2001
DOI: 10.1016/s0370-2693(01)00162-9
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Top flavour-changing neutral coupling signals at a linear collider

Abstract: We present an analysis of the sensitivity of the TESLA e + e − collider to top flavourchanging neutral couplings to the Z boson and photon. We consider the cases without beam polarization, with only e − polarization and with e − and e + polarization, showing that the use of the latter substantially enhances the sensitivity to discover or bound these vertices. For some of the couplings the expected LHC limits could be improved up to an order of magnitude for equal running times.

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Cited by 45 publications
(32 citation statements)
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“…At the LHC the production proceeds through the six parton-level processes shown in Eqs. (1)(2)(3)(4)(5)(6), among which only gg → tc has been extensively studied in the MSSM [11,12]. In calculating the cross section for each channel, we also include the rate for its charge conjugate channel.…”
Section: The Decaymentioning
confidence: 99%
“…At the LHC the production proceeds through the six parton-level processes shown in Eqs. (1)(2)(3)(4)(5)(6), among which only gg → tc has been extensively studied in the MSSM [11,12]. In calculating the cross section for each channel, we also include the rate for its charge conjugate channel.…”
Section: The Decaymentioning
confidence: 99%
“…This results in a negligible branching ratio Br(t → Zc) ∼ 10 −14 within the SM. In Model I the FCN coupling X ct can be sizeable [39], leading to top decays t → Zc [104], Zt production at LHC [105,106] and single top production at linear colliders [107,108,109,110]. For m T ∼ m t the new contributions to meson observables involving T diagrams are small, and this FCN coupling can be relatively large, |X ct | = 0.036 (see Fig.…”
Section: Mixing With An Up Singletmentioning
confidence: 99%
“…The CDF and DØ collaborations have reported interesting bounds on the FCNC top quark decays [334][335][336]. The SM expectations for such top quark FCNC processes are far below the detectable level but the MSSM can enhance them by several orders of magnitude to make them potentially accessible at future collider experiments [337][338][339]. The theoretical branching ratios and the experimental limits are summarised in Table 8.…”
Section: Introductionmentioning
confidence: 99%