2001
DOI: 10.1016/s0370-2693(01)00061-2
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Universal unitarity triangle and physics beyond the standard model

Abstract: We make the simple observation that there exists a universal unitarity triangle for all models, like the SM, the Two Higgs Doublet Models I and II and the MSSM with minimal flavour violation, that do not have any new operators beyond those present in the SM and in which all flavour changing transitions are governed by the CKM matrix with no new phases beyond the CKM phase. This universal triangle can be determined in the near future from the ratio (∆M ) d /(∆M ) s and sin 2β measured first through the CP asymm… Show more

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Cited by 522 publications
(771 citation statements)
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“…In practice, the most convenient strategy in this case is to fit the shift in the Inami-Lim topquark function entering B d , B s and K 0 mixing. We fit for this shift using the experimental measurements of ∆m d , ∆m s and ǫ K , after determining the parameters of the CKM matrix with the universal unitarity triangle analysis [17]. 7 We obtain the following lower bounds at 95% probability:…”
Section: Resultsmentioning
confidence: 99%
“…In practice, the most convenient strategy in this case is to fit the shift in the Inami-Lim topquark function entering B d , B s and K 0 mixing. We fit for this shift using the experimental measurements of ∆m d , ∆m s and ǫ K , after determining the parameters of the CKM matrix with the universal unitarity triangle analysis [17]. 7 We obtain the following lower bounds at 95% probability:…”
Section: Resultsmentioning
confidence: 99%
“…A more appealing scenario is to assume that the new flavor-changing couplings appearing in SM extensions are suppressed by some symmetry principle. The most restrictive and predictive symmetry principle of this type is the so-called Minimal Flavor Violation (MFV) hypothesis [1,2,3]: the assumption that the SM Yukawa couplings are the only sources of quark-flavor symmetry breaking. In this case all the cancellations that render FCNC automatically small in the SM apply just as well to the new degrees of freedom, allowing for very reasonable mass scales of the new particles.…”
Section: Introductionmentioning
confidence: 99%
“…In particular, flavor changing neutral current bounds such as those arising from K 0 −K 0 mixing impose strong constraints, M ≥ 10 4 TeV. These bounds can be relaxed by restricting the higher dimensional operator basis through adopting the MFV hypothesis [19,20,21,22,23,24,25,26,27,28]. This allows one to consider M to be a few TeV while naturally suppressing FCNC.…”
Section: Introductionmentioning
confidence: 99%