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Related papers: Newly discovered $\Xi_c^{0}$ resonances and their …

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We systematically study mass spectra and decay properties of $P$-wave $\Xi_c^\prime$ baryons of the $SU(3)$ flavor $\mathbf{6}_F$, using the methods of QCD sum rules and light-cone sum rules within the framework of heavy quark effective…

High Energy Physics - Phenomenology · Physics 2021-01-04 Hui-Min Yang , Hua-Xing Chen , Qiang Mao

We explore the recently observed $\Xi_b(6227)^{-}$ resonance to fix its quantum numbers. To this end, we consider various possible scenarios: It can be considered as either 1P/2S excitations of the $\Xi_b^-$ and $\Xi_b'(5935)^{-}$ ground…

High Energy Physics - Phenomenology · Physics 2018-11-21 T. M. Aliev , K. Azizi , Y. Sarac , H. Sundu

Many excited charmed strange baryons such as $\Xi_c(2790)$, $\Xi_c(2815)$, $\Xi_c(2930)$, $\Xi_c(2980)$, $\Xi_c(3055)$, $\Xi_c(3080)$ and $\Xi_c(3123)$ have been observed. In order to understand their internal structure and to determine…

High Energy Physics - Phenomenology · Physics 2017-12-20 Dan-Dan Ye , Ze Zhao , Ailin Zhang

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

Strong decays of $\Xi_c$ baryons with radial or orbital excitations with positive parity have been studied in a $^3P_0$ model. As candidates of these $Xi_c$, possible configurations and $J^P$ of $\Xi_c(2930)$, $\Xi_c(2980)$, $\Xi_c(3055)$,…

High Energy Physics - Phenomenology · Physics 2017-12-13 Dan-Dan Ye , Ze Zhao , Ailin Zhang

Mass spectra and decay properties of the low-lying orbital excited $\Xi_c^{(\prime)}$ baryons are investigated in the framework of the chiral quark model and quark pair creation mechanism, which are mainly based on the recently experimental…

High Energy Physics - Phenomenology · Physics 2025-09-22 Xiao-Huang Hu , Zhe-Tao Miao , Zi-Xuan Ma , Qi Huang , Yue Tan , Jia-Lun Ping

Recently five $\Omega_c$ excited states have been reported by the LHCb Collaboration, four of them corroborated by Belle. The Belle Collaboration has also discovered in 2017 one excited $\Xi_c$ with mass of 2930 MeV. In view of these recent…

High Energy Physics - Phenomenology · Physics 2019-12-02 L. Tolos , J. Nieves , R. Pavao

We conduct an investigation on the $1P$- and $2P$-wave charmed baryons using the methods of QCD sum rules and light-cone sum rules within the framework of heavy quark effective theory. Our results suggest that the $\Lambda_c(2910)^+$,…

High Energy Physics - Phenomenology · Physics 2023-11-06 Hui-Min Yang , Hua-Xing Chen

Possible spin-parity quantum numbers for excited charmed baryon resonances are discussed in this work. Our main results are: (i) Among the five newly observed $\Omega_c$ states, we have identified $\Omega_c(3090)$ and $\Omega_c(3119)$ with…

High Energy Physics - Phenomenology · Physics 2017-05-31 Hai-Yang Cheng , Cheng-Wei Chiang

The open charm strong decay widths and certain ratio of branching fractions of a charmed strange baryon $\Xi_c(2970)$ are calculated in a $^3P_0$ model. The results are compatible with the latest experimental data. The theoretical ratio of…

High Energy Physics - Phenomenology · Physics 2020-12-30 Ze Zhao

Three neutral resonances $\Xi_c(2923)^0$, $\Xi_c(2939)^0$ and $\Xi_c(2965)^0$ have been observed in the $\Lambda_c^+ K^-$ mass spectrum by the LHCb Collaboration. Given the $\Xi_c$ and $\Xi_c^\prime$ mass spectra predicted by the…

High Energy Physics - Phenomenology · Physics 2020-10-28 Qi-Fang Lü

The LHCb Collaboration recently reported the observation of a new excited bottom baryon $\Xi_b(6227)^0$ and announced an improvement in the measurements related to the previously observed $\Xi_b(6227)^-$ state. We conduct an analysis for…

High Energy Physics - Phenomenology · Physics 2021-04-14 K. Azizi , Y. Sarac , H. Sundu

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

We calculate the masses and residues of triply heavy baryons with spin-3/2, including $\Omega^*_{ccc}$, $\Omega^*_{ccb}$, $\Omega^*_{bbc}$ and $\Omega^*_{bbb}$, using the QCD sum rules method. Our calculations primarily focus on obtaining…

High Energy Physics - Phenomenology · Physics 2025-11-05 Z. Rajabi Najjar , K. Azizi

The strong decays of charm-strange baryons up to N=2 shell are studied in a chiral quark model. The theoretical predictions for the well determined charm-strange baryons, $\Xi_c^*(2645)$, $\Xi_c(2790)$ and $\Xi_c(2815)$, are in good…

High Energy Physics - Phenomenology · Physics 2013-05-30 Lei-Hua Liu , Li-Ye Xiao , Xian-Hui Zhong

The single charmed excited $\Xi_c(2930)$ state was discovered many years ago by BABAR collaboration and recently confirmed by Belle experiment. However, both of these experiments, unfortunately, could not fix the quantum numbers of this…

High Energy Physics - Phenomenology · Physics 2018-10-17 T. M. Aliev , K. Azizi , H. Sundu

