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Hyperon
Observation of Global Hyperon Polarization in Ultrarelativistic Heavy-Ion Collisions
Light Higgs Production in Hyperon Decay
Mass Generation Via the Higgs Boson and the Quark Condensate of the QCD Vacuum
Pentaquark and Tetraquark States Arxiv:1903.11976V2 [Hep-Ph]
The Quark Model and Deep Inelastic Scattering
RIKEN BNL Research Center Workshop Volume 108
Hyperon-Nucleon Interaction, Hypernuclei & Hyperonic Matter
Unveiling the Strong Interaction Among Hadrons at the LHC
Quarks, Pion, Kaons, and Hyperons Garrett Yar N Claremont Mckenna College
Exploring the Nature of the Universe
1. Introduction
Hyperon Spectra [Iizuka,Ishii,Kadoh,KH, 0910.1179] Mass Splitting of Baryons With
Hyperon Spectroscopy
Strangeness in Nuclei and Neutron Stars Arxiv:2002.09223V1 [Nucl-Ex]
All-Heavy Tetraquarks
Chiral Quark Model Study of Ud¯S¯S Tetraquark States*
Radiative Hyperon Decays 1 Radiative Hyperon Decays
CP Violation and Rare Decays in Hyperon and Charm Systems
Top View
Detailed Balance and Spin Content of Λ Using Statistical Model M
Quark Modelmodel
Huey-Wen Lin* and Kostas Orginos Lattice QCD Numerical Parameters
Spin-Spin Correlations of a Hyperon Pairs Produced in Hadronic Z° Decays T
GLUON CONTENT of the PROTON and HYPERON MAGNETIC MOMENTS Friedrich Wagner Max-Planck-Institut Ftir Physik Und Astrophysik, Munich, Fed.Rep.Germany
Dilatons in the Topological Soliton Model for the Hyperons
Hyperon-Nucleon Interaction from Chiral EFT
Multi-Strange and Charmed Antihyperon-Hyperon Physics for PANDA
Hyperon Polarization and Magnetic Moments
Hyperon-Photon Physics
Hyperon Physics – Past, Present and Future
Hyperon Production from Neutrino–Nucleon Reaction
On Antihyperon-Hyperon Production in Antiproton-Proton Collisions with the PANDA Experiment
Hyperon-Nuclear Interactions from SU(3) Chiral Effective Field Theory
Various Decays of Particles, Universal Decay Formulas and Their
Theoretical Studies of Hadrons and Nuclei
Solution to the Hyperon Puzzle Using Dark Matter
Nonleptonic Two-Body Decays of Single Heavy Baryons ΛQ, ΞQ, and ΩQ (Q = B, C) Induced by W Emission in the Covariant Confined Quark Model