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Related papers: Charmed ${\bf (70,1^-)}$ baryon multiplet

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The finite size of doubly heavy diquark gives a positive correction to the masses of baryons calculated in the local diquark approximation. We evaluate this correction for the basic states of doubly charmed baryons to give quite accurate…

High Energy Physics - Phenomenology · Physics 2019-11-28 V. V. Kiselev , A. V. Berezhnoy , A. K. Likhoded

In this two part series a chiral confining model of baryons is used to describe low--lying negative parity resonances $N^*$, $\Delta^*$, $\Lambda^*$ and $\Sigma^*$ in the mean field approximation. A physical baryon in this model consists of…

Nuclear Theory · Physics 2007-05-23 Y. Umino , M. K. Banerjee

Extending the SU(3) flavour symmetry breaking expansion from up, down and strange sea quark masses to partially quenched valence quark masses allows an extrapolation to the charm quark mass. This approach leads to a determination of charmed…

High Energy Physics - Lattice · Physics 2018-04-18 R. Horsley , Z. Koumi , Y. Nakamura , H. Perlt , P. E. L. Rakow , G. Schierholz , A. Schiller , H. Stuben , R. D. Young , J. M. Zanotti

The spectrum of the $c qq$ baryons contains a few states whose nature is not clearly a three-quark composite and which might have a sizable baryon-meson component. Examples include the $\Sigma_c(2800)$ or the $\Lambda_c(2940)$. Here we…

High Energy Physics - Phenomenology · Physics 2024-10-22 Mao-Jun Yan , Fang-Zheng Peng , Manuel Pavon Valderrama

The masses of heavy quark baryons are studied in an expansion in 1/N_c, SU(3) flavor symmetry breaking, and heavy-quark symmetry breaking. Very accurate model-independent mass relations are obtained for charm and bottom baryons.

High Energy Physics - Phenomenology · Physics 2009-11-07 E. Jenkins

In this proceedings report, we discuss unique features of charmed, or in general heavy, baryons with one heavy quark. A well and long-term known phenomena, the distinction of the two modes of the rho and lambda type of a three-quark system…

We study two- and three-baryon systems with two units of charm looking for possible bound states or resonances. All two-baryon interactions are consistently derived from a constituent quark model tuned in the light-flavor hadron…

High Energy Physics - Phenomenology · Physics 2020-08-12 H. Garcilazo , A. Valcarce

We calculate masses of light and heavy mesons as well as baryons of negative parity containing $u,d,s,c$ and $b$ quarks. It is an extension of our previous work where we had studied the positive parity baryons. We adopt a quark-diquark…

High Energy Physics - Phenomenology · Physics 2021-11-24 L. X. Gutiérrez-Guerrero , G. Paredes-Torres , A. Bashir

Mass spectra of strange baryons are calculated in the framework of the relativistic quark model based on the quasipotential approach. Baryons are treated as the relativistic quark-diquark bound systems. It is assumed that two quarks with…

High Energy Physics - Phenomenology · Physics 2016-10-28 R. N. Faustov , V. O. Galkin

The results of a recent quenched lattice QCD simulation for charmed baryons are presented. In contrast to a previous calculation, it is found that hyperfine splittings are in agreement with quark model expectations and comparable to…

High Energy Physics - Phenomenology · Physics 2009-10-31 R. M. Woloshyn

We review the weak-decay and spectroscopy properties of baryons with two charmed quarks. We also present the convergent speculations on exotic mesons $(QQ\bar{q}\bar{q})$ with two heavy quarks and two light antiquarks.

High Energy Physics - Phenomenology · Physics 2007-05-23 Jean-Marc Richard

The masses of the low-lying strange and charm baryons are evaluated using two degenerate flavors of twisted mass sea quarks for pion masses in the range of about 260 MeV to 450 MeV. The strange and charm valence quark masses are tuned to…

High Energy Physics - Lattice · Physics 2013-05-30 C. Alexandrou , J. Carbonell , D. Christaras , V. Drach , M. Gravina , M. Papinutto

In this article, we study the mass spectrum of the low-lying triply heavy hybrid baryon, which consists of three valence heavy quarks in a color octet and one valence gluon, with spin-parity $J^P=(\frac{1}{2})^+$ via QCD sum rules. This is…

High Energy Physics - Phenomenology · Physics 2023-08-22 Yi-Cheng Zhao , Chun-Meng Tang , Liang Tang

In this work, we systematically investigate the dibaryons with charm number $C$=1 and strangeness number $S$=$\pm$ 1 from the interactions of a charmed baryon and a strange baryon $\Lambda_c\Lambda$, $\Lambda_c\Sigma^{(*)}$,…

High Energy Physics - Phenomenology · Physics 2023-01-04 Shu-Yi Kong , Jun-Tao Zhu , Jun He

Quantitative corrections are estimated to three of Franklin's sum rules involving the masses of baryons containing at least one charmed quark and to three analogous sum rules for baryons containing at least one bottom quark. The corrections…

High Energy Physics - Phenomenology · Physics 2007-05-23 D. B. Lichtenberg

The mass spectrum of charmed and bottom baryons has been computed on anisotropic lattices using quenched lattice nonrelativistic QCD. Masses are extracted by using mass splittings which are more accurate than masses obtained directly by…

High Energy Physics - Phenomenology · Physics 2010-04-06 Nilmani Mathur , Randy Lewis , R. M. Woloshyn

We use the method of QCD Sum Rules to estimate the masses of the charm baryon, $\Lambda^+_c$, bottom baryon $\Lambda^0_b$, strange baryon $\Lambda^0_s$ and compare them to their experimental values.

High Energy Physics - Phenomenology · Physics 2018-08-17 Leonard S. Kisslinger , Bijit Singha

Quark and pole models of nonleptonic decays of charmed baryons are analysed from the point of view of their symmetry properties. The symmetry structure of the parity conserving amplitudes that corresponds to the contribution of the…

High Energy Physics - Phenomenology · Physics 2009-10-22 P. Zenczykowski

A good agreement between a flux tube-based quark model of light baryons (strange and nonstrange) and the $1/N_c$ expansion mass formula has been found in previous studies. In the present work a larger connection is established between the…

High Energy Physics - Phenomenology · Physics 2008-11-26 C. Semay , F. Buisseret , F. Stancu

A diquark model is used to investigate single charmed baryons. In this model, baryon is composed of two diquarks and an antiquark. Masses of lowest lying states with $J^P= 1/2 ^ \pm$ are obtained. Some masses are smaller than other…

High Energy Physics - Phenomenology · Physics 2008-08-13 Q. W. Wang