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Related papers: Excited Baryon Production and Decays

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We consider the strong decays of the lowest-lying radially excited baryons, in SU(6) language the states comprising the first excited 56-plet. Assuming a single-quark decay approximation, and negligible configuration mixing, we make…

High Energy Physics - Phenomenology · Physics 2009-10-31 Carl E. Carlson , Christopher D. Carone

We consider decays of the lowest-lying radially excited baryons. Assuming a single-quark decay approximation, and negligible configuration mixing, we make model-independent predictions for the partial decay widths to final states with a…

High Energy Physics - Phenomenology · Physics 2007-05-23 Carl E. Carlson

We study nonleptonic decays of the orbitally excited, \su6 \rep{70}-plet baryons in order to test the hypothesis that the successes of the nonrelativistic quark model have a natural explanation in the large-$N_c$ limit of QCD. By working in…

High Energy Physics - Phenomenology · Physics 2009-09-11 Christopher D. Carone , Howard Georgi , Lev Kaplan , David Morin

The decays of non-strange positive parity excited baryons via emission of a pseudo-scalar meson are studied in the framework of the 1/Nc expansion to order 1/Nc. In particular, the pionic decays of the l=0 Roper baryons and of the l=2…

High Energy Physics - Phenomenology · Physics 2014-11-18 J. L. Goity , N. N. Scoccola

Recently LHCb reported the discovery of five extremely narrow excited $\Omega_c$ baryons decaying into $\Xi_c^+ K^-$. We interpret these baryons as bound states of a $c$-quark and a $P$-wave $ss$-diquark. For such a system there are exactly…

High Energy Physics - Phenomenology · Physics 2017-06-21 Marek Karliner , Jonathan L. Rosner

The strong decays of excited nonstrange baryons into the final states Lambda K, Sigma K, and for the first time into Lambda(1405) K, Lambda(1520) K, Sigma(1385) K, Lambda K*, and Sigma K*, are examined in a relativized quark pair creation…

Nuclear Theory · Physics 2014-11-18 Simon Capstick , W. Roberts

The discussion of the 70-plet of negative parity baryons illustrates the large Nc QCD approach to orbitally excited baryons. In the case of the l=1 baryons the existing data allows to make numerous predictions to first order in the SU(3)…

High Energy Physics - Phenomenology · Physics 2017-08-23 Carlos L. Schat

Inspired by the recent observation of the $\Xi_{cc}^{++}$ by LHCb collaboration, we explore the "decay constants" of doubly heavy baryons in the framework of QCD sum rules. With the $\Xi_{cc}, \Xi_{bc}, \Xi_{bb}$, and $\Omega_{cc},…

High Energy Physics - Phenomenology · Physics 2018-11-26 Xiao-Hui Hu , Yue-Long Shen , Wei Wang , Zhen-Xing Zhao

Recently we considered the electromagnetic decays of the orbitally-excited SU(6) 70-plet baryons in large-N_c QCD, fitting to the helicity amplitudes measured in photoproduction experiments. Using the results of this analysis, we predict…

High Energy Physics - Phenomenology · Physics 2009-10-31 Carl E. Carlson , Christopher D. Carone

The masses of the positive parity $[{\bf 70},0^+]$ and $[{\bf 70},2^+]$ non-strange baryons are calculated in large $N_c$ QCD by considering the most dominant operators in an $1/N_c$ expansion. The approach is based on the introduction of…

High Energy Physics - Phenomenology · Physics 2009-11-11 N. Matagne , Fl. Stancu

Using the constrained-fitting method based on Bayesian priors, we extract the masses of the two lowest states of octet and decuplet baryons with both parities. The calculation is done on quenched 16^3x28 lattices of a=0.2 fm using an…

High Energy Physics - Lattice · Physics 2008-11-26 F. X. Lee , S. J. Dong , T. Draper , I. Horvath , K. F. Liu , N. Mathur , J. B. Zhang

We investigate the sextet $b$-baryon decay processes $\Omega_b\to J/\psi\Omega^{(*)}$,where $\Omega^*$ represents the $1P$-, $1D$- and $2S$-wave excited $\Omega$ hyperons in the spectroscopy. Using the constituent quark model, we obtain…

High Energy Physics - Phenomenology · Physics 2025-07-09 Kai-Lei Wang , Juan Wang , Yu-Kuo Hsiao , Xian-Hui Zhong

Phenomenological applications of an effective theory of low-lying excited states of charm and bottom isoscalar baryons are discussed at leading and next-to-leading order in the combined heavy quark and large $N_c$ expansion. The combined…

High Energy Physics - Phenomenology · Physics 2014-11-17 Z. Aziza Baccouche , Chi-Keung Chow , Thomas D. Cohen , Boris A. Gelman

We investigate the decays of the charmed baryons aiming at the systematic understanding of hadron internal structures based on the quark model by paying attention to heavy quark symmetry. We evaluate the decay widths from the one pion…

High Energy Physics - Phenomenology · Physics 2017-02-01 Hideko Nagahiro , Shigehiro Yasui , Atsushi Hosaka , Makoto Oka , Hiroyuki Noumi

Strong decays of charmed baryons are analyzed in the framework of heavy hadron chiral perturbation theory (HHChPT) in which heavy quark symmetry and chiral symmetry are synthesized. HHChPT works excellently for describing the strong decays…

High Energy Physics - Phenomenology · Physics 2008-11-26 Hai-Yang Cheng , Chun-Khiang Chua

The partial decay widths of positive parity baryons belonging to 56-plets of SU(6) are analyzed in the framework of the 1/Nc expansion. The channels considered are those with emission of a single pion, K or K-bar mesons, and the analysis is…

