ﻻ يوجد ملخص باللغة العربية
The structure of Omega-pi state with isospin I=1 and spin-parity J^p=3/2^- are dynamically studied in both the chiral SU(3) quark model and the extended chiral SU(3) quark model by solving a resonating group method (RGM) equation. The model parameters are taken from our previous work, which gave a satisfactory description of the energies of the baryon ground states, the binding energy of the deuteron, the nucleon-nucleon (NN) scattering phase shifts, and the hyperon-nucleon (YN) cross sections. The calculated results show that the Omega-pi state has an attractive interaction, and in the extended chiral SU(3) quark model such an attraction can make for an Omega-pi quasi-bound state with the binding energy of about several MeV.
Inspired by the recent observation of a narrow resonance-like structure around 2360 MeV in the p+n to d + pi 0 + pi 0 cross section, the possibility of forming a NN*(1440) quasi-molecular state is investigated by using a meson exchange model in which
Recently, a hint for dibaryon $NDelta(D_{21})$ was observed at WASA-AT-COSY with a mass about $30pm10$ MeV below the $NDelta$ threshold. It has a relatively small binding energy compared with the $d^*(2380)$ and a width close to the width of the $Del
Using the production reactions $pdto {}^3mbox{He},omega$ and $ppto ppomega$, the Dalitz plot distribution for the $omega to pi^+ pi^- pi^0$ decay is studied with the WASA detector at COSY, based on a combined data sample of $ (4.408pm 0.042) times 10
In this note we review the role of homotopy groups in determining non-perturbative (henceforth `global) gauge anomalies, in light of recent progress understanding global anomalies using bordism. We explain why non-vanishing of $pi_d(G)$ is neither a
Very recently, a new $Omega^{*}$ state was reported by the Belle Collaboration, with its mass of $2012.4 pm 0.7 text{(stat)}pm 0.6 text{(syst)} mathrm{MeV}$, which locates just below the $KXi^*$ threshold and hence hints to be a possible $KXi^*$ hadr