We present a study of excited charm-strange baryon states produced in $e^+e^-$ annihilations at or near a center-of-mass energy of $10.58\mathrm{Ge\kern -0.1em V}$, in a data sample with an integrated luminosity of $384 fb^{-1}$ recorded…

High Energy Physics - Experiment · Physics 2010-04-12 The BABAR Collaboration , B. Aubert

We report results from a study of the spin and parity of $\Xi_{c}(2970)^+$ using a $980~\mathrm{fb^{-1}}$ data sample collected by the Belle detector at the KEKB asymmetric-energy $e^{+}e^{-}$ collider. The decay angle distributions in the…

High Energy Physics - Experiment · Physics 2021-06-23 Belle Collaboration , T. J. Moon , K. Tanida , Y. Kato , S. K. Kim , I. Adachi , J. K. Ahn , H. Aihara , S. Al Said , D. M. Asner , V. Aulchenko , T. Aushev , R. Ayad , V. Babu , S. Bahinipati , P. Behera , C. Beleño , J. Bennett , M. Bessner , B. Bhuyan , T. Bilka , J. Biswal , G. Bonvicini , A. Bozek , M. Bračko , T. E. Browder , M. Campajola , L. Cao , D. Červenkov , M. -C. Chang , P. Chang , A. Chen , B. G. Cheon , K. Chilikin , K. Cho , S. -K. Choi , Y. Choi , S. Choudhury , D. Cinabro , S. Cunliffe , N. Dash , G. De Nardo , F. Di Capua , Z. Doležal , T. V. Dong , D. Dossett , S. Dubey , S. Eidelman , D. Epifanov , T. Ferber , B. G. Fulsom , R. Garg , V. Gaur , N. Gabyshev , A. Garmash , A. Giri , P. Goldenzweig , B. Golob , C. Hadjivasiliou , O. Hartbrich , K. Hayasaka , H. Hayashii , M. T. Hedges , W. -S. Hou , C. -L. Hsu , K. Inami , G. Inguglia , A. Ishikawa , R. Itoh , M. Iwasaki , Y. Iwasaki , W. W. Jacobs , S. Jia , Y. Jin , K. K. Joo , K. H. Kang , G. Karyan , T. Kawasaki , H. Kichimi , C. Kiesling , B. H. Kim , D. Y. Kim , K. T. Kim , S. H. Kim , Y. J. Kim , Y. -K. Kim , T. D. Kimmel , K. Kinoshita , P. Kodyš , S. Korpar , D. Kotchetkov , P. Križan , R. Kroeger , P. Krokovny , T. Kuhr , R. Kumar , K. Kumara , A. Kuzmin , I. S. Lee , J. Y. Lee , S. C. Lee , L. K. Li , Y. B. Li , L. Li Gioi , J. Libby , Z. Liptak , D. Liventsev , T. Luo , C. MacQueen , M. Masuda , T. Matsuda , D. Matvienko , M. Merola , K. Miyabayashi , H. Miyata , R. Mizuk , G. B. Mohanty , S. Mohanty , T. Mori , R. Mussa , T. Nakano , M. Nakao , Z. Natkaniec , A. Natochii , M. Nayak , M. Niiyama , N. K. Nisar , S. Nishida , K. Ogawa , S. Ogawa , H. Ono , P. Pakhlov , G. Pakhlova , S. Pardi , H. Park , S. -H. Park , S. Patra , S. Paul , T. K. Pedlar , R. Pestotnik , L. E. Piilonen , T. Podobnik , V. Popov , E. Prencipe , M. T. Prim , M. Ritter , N. Rout , G. Russo , D. Sahoo , Y. Sakai , S. Sandilya , A. Sangal , L. Santelj , V. Savinov , G. Schnell , J. Schueler , C. Schwanda , R. Seidl , Y. Seino , K. Senyo , M. E. Sevior , M. Shapkin , C. P. Shen , J. -G. Shiu , B. Shwartz , E. Solovieva , M. Starič , Z. S. Stottler , M. Sumihama , K. Sumisawa , T. Sumiyoshi , W. Sutcliffe , M. Takizawa , U. Tamponi , F. Tenchini , K. Trabelsi , M. Uchida , S. Uehara , T. Uglov , Y. Unno , S. Uno , P. Urquijo , S. E. Vahsen , R. Van Tonder , G. Varner , A. Vinokurova , V. Vorobyev , A. Vossen , C. H. Wang , E. Wang , M. -Z. Wang , P. Wang , S. Wehle , J. Wiechczynski , X. Xu , B. D. Yabsley , S. B. Yang , H. Ye , J. Yelton , J. H. Yin , C. Z. Yuan , Z. P. Zhang , V. Zhilich , V. Zhukova , V. Zhulanov

We study the charmed and bottomed doubly strange baryons within the heavy-quark-light-diquark framework. The two strange quarks are assumed to lie in $S$ wave and thus their total spin is 1. We calculate the mass spectra of the $S$ and $P$…

High Energy Physics - Phenomenology · Physics 2017-08-02 Wei Wang , Rui-Lin Zhu

In this article, we study the charmed baryon states $\Lambda_c(2625)$ and $\Xi_c(2815)$ with the spin-parity ${3\over 2}^-$ by subtracting the contributions from the corresponding charmed baryon states with the spin-parity ${3\over 2}^+$…

High Energy Physics - Phenomenology · Physics 2015-08-12 Zhi-Gang Wang
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