^{P})= 0(\frac{3}{2}^{-})$. A unified interpolating…

High Energy Physics - Phenomenology · Physics 2026-05-14 Xiang Yu , Jin-Peng Zhang , Xu-Liang Chen , Ding-Kun Lian , Qi-Nan Wang , Wei Chen
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