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2009

Axigluon Couplings in the Presence of Extra Color-Octet Spin-One Fields

Zerwekh, Alfonso R.

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In this paper, we study how the interaction of the axigluon with quarks is modified when we introduce new color-octet spin-one fields in a chiral color model.

We show that in this case the strength of this interaction is not completely determined by the gauge symmetry any more and can be significantly weaker than the one predicted in the original chiral color model.
In this way, we reinterpret the non-observability of the axigluon at the Tevatron, not as a limit on the axigluon mass, but as a limit on the strength of the axigluon coupling to quarks.

Axigluon Couplings in the Presence of Extra Color-Octet Spin-One Fields · Around

Built on

P. H. Frampton and S. L. Glashow, “Unifiable Chiral Color With Natural Gim Mechanism,” Phys. Rev. Lett. 58
1987
Earlier work this paper cites.
P. H. Frampton and S. L. Glashow, “Chiral Color: An Alternative to the Standard Model,” Phys. Lett. B 190
1987
Earlier work this paper cites.

Similar

P. H. Frampton, “Gauge Field Theory”, John Wiley & Sons, INC, 2000, second edition
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A. R. Zerwekh, “Consequences of partial vector meson dominance for the phenomenology of colored technihadrons,” Eur. Phys. J. C 49
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P. Ferrario and G. Rodrigo, “Constraining heavy colored resonances from top-antitop quark events,” arXiv:0906.5541 [hep-ph]
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M. V. Martynov and A. D. Smirnov, “Chiral color symmetry and possible G ′ G^{\prime} -boson effects at the Tevatron and LHC,” arXiv:0906.4525 [hep-ph]
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A. R. Zerwekh, “Effective description of a gauge field and a tower of massive vector resonances,” arXiv:hep-ph/0307130
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A. Pukhov, arXiv:hep-ph/0412191
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T. Aaltonen et al
Original
2009
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