Abstract:These lectures give a brief description of CP violation in B and K meson decays with particular emphasize put on the determination of the CKM matrix. The following topics will be discussed: i) The CKM matrix, the unitarity triangle and general aspects of the theoretical framework, ii) Particle-antiparticle mixing and various types of CP violation, iii) Standard analysis of the unitarity triangle, iv) The ratio ε ′ /ε, v) The most important strategies for the determination of the angles α, β and γ from B decays… Show more
“…This allowed to perform a new check of the Standard Model based on the test of the unitarity of the CKM mixing matrix, the so-called unitarity triangle test of the SM. It was shown [39][40][41][42][43] that the SM with three families of quarks is in an good agreement with existing data, which include the data on the measurements of the effects of CP violation. In the unitarity triangle (UT) test the experimental values of the K L − K S mass difference ∆m K and the B dH − B dL mass difference ∆m B d are used.…”
There are claims in the literature that in neutrino oscillations and oscillations of neutral kaons and B-mesons the oscillation phase differs from the standard one by a factor of two. We reconsider the arguments leading to this extra factor and investigate, in particular, the non-relativistic regime. We actually find that the very same arguments lead to an ambiguous phase and that the extra factor of two is a special case. We demonstrate that the unitarity triangle (UT) fit in the Standard Model with three families is a suitable means to discriminate between the standard oscillation phase and the phase with an extra factor of two. If K L − K S and B dH − B dL mass differences are extracted from the K 0 −K 0 and B 0 d −B 0 d data, respectively, with the extra factor of two in the oscillation phases, then the UT fit becomes significantly worse in comparison with the standard fit and the extra factor of two is disfavoured by the existing data at the level of more than 3 σ. *
“…This allowed to perform a new check of the Standard Model based on the test of the unitarity of the CKM mixing matrix, the so-called unitarity triangle test of the SM. It was shown [39][40][41][42][43] that the SM with three families of quarks is in an good agreement with existing data, which include the data on the measurements of the effects of CP violation. In the unitarity triangle (UT) test the experimental values of the K L − K S mass difference ∆m K and the B dH − B dL mass difference ∆m B d are used.…”
There are claims in the literature that in neutrino oscillations and oscillations of neutral kaons and B-mesons the oscillation phase differs from the standard one by a factor of two. We reconsider the arguments leading to this extra factor and investigate, in particular, the non-relativistic regime. We actually find that the very same arguments lead to an ambiguous phase and that the extra factor of two is a special case. We demonstrate that the unitarity triangle (UT) fit in the Standard Model with three families is a suitable means to discriminate between the standard oscillation phase and the phase with an extra factor of two. If K L − K S and B dH − B dL mass differences are extracted from the K 0 −K 0 and B 0 d −B 0 d data, respectively, with the extra factor of two in the oscillation phases, then the UT fit becomes significantly worse in comparison with the standard fit and the extra factor of two is disfavoured by the existing data at the level of more than 3 σ. *
“…This framework is known as the operator product expansion, and is described in more detail in, e.g., Refs. [33,34]. In many concrete models, the operators that are most sensitive to NP are a subset of …”
Section: Model-independent Analysis Of New Physics Contributions To Lmentioning
confidence: 99%
“…This scenario has been studied in extensions of the CKM fit of the SM which includes B = 2 measurements to constrain the CKM elements V tq [256,259], in combination with many other flavour-changing processes. Including LHCb measurements [139,229] 34 the SM point [256] (prior to the LHCb results being available, a similar analysis gave a discrepancy of 3.6σ driven mainly by the anomalous dimuon asymmetry [259]). The analysis gives s consistent with the SM, within large uncertainties, whereas the more precise data in the B 0 system hint at a deviation in d (see Fig.…”
Section: Model Independent Constraints On New Physics In B Mixingmentioning
confidence: 99%
“…(34) are restricted to a particular set of observables, mainly those with B = 2, since correlations with B = 1 measurements are 34 But …”
Section: Model Independent Constraints On New Physics In B Mixingmentioning
region at a hadron collider. This document discusses the implications of these first measurements on classes of extensions to the Standard Model, bearing in mind the interplay with the results of searches for on-shell production of new particles at ATLAS and CMS. The physics potential of an upgrade to the LHCb detector, which would allow an order of magnitude more data to be collected, is emphasised.
“…7,8 An up-to-date review of experimental constraints on B meson mixing can also be found in the PDG. 9 The following discussion applies to neutral mesons of any kind.…”
Section: Beauty Mixing Phenomenology In a Nutshellmentioning
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