11 research outputs found

    Constraining the Unitarity Triangle with B -> V gamma

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    We discuss the exclusive radiative decays B→K∗γB\to K^{*}\gamma, Bâ†’ÏÎłB \to\rho\gamma, and Bâ†’Ï‰ÎłB\to\omega\gamma in QCD factorization within the Standard Model. The analysis is based on the heavy-quark limit of QCD. Our results for these decays are complete to next-to-leading order in QCD and to leading order in the heavy-quark limit. Special emphasis is placed on constraining the CKM-unitarity triangle from these observables. We propose a theoretically clean method to determine CKM parameters from the ratio of the B→ρlÎœB\to\rho l\nu decay spectrum to the branching fraction of Bâ†’ÏÎłB\to\rho\gamma. The method is based on the cancellation of soft hadronic form factors in the large energy limit, which occurs in a suitable region of phase space. The ratio of the Bâ†’ÏÎłB\to\rho\gamma and B→K∗γB\to K^{*}\gamma branching fractions determines the side RtR_{t} of the standard unitarity triangle with reduced hadronic uncertainties. The recent Babar bound on B(B0→ρ0Îł)B(B^0\to\rho^0\gamma) implies Rt<0.81(Ο/1.3)R_t < 0.81 (\xi/1.3), with the limiting uncertainty coming only from the SU(3) breaking form factor ratio Ο\xi. This constraint is already getting competitive with the constraint from BsB_{s}-Bˉs\bar B_{s} mixing. Phenomenological implications from isospin-breaking effects are briefly discussed.Comment: 23 pages, 8 figure

    Supersymmetric Contributions to Bs->K+K-

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    Inspired by the existing calculation of B->piK decays in supersymmetry (SUSY), we evaluate the dominant SUSY contributions to Bs->K+K-. We show that the observables of this process can be significantly modified in the presence of SUSY. In particular, the branching ratio can be increased considerably compared to the prediction of the standard model (SM). The effect is even more dramatic for the CP-violating asymmetries A_dir and A_mix. These asymmetries, expected to be small in the SM (A_dir is predicted to take only positive values), change drastically with SUSY contributions. The measurement of these observables can therefore be used to detect the presence of physics beyond the SM, and put constraints on its parameters.Comment: 17 pages, 2 figures. This new version contains one added reference and some minor style change

    R-Parity Violation and Non-Abelian Discrete Family Symmetry

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    We investigate the implications of R-parity violating operators in a model with family symmetry. The family symmetry can determine the form of R-parity violating operators as well as the Yukawa matrices responsible for fermion masses and mixings. In this paper we consider a concrete model with non-abelian discrete symmetry Q_6 which contains only three R-parity violating operators. We find that ratios of decay rates of the lepton flavor violating processes are fixed thanks to the family symmetry, predicting BR(tau to 3e)/BR(tau to 3mu) ~ 4 m_{mu}^2/m_{tau}^2.Comment: 20 pages, 3 figure

    Can there be any new physics in b -> d penguins

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    We analyze the possibility of observing new physics effects in the b→db \to d penguin amplitudes. For this purpose, we consider the decay mode B→K0Kˉ0B \to K^0 \bar K^0 , which has only b→db \to d penguin contributions. Using the QCD factorization approach, we find very tiny CP violating effects in the standard model for this process. Furthermore, we show that the minimal supersymmetric standard model with LRLR mass insertion and R-parity violating supersymmetric model can provide substantial CP violation effects. Observation of sizable CP violation in this mode would be a clear signal of new physics.Comment: Published versio

