41 research outputs found

    Novi ishodi suradnje NA48 o rijetkim raspadima neutralnih kaona

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    Recent results obtained by the NA48 collaboration on neutral kaon rare decays are reported. A first observation of KS → π 0γγ and a detailed study of KL,S → π +π −e +e − have been performed.Izvješćujemo o nedavnim ishodima suradnje NA48 o rijetkim raspadima neutralnih kaona. Načinili smo prvo opažanje KS → π 0γγ i podrobno proučili raspad KL,S → π +π −e +e −

    Novi ishodi suradnje NA48 o rijetkim raspadima neutralnih kaona

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    Recent results obtained by the NA48 collaboration on neutral kaon rare decays are reported. A first observation of KS → π 0γγ and a detailed study of KL,S → π +π −e +e − have been performed.Izvješćujemo o nedavnim ishodima suradnje NA48 o rijetkim raspadima neutralnih kaona. Načinili smo prvo opažanje KS → π 0γγ i podrobno proučili raspad KL,S → π +π −e +e −

    Phenomenological Constraints on Extended Quark Sectors

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    We study the flavor physics in two extensions of the quark sector of the Standard Model (SM): a four generation model and a model with a single vector--like down--type quark (VDQ). In our analysis we take into account the experimental constraints from tree--level charged current processes, rare Kaon decay processes, rare B decay processes, the ZbbˉZ\to b \bar{b} decay, KK, BB and DD mass differences, and the CP violating parameters \frac \epsilon^\prime}{\epsilon}, ϵK\epsilon_K and aψKa_{\psi K}. All the constraints are taken at two sigma. We find bounds on parameters which can be used to represent the New Physics contributions in these models (λtbd\lambda_{t^ \prime}^{bd}, λtbs\lambda_{t^ \prime}^{bs} and λtsd\lambda_{t^ \prime}^{sd} in the four--generation model, and UbdU_{bd}, UbsU_{bs} and UsdU_{sd} in the VDQ model) due to all the above constraints. In both models the predicted ranges for aSLa_{SL} (the CP asymmetry in semi-leptonic decays), ΔMD\Delta M_D, B(K+π+ννˉ)B(K^+\to\pi^+ \nu \bar{\nu}), B(KLπ0ννˉ)B(K_L\to\pi^0 \nu \bar{\nu}) and B(KLμμˉ)SDB(K_L\to \mu \bar{\mu})_{SD} can be significantly higher than the predictions of the SM, while the allowed ranges for aψKa_{\psi K} and for ΔmBS\Delta m_{B_S} are consistent with the SM prediction.Comment: 22 pages, 5 figures (v3: added a reference, updated a reference, added missing units

    On V_ud determination from kaon decays

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    The pion beta decay pi^+ -> pi^0 e^+ nu proceeds through pure weak vector hadronic currents and, therefore, the theoretical prediction for it is more reliable than for the processes with axial-vector current contribution. For example, recently the pion beta decay has been used for V_ud determination. The main aim of this letter is to point that kaon beta decay K^0 -> K^+(pi^+ pi^0) e^- nu-bar analogously can be used for this purpose.Comment: 3 pages, no figures, one reference adde

    Search for the dark photon in π0π^0 decays

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    A sample of 1.69imes1071.69 imes 10^7 fully reconstructed pi0ogammae+epi^0 ogamma e^+e^- decay candidates collected by the NA48/2 experiment at CERN in 2003--2004 is analysed to search for the dark photon (AA') production in the pi0ogammaApi^0 ogamma A' decay followed by the prompt Aoe+eA' o e^+e^- decay. No signal is observed, and an exclusion region in the plane of the dark photon mass mAm_A' and mixing parameter arepsilon2arepsilon^2 is established. The obtained upper limits on arepsilon2arepsilon^2 are more stringent than the previous limits in the mass range 9~ m MeV/c^2<70~ m MeV/c^2. The NA48/2 sensitivity to the dark photon production in the KpmopipmAK^pm opi^pm A' decay is also evaluated

