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Related papers: Baryon Antibaryon Nonets

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We study $S$-wave interactions of the baryon decuplet with the octet of pseudoscalar mesons using the lowest order chiral Lagrangian. We find two bound states in the SU(3) limit corresponding to the octet and decuplet representations. These…

Nuclear Theory · Physics 2011-02-09 E. Oset , S. Sarkar , M. J. Vicente Vacas

We study the branching ratios and up-down asymmetries in the charmed baryon weak decays of ${\bf B}_c\to {\bf B}_DM$ with ${\bf B}_{c(D)}$ anti-triplet charmed (decuplet) baryon and $M$ pseudo-scalar meson states based on the flavor…

High Energy Physics - Phenomenology · Physics 2019-07-03 Chao-Qiang Geng , Chia-Wei Liu , Tien-Hsueh Tsai , Yao Yu

In the theory with a Majorana fermion ($X$) coupled to quark-like fermions ($Q$) via a dimension-six four-fermion vector-vector interaction, we have computed in an earlier work the baryon asymmetry generated in the decay and scattering…

High Energy Physics - Phenomenology · Physics 2025-04-15 Shrihari Gopalakrishna , Rakesh Tibrewala

We consider a model in which dark matter is a composite baryon of a dark sector governed by $SU(3)$ gauge theory, with vector-like quarks also charged under $U(1)_Y$. The model provides simple answer to the dark matter stability problem: it…

High Energy Physics - Phenomenology · Physics 2016-10-21 Ran Huo , Shigeki Matsumoto , Yue-Lin Sming Tsai , Tsutomu T. Yanagida

Motivated by the recent LHCb observation of doubly-charmed baryon $\Xi_{cc}^{++}$ in the $\Lambda_c^+ K^-\pi^+\pi^+$ final state, we analyze the weak decays of doubly heavy baryons $\Xi_{cc}$, $\Omega_{cc}$, $\Xi_{bc}$, $\Omega_{bc}$,…

High Energy Physics - Phenomenology · Physics 2017-11-28 Wei Wang , Zhi-Peng Xing , Ji Xu

We propose a non-supersymmetric SU(5) model in which only the third family of fermions are unified. The model remedies the non-unification of the three Standard Model couplings in non-supersymmetric SU(5). It also provides a mechanism for…

High Energy Physics - Phenomenology · Physics 2012-11-26 Shreyashi Chakdar , Tianjun Li , S. Nandi , Santosh Kumar Rai

Some flavor SU(3) results are presented for decays of the $\Lambda_b$ baryon into non-charmed final states $PB$, where $P$ is a pseudoscalar mesons and $B$ is a spin-1/2 baryon. Although these relations are among amplitudes and hence not…

High Energy Physics - Phenomenology · Physics 2014-02-12 Michael Gronau , Jonathan L. Rosner

We revisit the mass splittings of SU(3) baryons, taking into account the second-order effects of isospin and SU(3) flavor symmetry breakings within the framework of a chiral soliton model. The masses of the baryon decuplet turn out to be…

High Energy Physics - Phenomenology · Physics 2015-05-27 Ghil-Seok Yang , Hyun-Chul Kim

In a model of supersymmetric SU(5) Grand Unification with a spatial dimension described by the orbifold $S^1/(Z_2 \times Z_2')$, proton decay is naturally suppressed at all orders. This is achieved by a suitable implementation of the…

High Energy Physics - Phenomenology · Physics 2008-11-26 Gautam Bhattacharyya , K. Sridhar

The angular distributions of the baryon-antibaryon low-mass enhancements seen in the charmless three-body baryonic B decays B^+ \to p pbar K^+, B^0 \to p pbar K_S^0, and B^0 \to p Lambdabar pi^- are reported. Searches for the pentaquarks…

High Energy Physics - Experiment · Physics 2019-08-14 K. Abe

Searches for $B$ mesons decaying to final states containing a baryon and a lepton are performed, where the baryon is either $\Lambda_c$ or $\Lambda$ and the lepton is a muon or an electron. These decays violate both baryon and lepton number…

High Energy Physics - Experiment · Physics 2011-06-07 P. del Amo Sanchez et al.

The flavor SU(3) group structure of pentaquark baryons which form $\bm{1}$, $\bm{8}$, $\bm{10}$, $\bar{\bm{10}}$, $\bm{27}$, and $\bm{35}$ multiplets is investigated in quark model. The flavor wave functions of all the pentaquark baryons…

High Energy Physics - Phenomenology · Physics 2017-08-23 Yongseok Oh , Hungchong Kim

We calculate hyperon-nucleon and hyperon-hyperon interactions at next-to-leading order in SU(3) baryon chiral perturbation theory extending earlier work by the Bonn-Juelich group. The constructed potentials in momentum space include all…

Nuclear Theory · Physics 2013-09-25 Stefan Petschauer

We consider charmless weak decays of beauty-baryons into decuplet baryons and pseudoscalar mesons in a general framework based on $SU(3)$-flavor decomposition of the decay amplitudes. The dynamical assumption independent $SU(3)$ analysis…

High Energy Physics - Phenomenology · Physics 2020-09-30 Shibasis Roy , Rahul Sinha , N. G. Deshpande

We search for the flavor-changing neutral-current decays B->K(*)nu nubar, and the invisible decays J/psi->nu nubar and psi(2S)->nu nubar via B->K(*)J/psi and B->K(*)psi(2S) respectively, using a data sample of 471 x10^6 BB pairs collected…

High Energy Physics - Experiment · Physics 2013-06-12 The BABAR Collaboration

Semiclassical quantization of the SU(3)-skyrmions is performed by means of the collective coordinate method. The quantization condition known for the SU(2)-solitons quantized with SU(3) collective coordinates is generalized for the SU(3)…

High Energy Physics - Theory · Physics 2010-11-19 V. B. Kopeliovich

SU(3) symmetry relations on the recently constructed hyperon-nucleon potentials are used to develop potential models for all possible baryon-baryon interaction channels. The main focus is on the interaction channels with total strangeness…

Nuclear Theory · Physics 2009-10-31 V. G. J. Stoks , Th. A. Rijken

In a particle theory model whose most readily discovered new particle is the $\sim 1$TeV bilepton resonance in same-sign leptons, currently being sought at CERN's LHC, there exist three quarks ${\cal D, S, T}$ which will be bound by QCD…

High Energy Physics - Phenomenology · Physics 2021-09-06 Paul H. Frampton

The minimal standard model of quarks and leptons is extended with a set of vectorlike fermions to allow baryon number $B$ to become a gauged $U(1)_B$ symmetry. The $B$ assignments of the new particles are determined by renormalizable…

High Energy Physics - Phenomenology · Physics 2021-01-13 Ernest Ma

We investigate the structure of the SU(3) octet and decuplet baryons employing a constituent quark model designed for the study of the baryon-baryon interaction and successfully applied to the meson spectra. The model considers through the…

High Energy Physics - Phenomenology · Physics 2009-11-11 A. Valcarce , H. Garcilazo , J. Vijande
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