Analysis of
Ω ( 2012 )
as a molecule in the chiral quark model
暂无分享,去创建一个
[1] J. Ping,et al. Investigation of hidden-charm pentaquarks with strangeness S=-1\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$S=-1$$\ , 2021, The European Physical Journal C.
[2] J. Ping,et al. Investigation of $$\varXi _c^0$$ Ξ c 0 in a chiral quark model , 2020, The European Physical Journal C.
[3] J. Ping,et al. X(2900) in a chiral quark model , 2020, 2010.04045.
[4] L. Geng,et al. Revisiting the $$\Omega (2012)$$ as a hadronic molecule and its strong decays , 2020, 2003.07588.
[5] T. Gutsche,et al. Strong decays of the hadronic molecule ${\mathbf{\Omega }}^{\mathbf{{\ast}}}$(2012) , 2019, Journal of Physics G: Nuclear and Particle Physics.
[6] E. Hiyama,et al. Compact ssscc¯ pentaquark states predicted by a quark model , 2019, Physics Letters B.
[7] M. Polyakov,et al. Ω(2012) through the looking glass of flavour SU(3) , 2018, Physics Letters B.
[8] E. Oset,et al. Coupled channels dynamics in the generation of the $$\Omega (2012)$$Ω(2012) resonance , 2018, The European Physical Journal C.
[9] Xurong Chen,et al. The Ξ* and Ωη Interaction Within a Chiral Unitary Approach* , 2015, 1510.07419.
[10] S. Sarkar,et al. Erratum to: “Baryonic resonances from baryon decuplet-meson octet interaction” [Nucl. Phys. A 750 (2005) 294] , 2006 .
[11] E. Oset,et al. Baryonic resonances from Baryon decuplet-meson octet interactions and the exotic resonance S=1, I=1, J(P)=3/2(-) , 2004, nucl-th/0501027.
[12] M. Lutz,et al. On baryon resonances and chiral symmetry , 2003, nucl-th/0305101.
[13] Isgur,et al. Baryons in a relativized quark model with chromodynamics. , 1985, Physical review. D, Particles and fields.
[14] J. Simons. Resonance state lifetimes from stabilization graphs , 1981 .
[15] Yuval Ne'eman,et al. DERIVATION OF STRONG INTERACTIONS FROM A GAUGE INVARIANCE , 1961 .