dorsal/arxiv
View SchemaVector Meson Dominance and Rho-Omega Mixing
| Authors | S. A. Coon, M. D. Scadron |
|---|---|
| Categories | |
| ArXiv ID | nucl-th/9808014 |
| URL | https://arxiv.org/abs/nucl-th/9808014 |
| DOI | 10.1103/PhysRevC.58.2958 |
| Journal | Phys.Rev.C58:2958-2962,1998 |
Abstract
The scale of a phenomenologically successful charge-symmetry-violating nucleon-nucleon interaction, that attributed to meson exchange with a $\Delta I =1$ rho-omega transition, is set by the Coleman-Glashow SU(2) breaking tadpole mechanism. A single tadpole scale has been obtained from symmetry arguments, electromagnetic meson and baryon measured mass splittings, and the observed isospin violating ($\Delta I=1$) decay $\omega \to \pi^+\pi^-$. The hadronic realization of this tadpole mechanism lies in the $I = 1$ $a_0$ scalar meson. We show that measured hadronic and two-photon widths of the $a_0$ meson, with the aid of the Vector Meson Dominance model, recover the universal Coleman-Glashow tadpole scale.
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"abstract": "The scale of a phenomenologically successful charge-symmetry-violating\nnucleon-nucleon interaction, that attributed to meson exchange with a $\\Delta I\n=1$ rho-omega transition, is set by the Coleman-Glashow SU(2) breaking tadpole\nmechanism. A single tadpole scale has been obtained from symmetry arguments,\nelectromagnetic meson and baryon measured mass splittings, and the observed\nisospin violating ($\\Delta I=1$) decay $\\omega \\to \\pi^+\\pi^-$. The hadronic\nrealization of this tadpole mechanism lies in the $I = 1$ $a_0$ scalar meson.\nWe show that measured hadronic and two-photon widths of the $a_0$ meson, with\nthe aid of the Vector Meson Dominance model, recover the universal\nColeman-Glashow tadpole scale.",
"arxiv_id": "nucl-th/9808014",
"authors": [
"S. A. Coon",
"M. D. Scadron"
],
"categories": [
"nucl-th"
],
"doi": "10.1103/PhysRevC.58.2958",
"journal_ref": "Phys.Rev.C58:2958-2962,1998",
"title": "Vector Meson Dominance and Rho-Omega Mixing",
"url": "https://arxiv.org/abs/nucl-th/9808014"
},
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