12 research outputs found

    The Bosonization of the Electroweak Penguin Operators

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    We give the complete O(p2)O(p^2) bosonization of the electroweak Penguin operators Q7,8Q_{7,8} and compare the result with that of the gluon Penguin operators Q5,6Q_{5,6}. We find that, in addition to the usual (constant and current-current) parts, there are three new terms not discussed previously in the literature. Two of these are present in the factorization approximation and should be included in the standard definition of the B7,8B_{7,8}-factors. The impact of these corrections on the direct CPCP-violating parameter ε/ε\varepsilon '/\varepsilon is briefly discussed.Comment: 9 pages, uuencoded Latex + eps file

    Four Zero Texture Fermion Mass Matrices in SO(10) GUT

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    We attempt the integration of the phenomenologically successful four zero texture of fermion mass matrices with the renormalizable SO(10) GUT. The resulting scenario is found to be highly predictive. Firstly, we examine the phenomenological implications of a class of the lepton mass matrices with parallel texture structures and obtain interesting constraints on the parameters of the charged lepton and the neutrino mass matrices. We combine these phenomenological constraints with the constraints obtained from SO(10) GUT to reduce the number of the free parameters and to further constrain the allowed ranges of the free parameters. The solar/atmospheric mixing angles obtained in this analysis are in fairly good agreement with the data.Comment: 14 pages, 3 figures, 1 tabl

    The Physics of K0Kˉ0K^0 -\bar K^0 Mixing: B^K\widehat{B}_K and ΔMLS\Delta M_{LS} in the Chiral Quark Model

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    We compute the B^K\widehat B_K parameter and the mass difference ΔMLS\Delta M_{LS} of the K0Kˉ0K^0-\bar K^0 system by means of the chiral quark model. The chiral coefficients of the relevant ΔS=2\Delta S=2 and ΔS=1\Delta S=1 chiral lagrangians are computed via quark-loop integration. We include the relevant effects of one-loop corrections in chiral perturbation theory. The final result is very sensitive to non-factorizable corrections of O(αSN)O(\alpha_S N) coming from gluon condensation. The size of the gluon condensate is determined by fitting the experimental value of the amplitude K+π+π0K^+ \to \pi^+\pi^0. By varying all the relevant parameters we obtain B^K=0.87±0.33 .\widehat{B}_K= 0.87 \pm 0.33\ . We evaluate within the model the long-distance contributions to ΔMLS\Delta M_{LS} induced by the double insertion of the ΔS=1\Delta S = 1 chiral lagrangian and study the interplay between short- and long-distance amplitudes. By varying all parameters we obtain ΔMLSth/ΔMLSexp=0.760.34+0.64.\Delta M_{LS}^{th}/\Delta M_{LS}^{exp} = 0.76 ^{+0.64}_{-0.34} . Finally, we investigate the phenomenological constraints on the Kobayashi-Maskawa parameter Im λt\lambda _t entering the determination of ϵ/ϵ\epsilon'/\epsilon.Comment: 31 pages, Latex file including 7 eps figures. Revised version to appear in Nucl. Phys.

    The ΔS=1\Delta S = 1 Weak Chiral Lagrangian as the Effective Theory of the Chiral Quark Model

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    We use the chiral quark model to estimate the coefficients of the weak chiral lagrangian as obtained from the bosonization of the ten relevant operators of the ΔS=1\Delta S = 1 effective quark lagrangian. All contributions of order Nc2N_c^2 as well as NcN_c and αsNc\alpha_s N_c are included. The chiral coefficients are given in terms of fπf_{\pi}, the quark and gluon condensates and the scale-dependent NLO Wilson coefficients of the corresponding operators. In addition, they depend on the constituent quark mass MM, a parameter characteristic of the model. The γ5\gamma_5-scheme dependence of the chiral coefficients, computed via dimensional regularization, and the Fierz transformation properties of the operator basis are discussed in detail. We apply our result to the evaluation of the hadronic matrix elements for the decay K02πK^0 \rightarrow 2 \pi, consistently including the renormalization induced by the meson loops. The effect of this renormalization is sizable and introduces a long-distance scale dependence that matches in the physical amplitudes the short-distance scale dependence of the Wilson coefficients.Comment: Revised version to appear in Nucl. Phys. B 48 pages, uuencoded LATEX file including 4 eps figure

    The ΔI=1/2\Delta I = 1/2 Selection Rule

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    We compute the isospin I=0I= 0 and 2 amplitudes for the decay of a kaon into two pions by estimating the relevant hadronic matrix elements in the chiral quark model. The results are parametrized in terms of the quark and gluon condensates and of the constituent quark mass MM. The latter is a parameter characteristic of the model, that we restrict by matching the results in the two γ5\gamma_5-schemes (HV and NDR) of dimensional regularization. We find that, for values of these parameters within the current determinations, the ΔI=1/2\Delta I= 1/2 selection rule is well reproduced by means of the cumulative effects of short-distance NLO Wilson coefficients, penguin diagrams, non-factorizable soft-gluon corrections and meson-loop renormalization.Comment: Revised version to be published in Nuclear Physics

    #epsilon#/#epsilon# O(p"4) in the chiral expansion

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    Consiglio Nazionale delle Ricerche - Biblioteca Centrale -. P.le Aldo Moro, 7, Rome / CNR - Consiglio Nazionale delle RichercheSIGLEITItal

    The physics of K"0-K"0 mixing:B_K and DELTAM_ls in the chiral quark model

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    Consiglio Nazionale delle Ricerche (CNR). Biblioteca Centrale / CNR - Consiglio Nazionale delle RichercheSIGLEITItal

    The DELTA I = 1/2 selection rule

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    Consiglio Nazionale delle Ricerche (CNR). Biblioteca Centrale / CNR - Consiglio Nazionale delle RichercheSIGLEITItal

    The DELTA S = 1 weak Chiral Lagrangian as the effective theory of the Chiral quark model

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    Consiglio Nazionale delle Ricerche (CNR). Biblioteca Centrale / CNR - Consiglio Nazionale delle RichercheSIGLEITItal
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