dorsal/arxiv
View SchemaIs the eta Meson a Goldstone Boson?
| Authors | M. Kirchbach, H. -J. Weber |
|---|---|
| Categories | |
| ArXiv ID | nucl-th/9612010 |
| URL | https://arxiv.org/abs/nucl-th/9612010 |
| Journal | Comments Nucl.Part.Phys. 22 (1998) 171-183 |
Abstract
The decoupling of the eta meson from the nucleon, as recently deduced from analyzing \bar p p collisions and eta photoproduction off the proton at threshold, is shown to provide an argument against the octet Goldstone boson nature of the eta meson. This argument concerns the structure of the strong isoscalar axial vector current. A vanishing eta-N coupling means a vanishing contribution of the eta-pole term to the hypercharge nucleon axial vector current. Therefore, no partial conservation of the latter can be achieved. This new situation invalidates the octet Goldberger--Treiman relation for the eta-N coupling constant that is indicative of the octet Goldstone boson nature of the eta meson. In such a case there is no longer a compelling reason for the standard belief that the eta meson should be coupled to the hadronic vacuum through the hypercharge axial vector current. Rather, it will be coupled to it as any ordinary neutral pseudoscalar meson via the neutral axial vector current of the electroweak theory. As a result of the suggested universal structure of the weak and strong neutral axial vector currents the eta meson satisfies the strange analog of the Goldberger-Treiman relation so that it acquires features of a strange Goldstone boson. Hence the eta-NN vertex constant appears proportional to $\Delta s$, the fraction of nucleon spin carried by the strange quark sea, thus explaining its suppression naturally.
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"abstract": "The decoupling of the eta meson from the nucleon, as recently deduced from\nanalyzing \\bar p p collisions and eta photoproduction off the proton at\nthreshold, is shown to provide an argument against the octet Goldstone boson\nnature of the eta meson. This argument concerns the structure of the strong\nisoscalar axial vector current. A vanishing eta-N coupling means a vanishing\ncontribution of the eta-pole term to the hypercharge nucleon axial vector\ncurrent. Therefore, no partial conservation of the latter can be achieved. This\nnew situation invalidates the octet Goldberger--Treiman relation for the eta-N\ncoupling constant that is indicative of the octet Goldstone boson nature of the\neta meson. In such a case there is no longer a compelling reason for the\nstandard belief that the eta meson should be coupled to the hadronic vacuum\nthrough the hypercharge axial vector current. Rather, it will be coupled to it\nas any ordinary neutral pseudoscalar meson via the neutral axial vector current\nof the electroweak theory. As a result of the suggested universal structure of\nthe weak and strong neutral axial vector currents the eta meson satisfies the\nstrange analog of the Goldberger-Treiman relation so that it acquires features\nof a strange Goldstone boson. Hence the eta-NN vertex constant appears\nproportional to $\\Delta s$, the fraction of nucleon spin carried by the strange\nquark sea, thus explaining its suppression naturally.",
"arxiv_id": "nucl-th/9612010",
"authors": [
"M. Kirchbach",
"H. -J. Weber"
],
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],
"journal_ref": "Comments Nucl.Part.Phys. 22 (1998) 171-183",
"title": "Is the eta Meson a Goldstone Boson?",
"url": "https://arxiv.org/abs/nucl-th/9612010"
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