1,318 research outputs found

    Waiting for Clear Signals of New Physics in B and K Decays

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    We classify the extensions of the Standard Model (SM) according to the structure of local operators in the weak effective Hamiltonian and the presence or absence of new flavour and CP-violating interactions beyond those represented by the CKM matrix. In particular we review characteristic properties of models with minimal flavour violation (MFV), models with significant contributions from Higgs penguins and models with enhanced Z^0 penguins carrying a large new CP-violating phase. Within the latter models, the anomalous behaviour of certain B\to\pi K observables implies large departures from the SM predictions for rare and CP-violating K and B decays. Most spectacular is the enhancement of Br(K_L->pi^0 nu nubar) by one order of magnitude and a strong violation of the MFV relation (\sin2\beta)_{\pi\nu\bar\nu}=(\sin2\beta)_{\psi K_S}. On the other hand our prediction for (\sin2\beta)_{\phi K_S}\approx 0.9 differs from the Belle result by the sign but is consistent with the BaBar value. We give a personal shopping list for the coming years.Comment: Main latex-file, 4 figures, 22 page

    Universal Unitarity Triangle and Physics Beyond the Standard Model

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    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 (Delta M)_d/(Delta M)_s and sin(2 beta) measured first through the CP asymmetry in B_d^0 to psi K_S and later in K to pi nu nubar decays. Also suitable ratios of the branching ratios for B to X_{d,s} nu nubar and B_{d,s} to mu^+ mu^- and the angle gamma measured by means of CP asymmetries in B decays can be used for this determination. Comparison of this universal triangle with the non-universal triangles extracted in each model using epsilon, (Delta M)_d and various branching ratios for rare decays will allow to find out in a transparent manner which of these models, if any, is singled out by experiment. A virtue of the universal triangle is that it allows to separate the determination of the CKM parameters from the determination of new parameters present in the extensions of the SM considered here.Comment: 12 pages, 1 figur

    On the Correlations between Flavour Observables in Minimal U(2)^3 Models

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    The stringent correlations between flavour observables in models with CMFV are consistent with the present data except for the correlation Delta M_{s,d}-epsilon_K. Motivated by the recent work of Barbieri et al, we compare the CMFV correlations with the ones present in a special class of models with an approximate global U(2)^3 flavour symmetry, constrained by a minimal set of spurions governing the breakdown of this symmetry and the assumption that only SM operators are relevant in flavour physics. This analog of CMFV to be called MU(2)^3 allows to avoid the Delta M_{s,d}-epsilon_K tension in question because of reduced flavour symmetry and implied non-MFV contributions to Delta M_{s,d}. While the patterns of flavour violation in K meson system is the same as in CMFV models, the CP-violation in B_{s,d} meson systems can deviate from the one in the SM and CMFV models. We point out a stringent triple S_{psi K_S}-S_{psi phi}-|V_ub| correlation in this class of models that could in the future provide a transparent distinction between different MU(2)^3 models and in the context of these models determine |V_ub| by means of precise measurements of S_{psi K_S} and S_{psi phi} with only small hadronic uncertainties. For fixed S_{psi K_S} the correlation between B(B^+ -> tau^+nu_tau) and S_{psi phi} follows. We also find that MU(2)^3 models could in principle accommodate a negative value of S_{psi phi}, provided |V_ub| is found to be in the ballpark of exclusive determinations and the particular MU(2)^3 model provides a 25% enhancement of epsilon_K. A supersymmetric U(2)^3 model worked out in the Barbieri-School appears to satisfy these requirements. However if B(B^+ -> tau^+nu_tau)>1.0 10^{-4} will be confirmed by future experiments only positive S_{psi phi} is allowed in this framework. We summarize briefly the pattern of flavour violation in rare K and B_{s,d} decays in MU(2)^3 models.Comment: 28 pages, 6 figures; v2: Few references and discussion on CP violation in B_s-> mu^+ mu^- added; v3: Several clarifying comments added, conclusions unchanged, version accepted for publication in JHE