High Energy Physics - Phenomenology · Physics 2009-11-05 J. L. Goity , C. Jayalath , N. N. Scoccola

The progresses in the experimental sector have been the harbinger of the observations of many new hadrons. Very recently, LHCb Collaboration announced the observation of two new $\Sigma_b(6097)^{\pm}$ states in the $\Lambda^0_b\pi^{\pm}$…

High Energy Physics - Phenomenology · Physics 2019-05-15 T. M. Aliev , K. Azizi , Y. Sarac , H. Sundu

Using 980 $fb^-1$ of data collected with the Belle detector operating at the KEKB asymmetric-energy e^+e^- collider, we report a study of the electromagnetic decays of excited {charmed baryons} $\Xi_c(2790)$ and $\Xi_c(2815)$. A clear…

High Energy Physics - Experiment · Physics 2020-11-04 Belle Collaboration , J. Yelton , I. Adachi , J. K. Ahn , H. Aihara , S. AlSaid , D. M. Asner , T. Aushev , R. Ayad , V. Babu , S. Bahini pati , P. Behera , C. Bele , J. Bennett , V. Bhardwaj , B. Bhuyan , T. Bilka , J. Biswal , G. Bonvicini , A. Bozek , M. Bracko , T. E. Browder , M. Campajola , D. Cervenkov , M. -C. Chang , P. Chang , V. Chekelian , A. Chen , B. G. Cheon , K. Chilikin , K. Cho , S. -J. Cho , S. - K. Choi , Y. Choi , S. Choudhury , D. Cinabro , S. Cunliffe , G. DeNardo , F. DiCapua , Z. Dolezal , T. V. Dong , S. Eidelman , D. Epifanov , T. Ferber , B. G. Fulsom , R. Garg , V. Gaur , N. Gabyshev , A. Garmash , A. Giri , P. Goldenzweig , C. Hadjivasiliou , O. Hartbrich , K. Hayasaka , H. Hayashii , M. T. Hedges , M. HernandezVillanueva , W. -S. Hou , C. -L. Hsu , T. Iijima , K. Inami , G. Inguglia , A. Ishikawa , R. Itoh , M. Iwasaki , Y. Iwasaki , W. W. Jacobs , S. Jia , Y. Jin , C. W. Joo , K. K. Joo , A. B. Kaliyar , K. H. Kang , G. Karyan , Y. Kato , T. Kawasaki , H. Kichimi , C. Kiesling , B. H. Kim , D. Y. Kim , S. H. Kim , Y. -K. Kim , K. Kinoshita , P. Kodys , S. Korpar , D. Kotchetkov , P. Krizan , R. Kroeger , P. Krokovny , R. Kulasiri , R. Kumar , K. Kumara , A. Kuzmin , Y. -J. Kwon , K. Lalwani , J. S. Lange , S . C. Lee , P. Lewis , L. K. Li , Y. B. Li , L. LiGioi , J. Libby , K. Lieret , Z. Liptak , D. Liventsev , T. Luo , C. MacQueen , M. Masuda , T. Matsuda , D. Matvienko , J. T. McNeil , M. Merola , H. Miyata , R. Mizuk , G. B. Mohanty , S. Mohanty , T. J. Moon , T. Mori , M. Mrvar , R. Mussa , E. Nakano , M. Nakao , Z. Natkaniec , A. Natochii , M. Nayak , N. K. Nisar , S. Nishida , K. Ogawa , S. Ogawa , H. Ono , Y. Onuki , P. Oskin , 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 , A. Rostomyan , N. Rout , G. Russo , D. Sahoo , Y. Sakai , S. Sandilya , L. Santelj , T. Sanuki , V. Savinov , G. Schnell , J. Schueler , C. Schwanda , Y. Seino , K. Senyo M. E. Sevior , M. Shapkin , V. Shebalin , C. P. Shen , J. -G. Shiu , B. Shwartz , J. B. Singh , A. Sokolov , E. Solovieva , M. Staric , Z. S. Stottler , J. F. Strube , M. Sumihama , K. Sumisawa , T. Sumiyoshi , W. Sutcliffe , M. Takizawa , U. Tamponi , K. Tanida , F. Tenchini , M. Uchida , T. Uglov , Y. Unno , S. Uno , P. Urquijo , Y. Usov , S. E. Vahsen , R. VanTonder , G. Varner , A. Vinokurova , V. Vorobyev , E. Waheed , C. H. Wang , E. Wang , M. -Z. Wang , P. Wang , X. L. Wang , M. Watanabe , E. Won , X. Xu , B. D. Yabsley , W. Yan , S. B. Yang , H. Ye , J. H. Yin , Z. P. Zhang , V. Zhilich , V. Zhukova , V. Zhulanov

We analyze strong one-pion and radiative one-photon decays of heavy flavored baryons within a relativistic three-quark model. Employing the same parameters as were used for the description of the semileptonic decays of heavy baryons, we…

High Energy Physics - Phenomenology · Physics 2009-10-31 M. A. Ivanov , J. G. Korner , V. E. Lyubovitskij , A. G. Rusetsky

There are two apparent puzzles connected with the two-body and three-body doubly charmed baryonic B decays. First, earlier calculations based on QCD sum rules or the diquark model predict $Br(\bar B^0\to\Xi_c^+\bar\Lambda_c^-)\approx…

High Energy Physics - Phenomenology · Physics 2008-11-26 Hai-Yang Cheng , Chun-Khiang Chua , Shang-Yuu Tsai
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