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For many decades after the invention of the quark model in 1964 there was no evidence that hadrons are formed from anything other than the simplest pairings of quarks and antiquarks, mesons being formed of a quark-antiquark pair and baryons…

High Energy Physics - Phenomenology · Physics 2017-10-25 Ahmed Ali , Jens Sören Lange , Sheldon Stone

The use of Heavy Quark Symmetry to study bottom and charmed baryons leads to important simplifications of the non-relativistic three body problem, which turns out to be easily solved by a simple variational ansatz. Our simple scheme…

Nuclear Theory · Physics 2009-09-29 C. Albertus , J. E. Amaro , E. Hernandez , J. Nieves

Spectroscopy and strong decays of the charmed baryons are reviewed. Possible spin-parity quantum numbers of several newly observed charmed baryon resonances are discussed. Strong decays of charmed baryons are analyzed in the framework of…

High Energy Physics - Phenomenology · Physics 2011-06-15 Hai-Yang Cheng

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

The chiral $SU(3)$ Lagrangian with charmed baryons of spin $J^P=1/2^+$ and $J^P=3/2^+$ is analyzed. We consider all counter terms that are relevant at next-to-next-to-next-to-leading order (N$^3$LO) in a chiral extrapolation of the charmed…

High Energy Physics - Phenomenology · Physics 2015-06-18 M. F. M. Lutz , D. Samart , Y. Yan

In the present work we investigate the mass spectrum and semileptonic decays of double charm and bottom baryon states using the hypercentral quark model. We solve the six-dimensional Schr\"odinger equation via deep learning and particle…

High Energy Physics - Phenomenology · Physics 2025-04-08 Zahra Ghalenovi , Masoumeh Moazzen Sorkhi , Amir Hossein Sovizi

We calculate the masses of baryons containing one, two, or three heavy quarks using lattice QCD. We consider all possible combinations of charm and bottom quarks, and compute a total of 36 different states with $J^P = \frac12^+$ and $J^P =…

High Energy Physics - Lattice · Physics 2014-11-26 Zachary S. Brown , William Detmold , Stefan Meinel , Kostas Orginos

We review the experimental and theoretical status of baryons containing one heavy quark. The charm and bottom baryon states are classified and their mass spectra are listed. The appropriate theoretical framework for the description of heavy…

High Energy Physics - Phenomenology · Physics 2011-01-25 J. G. Koerner , D. Pirjol , M. Kraemer

We present some recent results from soliton model calculations for the spectrum of baryons with a single heavy quark.The model comprises chiral symmetry for light flavors and (approximate) heavy spin-flavor symmetry for the heavy quarks. We…

High Energy Physics - Phenomenology · Physics 2015-11-30 H. Weigel , J. P. Blanckenberg

We propose that the recently discovered \Theta baryon is a bound state of four quarks and an antiquark, containing two highly correlated ud-pairs. If so, the \Theta baryon has positive parity, and it lies in an near-ideally mixed SU(3)_{f}…

High Energy Physics - Phenomenology · Physics 2009-11-10 R. L. Jaffe , F. Wilczek

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 the framework of the SU(3) chiral quark model, the $S-$wave baryon-baryon bound states are investigated. It is found that according to the symmetry character of the system and the contributions from chiral fields, there are three types…

Nuclear Theory · Physics 2009-11-06 P. N. Shen , Q. B. Li , Z. Y. Zhang , Y. W. Yu

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…

The magnetic moments, transition magnetic moments and the radiative decay widths of singly charmed baryons are calculated with $ {J^P = \frac{1}{2}}^+$ and $ {J^P = \frac{3}{2}}^+$ in the constitute quark model. Further, the strong decay…

High Energy Physics - Phenomenology · Physics 2019-09-24 Keval Gandhi , Zalak Shah , Ajay Kumar Rai

Based on the color-spin interaction in diquarks, we argue that charmed multiquark hadrons are likely to exist. Because of the appreciable number of charm quarks produced in central nucleus-nucleus collisions at ultrarelativistic energies,…

High Energy Physics - Phenomenology · Physics 2008-11-26 Su Houng Lee , Shigehiro Yasui , Wei Liu , Che Ming Ko

We study the so-called extended linear sigma model for the case of four quark flavors. This model is based on global chiral symmetry and dilatation invariance and includes, besides scalar and pseudoscalar mesons, vector and axial-vector…

High Energy Physics - Phenomenology · Physics 2015-09-23 Walaa I. Eshraim , Francesco Giacosa , Dirk H. Rischke

We give a general formulation of the quark-diagram scheme for the nonleptonic weak decays of baryons. We apply it to all the decays of the antitriplet and sextet charmed baryons and express their decay amplitudes in terms of the…

High Energy Physics - Phenomenology · Physics 2009-10-28 Ling-Lie Chau , Hai-Yang Cheng , B. Tseng

The properties of baryons containing one heavy quark are studied in the Skyrme model, where they are treated as bound states of a heavy meson with an $SU(2)$ chiral soliton. In the large $N_c$ limit, the baryon spectrum is an infinite tower…

High Energy Physics - Phenomenology · Physics 2009-10-22 Zachary Guralnik , Michael Luke , Aneesh V. Manohar

I present results of a heavy hadron chiral perturbation theory analysis of the decays and masses of the recently discovered excited charm mesons. The present data on the electromagnetic branching ratios are consistent with heavy quark…

High Energy Physics - Phenomenology · Physics 2014-11-18 Thomas Mehen

The experimental signature of an S=+1 baryon of mass 1540 MeV and width 10-25 MeV has led to speculation that this is an exotic baryon consisting of 4 quarks and 1 antiquark lying at the top of a $\bar{10}$ SU(3) multiplet. The observed…

High Energy Physics - Phenomenology · Physics 2007-05-23 Steven Golbeck , Mikhail Savrov
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