    Non-factorizable Contributions to B→ππB \to \pi\pi Decays

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    We investigate to what extent the experimental information on B→ππB \to \pi\pi branching fractions and CP asymmetries can be used to better understand the QCD dynamics in these decays. For this purpose we decompose the independent isospin amplitudes into factorizable and non-factorizable contributions. The former can be estimated within the framework of QCD factorization for exclusive BB decays. The latter vanish in the heavy-quark limit, mb→∞m_b \to \infty, and are treated as unknown hadronic parameters. We discuss at some length in which way the non-factorizable contributions are treated in different theoretical and phenomenological frameworks. We point out the potential differences between the phenomenological treatment of power-corrections in the ``BBNS approach'', and the appearance of power -suppressed operators in soft-collinear effective theory (SCET). On that basis we define a handful of different (but generic) scenarios where the non-factorizable part of isospin amplitudes is parametrized in terms of three or four unknowns, which can be constrained by data. We also give some short discussion on the implications of our analysis for B→πKB \to \pi K decays. In particular, since non-factorizable QCD effects in B→ππB \to \pi \pi may be large, we cannot exclude sizeable non-factorizable effects, which violate SU(3)FSU(3)_F flavour symmetry, or even isospin symmetry (via long-distance QED effects). This may help to explain certain puzzles in connection with isospin-violating observables in B→πKB \to \pi K decays.Comment: published version, minor correction

    The 2004 UTfit Collaboration Report on the Status of the Unitarity Triangle in the Standard Model

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    Using the latest determinations of several theoretical and experimental parameters, we update the Unitarity Triangle analysis in the Standard Model. The basic experimental constraints come from the measurements of |V_ub/V_cb|, Delta M_d, the lower limit on Delta M_s, epsilon_k, and the measurement of the phase of the B_d - anti B_d mixing amplitude through the time-dependent CP asymmetry in B^0 to J/psi K^0 decays. In addition, we consider the direct determination of alpha, gamma, 2 beta + gamma and cos(2 beta) from the measurements of new CP-violating quantities, recently performed at the B factories. We also discuss the opportunities offered by improving the precision of the various physical quantities entering in the determination of the Unitarity Triangle parameters. The results and the plots presented in this paper can also be found at http://www.utfit.org, where they are continuously updated with the newest experimental and theoretical results.Comment: 32 pages, 17 figures. High resolution figures and updates can be found at http://www.utfit.org v2: misprints correcte

    Exploring the Unitarity Triangle through CP violation observables in Bs→K+K−B_s \to K^+ K^-

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    We discuss the determination of the CKM parameters from the forthcoming CPCP violation observables in Bs→K+K−B_s \to K^+ K^- decays. Combining the information on mixing induced CP violation in Bs→K+K−B_s \to K^+ K^-, with the Bd→J/ψKsB_d \to J/\psi K_s precision observable sin⁥2ÎČ\sin 2\beta and the Bs0B^0_s--Bs0ˉ\bar{B^0_s} mixing phase ϕs\phi_s, we propose a determination of the unitarity triangle (ρˉ,ηˉ)(\bar\rho, \bar\eta). Computing the penguin parameters (r,Ξ)(r, \theta) within QCD factorization yield precise determination of (ρˉ,ηˉ)(\bar\rho, \bar\eta), reflected by a weak dependence on the Ξ\theta which is shown as a second order effect. The impact of the direct CP violation observable CKKC_{KK} on the penguin parameters are investigated and a lower bound on CKKC_{KK} is extracted. We also discuss the effect of the Bs0B^0_s--Bs0ˉ\bar{B^0_s} new physics mixing phase on the penguin parameters (r,Ξ)(r, \theta) and SKKS_{KK}. Using the SU(3)-flavour symmetry argument and the current BB-factories data provided by the Bd→π+π−B_d \to \pi^+ \pi^- modes, we complement the Bs→K+K−B_s \to K^+ K^- CP-violating observables in a variety of ways, in particular we find that SKK>0S_{KK}>0. Finally we analyze systematically the SU(3)-symmetry breaking factor within QCD factorization.Comment: 22 pages, 6 figures, typos corrected, reference and some remarks adde

    Direct CP Violation, Branching Ratios and Form Factors B→πB \to \pi, B→KB \to K in BB Decays