    epsilon'/epsilon at the NLO: 10 Years Later

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    During the last four years several parameters relevant for the analysis of the CP-violating ratio epsilon'/epsilon improved and/or changed significantly. In particular, the experimental value of epsilon'/epsilon and the strange quark mass decreased, the uncertainty in the CKM factor has been reduced, and for a value of the hadronic matrix element of the dominant electroweak penguin operator Q_8, some consensus has been reached among several theory groups. In view of this situation, ten years after the first analyses of epsilon'/epsilon at the next-to-leading order, we reconsider the analysis of epsilon'/epsilon within the SM and investigate what can be said about the hadronic Q_6 matrix element of the dominant QCD penguin operator on the basis of the present experimental value of epsilon'/epsilon and todays values of all other parameters. Employing a conservative range for the reduced electroweak penguin matrix element R_8=1.0+-0.2 from lattice QCD, and present values for all other input parameters, on the basis of the current world average for epsilon'/epsilon, we obtain the reduced hadronic matrix element of the dominant QCD penguin operator R_6=1.23+-0.16 implying _0^NDR(m_c) ~ -0.8 _2^NDR(m_c). We compare these results with those obtained in large-N_c approaches in which generally R_6 ~ R_8 and _0^NDR(m_c) is chirally suppressed relatively to _2^NDR(m_c). We present the correlation between R_6 and R_8 that is implied by the data on epsilon'/epsilon provided new physics contributions to epsilon'/epsilon can be neglected.Comment: 18 pages, 1 eps figure, version to appear in JHE

    Order p^6 chiral couplings from the scalar K Pi form factor

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    Employing results from a recent determination of the scalar KPi form factor F_0^KPi within a coupled channel dispersion relation analysis \cite{JOP01}, in this work we calculate the slope and curvature of F_0^KPi(t) at zero momentum transfer. Knowledge of the slope and curvature of the scalar KPi form factor, together with a recently calculated expression for F_0^KPi(t) in chiral perturbation theory at order p^6, enable to estimate the O(p^6) chiral constants C_12^r=(0.3 +- 5.4)10^-7 and (C_12^r+C_34^r)=(3.2 +- 1.5)10^-6. Our findings also allow to estimate the contribution coming from the C_i to the vector form factor F_+^KPi(0) which is crucial for a precise determination of |V_us| from K_l3 decays. Our result F_+^KPi(0)|_C_i^r=-0.018 +- 0.009, though inflicted with large uncertainties, is in perfect agreement with a previous estimate by Leutwyler and Roos already made twenty years ago.Comment: 19 pages, discussion of scale dependence of the chiral couplings added; version to appear in JHE

    Charged Kaon K \to 3 pi CP Violating Asymmetries at NLO in CHPT

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    We give the first full next-to-leading order analytical results in Chiral Perturbation Theory for the charged Kaon K \to 3 pi slope g and decay rates CP-violating asymmetries. We have included the dominant Final State Interactions at NLO analytically and discussed the importance of the unknown counterterms. We find that the uncertainty due to them is reasonable just for \Delta g_C, i.e. the asymmetry in the K^+ \to pi^+ pi^+ pi^- slope g; we get \Delta g_C = -(2.4 +- 1.2) 10^{-5}. The rest of the asymmetries are very sensitive to the unknown counterterms. In particular, the decay rate asymmetries can change even sign. One can use this large sentivity to get valuable information on those counterterms and on Im(G_8) coupling --very important for the CP-violating parameter epsilon'_K-- from the eventual measurement of these asymmetries. We also provide the one-loop O(e^2 p^2) electroweak octet contributions for the neutral and charged Kaon K \to 3 pi decays.Comment: 43+2 pages, 2 figures. Version accepted in JHEP. Small changes in the final numerics of CP asymmetries due to change in input valu
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