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Direct top quark production at hadron colliders as a probe of new physics
Phys. Rev. D 56, 5725 – Published 1 November, 1997
DOI: https://doi.org/10.1103/PhysRevD.56.5725
Abstract
We examine the effect of an anomalous flavor-changing chromomagnetic moment which allows direct top quark production (two partons combining into an unaccompanied single top quark in the channel) at hadron colliders. We consider both and couplings. We find that the anomalous charm quark coupling parameter can be measured down to at the Fermilab Tevatron with the Main Injector upgrade (CERN LHC). The anomalous up quark coupling parameter can be measured to at the Tevatron (LHC).
References (21)
- F. Abe et al., Phys. Rev. Lett. 74, 2626 (1995).
- S. Abachi et al., Phys. Rev. Lett. 74, 2632 (1995).
- J. Incandela, Nuovo Cimento A 109, 741 (1996).
- Thomas J. LeCompte, FERMILAB-CONF-96-021-E, 1996.
- A.P. Heinson, Future Top Physics at the Tevatron and LHC, Proceedings of the QCD and high energy hadronic interactions, Les Arcs, 1996 (Editions Frontières, Gif-sur-Yvette, France, 1996), pp. 43–52.
- T. Han, K. Whisnant, B. L. Young, and X. Zhang, Phys. Rev. D 55, 7241 (1997); K. Whisnant, Jin-Min Yang, Bing-Lin Young, and X. Zhang, 56, 467 (1997); R. Martinez and J-Alexis Rodriguez, 55, 3212 (1997).
- D. Atwood, A. Kagan, and T.G. Rizzo, Phys. Rev. D 52, 6264 (1995); Douglas O. Carlson, Ehab Malkawi, and C.P. Yuan, Phys. Lett. B 337, 145 (1994); G.J. Gounaris, M. Kuroda, and F.M. Renard, Phys. Rev. D 54, 6861 (1996); G.J. Gounaris, J. Layssac, and F.M. Renard, 55, 5786 (1997).
- B. Grzadkowski, J.F. Gunion, and P. Krawczyk, Phys. Lett. B 268, 106 (1991); G. Eliam, J.L. Hewett, and A. Soni, Phys. Rev. D 44, 1473 (1991); M. Luke and M.J. Savage, Phys. Lett. B 307, 387 (1993).
- G. Couture, C. Hamzaoui, and H. König, Phys. Rev. D 52, 1713 (1995).
- Jorge L. Lopez, D.V. Nanopoulos, and Raghavan Rangarajan, Phys. Rev. D 56, 3100 (1997).
- T.P. Cheng and M. Sher, Phys. Rev. D 48, 3484 (1987); W.S. Hou, Phys. Lett. B 296, 179 (1992); L.J. Hall and S. Weinberg, Phys. Rev. D 48, 979 (1993); D. Atwood, L. Reina, and A. Soni, 53, 1199 (1996).
- C.T. Hill, Phys. Lett. B 266, 419 (1991); 345, 483 (1995); B. Holdom, 339, 114 (1994); 351, 279 (1995).
- H. Georgi, L. Kaplan, D. Morin, and A. Schenk, Phys. Rev. D 51, 3888 (1995); for a review of composite models, see, e.g., R.D. Peccei, in Proceedings of the 1987 Lake Louise Winter Institute: Selected Topics in the Electroweak Interactions, edited by J.M. Cameron et al. (World Scientific, Singapore, 1987).
- X. Zhang, Phys. Rev. D 51, 5309 (1995); J. Berger, A. Blotz, H.-C. Kim, and K. Goeke, 54, 3598 (1996).
- T. Han, K. Whisnant, B.-L. Young, and X. Zhang, Phys. Lett. B 385, 311 (1996).
- A.D. Martin, R.G. Roberts, and W.J. Stirling, Phys. Rev. D 50, 6734 (1994).
- H.L. Lai, J. Botts, J. Huston, J.G. Morfin, J.F. Owens, J. Qiu, W.K. Tung, and H. Weerts, Phys. Rev. D 51, 4763 (1995).
- A.P. Heinson, A.S. Belyaev, and E.E. Boos, Phys. Rev. D 56, 3114 (1997).
- F.A. Berends, H. Kuijf, B. Tausk, and W.T. Giele, Nucl. Phys. B357, 32 (1991).
- R.M. Barnett, H.E. Haber, and D.E. Soper, Nucl. Phys. B306, 697 (1988); F.W. Olness and W.-K. Tung, B308, 813 (1988).
- E. Malkawi and T. Tait, Phys. Rev. D 54, 5758 (1996).