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    The B→πB \to \pi and B→KB \to K transitions involved in hadronic B decays are investigated in a phenomenological way through the framework of QCD factorization. By comparing our results with experimental branching ratios from the BELLE, BABAR and CLEO Collaborations for all the B decays including either a pion or a kaon, we propose boundaries for the transition form factors B→πB \to \pi and B→KB \to K depending on the CKM matrix element parameters ρ\rho and η\eta. From this analysis, the form factors required to reproduce the experimental data for branching ratios are FB→π=0.31±0.12F^{B \to \pi}= 0.31 \pm 0.12 and FB→K=0.37±0.13F^{B \to K}= 0.37\pm 0.13. We calculate the direct CP violating asymmetry parameter, aCPa_{CP}, for B→π+π−πB \to \pi^{+} \pi^{-} \pi and B→π+π−KB \to \pi^{+} \pi^{-} K decays, in the case where ρ−ω\rho-\omega mixing effects are taken into account. Based on these results, we find that the direct CP asymmetry for B−→π+π−π−B^{-} \to \pi^{+} \pi^{-} \pi^{-}, Bˉ0→π+π−π0\bar{B}^{0} \to \pi^{+} \pi^{-} \pi^{0}, B−→π+π−K−B^{-} \to \pi^{+} \pi^{-} K^{-}, and Bˉ0→π+π−Kˉ0\bar{B}^{0} \to \pi^{+} \pi^{-} \bar{K}^{0}, reaches its maximum when the invariant mass π+π−\pi^{+} \pi^{-} is in the vicinity of the ω\omega meson mass. The inclusion of ρ−ω\rho-\omega mixing provides an opportunity to erase, without ambiguity, the phase uncertainty mod(π)(\pi) in the determination of the CKM angles α\alpha in case of b→ub\to u and Îł\gamma in case of b→sb \to s.Comment: 74 pages, 15 figures, 8 tables. A few misprints corrected, two references adde

    Minimal Flavour Violation Waiting for Precise Measurements of Delta M_s, S_{psi phi}, A^s_SL, |V_ub|, gamma and B^0_{s,d} -> mu+ mu-

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    We emphasize that the recent measurements of the B^0_s - bar B^0_s mass difference Delta M_s by the CDF and D0 collaborations offer an important model independent test of minimal flavour violation (MFV). The improved measurements of the angle gamma in the unitarity triangle and of |V_ub| from tree level decays, combined with future accurate measurements of Delta M_s, S_{psi K_S}, S_{psi phi}, Br(B_{d,s} -> mu+ mu-), Br(B -> X_{d,s} nu bar nu), Br(K+ -> pi+ nu bar nu) and Br(K_L -> pi^0 nu bar nu) and improved values of the relevant non-perturbative parameters, will allow to test the MFV hypothesis in a model independent manner to a high accuracy. In particular, the difference between the reference unitarity triangle obtained from tree level processes and the universal unitarity triangle (UUT) in MFV models would signal either new flavour violating interactions and/or new local operators that are suppressed in MFV models with low tan(beta), with the former best tested through S_{psi phi} and K_L -> pi^0 nu bar nu. A brief discussion of non-MFV scenarios is also given. In this context we identify in the recent literature a relative sign error between Standard Model and new physics contributions to S_{psi phi}, that has an impact on the correlation between S_{psi phi} and A^s_SL. We point out that the ratios S_{psi phi}/A^s_SL and (Delta M_s)/(Delta Gamma_s) will allow to determine (Delta M_s)/(Delta M_s)^SM. Similar proposals for the determination of (Delta M_d)/(Delta M_d)^SM are also given.Comment: 22 pages, 8 figures, 1 table. Extended discussion of the correlation between S_{psi phi} and A^s_SL and new proposals to determine Delta M_q/(Delta M_q)^SM from future measurements, with respect to the first version. Minor changes and few references adde
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