    Effects of the scalar FCNC in b→sl+l−b\to sl^+l^- transitions and supersymmetry

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    We investigate the potential effects of the scalar flavour changing neutral currents that are generated e.g. in supersymmetry with tan⁥ÎČ≫1\tan\beta\gg1 in the b→sl+l−b\to sl^+l^- transitions. Using the experimental upper limit on BR(Bs0→Ό+Ό−)BR(B^0_s\to\mu^+\mu^-) we place stringent model independent constraints on the impact these currents may have on the rates BR(B→XsÎŒ+Ό−)BR(B\to X_s\mu^+\mu^-) and BR(B→KÎŒ+Ό−)BR(B\to K\mu^+\mu^-). We find that in the first case, contrary to the claim made recently in the literature, the maximal potential effects are always smaller than the uncertainty of the Standard Model NNLO prediction, that is of order 5-15%. In the second case, the effects can be large but the experimental errors combined with the unsettled problems associated with the relevant formfactors do not allow for any firm conclusion about the detectability of a new physics signal in this process. In supersymmetry the effects of the scalar flavour changing neutral currents are further constrained by the experimental lower limit on the Bs0B^0_s-Bˉs0\bar B^0_s mass difference, so that most likely no detectable signal of the supersymmetry generated scalar flavour changing neutral currents in processes B→XsÎŒ+Ό−B\to X_s\mu^+\mu^- and B→KÎŒ+Ό−B\to K\mu^+\mu^- is possible.Comment: 24 pages 1 ps figure. Version accepted for Eur.Phys.J.

    Rare K decays in a model of quark and lepton masses

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    An extension of a model of neutrino masses to the quark sector provides an interesting link between these two sectors. A parameter which is important to describe neutrino oscillations and masses is found to be a crucial one appearing in various ``penguin'' operators, in particular the so-called Z penguin. This parameter is severely constrained by the rare decay process KL→Ό+Ό−K_{L} \to \mu^{+} \mu^{-}. This in turn has interesting implications on the decay rates of other rare processes such as KL→ΌeK_{L} \to \mu e, etc..., as well as on the masses of the neutrinos and the masses of the vector-like quarks and leptons which appear in our model.Comment: 34 pages, 10 figures, corrected some typos in the introductio

    Charming penguins in B -> PP decays and the extraction of gamma

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    It is shown that inclusion of charming penguins of the size suggested by short-distance dynamics may shift down by 10o−15o10^o-15^o the value of γ\gamma extracted via the overall fit to the B→PPB \to PP branching ratios. A substantial dependence of the fit on their precise values is found, underscoring the need to improve the reliability of data.Comment: 11 pages, 1 figure, v2 - references reordere

    Brief review of the searches for the rare decays Bs0→Ό+Ό−B^0_s \rightarrow \mu^+ \mu^- and B0→Ό+Ό−B^0 \rightarrow \mu^+ \mu^-

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    The current experimental status of the searches for the very rare decays Bs0→Ό+Ό−B^0_s \rightarrow \mu^+ \mu^- and B0→Ό+Ό−B^0 \rightarrow \mu^+ \mu^- is discussed. These channels are highly sensitive to various extensions of the Standard Model, specially in the scalar and pseudoscalar sector. The recent, most sensitive measurements from the CDF, ATLAS, CMS and LHCb collaborations are discussed and the combined upper exclusion limit on the branching fractions determined by the LHC experiments is shown to be 4.2×10−94.2\times 10^{-9} for Bs0→Ό+Ό−B^0_s \rightarrow \mu^+ \mu^- and 0.8×10−90.8\times 10^{-9} for B0→Ό+Ό−B^0 \rightarrow \mu^+ \mu^-. The implications of these tight bounds on a selected set of New Physics models is sketched.Comment: 20 pages, 15 figures, invited review for Modern Physics Letters

    Penguin decays of B mesons

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    Penguin, or loop, decays of B mesons induce effective flavor-changing neutral currents, which are forbidden at tree level in the Standard Model. These decays give special insight into the CKM matrix and are sensitive to non-standard model effects. In this review, we give a historical and theoretical introduction to penguins and a description of the various types of penguin processes: electromagnetic, electroweak, and gluonic. We review the experimental searches for penguin decays, including the measurements of the electromagnetic penguins b -> s gamma and B -> K* gamma and gluonic penguins B -> K pi, B+ -> omega K+ and B -> eta' K, and their implications for the Standard Model and New Physics. We conclude by exploring the future prospects for penguin physics.Comment: 49 pages, LATEX, 30 embedded figures, submitted to Annual Reviews of Nuclear and Particle Scienc
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