449 research outputs found

    Color suppressed contributions to the decay modes B_{d,s} -> D_{s,d} D_{s,d}, B_{d,s} -> D_{s,d} D^*_{s,d}, and B_{d,s} -> D^*_{s,d} D^*_{s,d}

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    The amplitudes for decays of the type Bd,s→Ds,dDs,dB_{d,s} \to D_{s,d} D_{s,d}, have no factorizable contributions, while Bd,s→Ds,dDs,d∗B_{d,s} \to D_{s,d} D^*_{s,d}, and Bd,s→Ds,d∗Ds,d∗B_{d,s} \to D^*_{s,d} D^*_{s,d} have relatively small factorizable contributions through the annihilation mechanism. The dominant contributions to the decay amplitudes arise from chiral loop contributions and tree level amplitudes which can be obtained in terms of soft gluon emissions forming a gluon condensate. We predict that the branching ratios for the processes Bˉd0→Ds+Ds−\bar B^0_d \to D_s^+ D_s^-, Bˉd0→Ds+∗Ds−\bar B^0_d \to D_s^{+*} D_s^- and Bˉd0→Ds+Ds−∗\bar B^0_d \to D_s^+ D_s^{-*} are all of order (2−3)×10−4(2- 3) \times 10^{-4}, while Bˉs0→Dd+Dd−\bar B^0_s \to D_d^+ D_d^-, Bˉs0→Dd+∗Dd−\bar B^0_s \to D_d^{+*} D_d^- and Bˉs0→Dd+Dd−∗\bar B^0_s \to D_d^+ D_d^{-*} are of order (4−7)×10−3(4- 7) \times 10^{-3}. We obtain branching ratios for two D∗D^*'s in the final state of order two times bigger.Comment: 15 pages, 4 figure

    Violation of quark-hadron duality and spectral chiral moments in QCD

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    We analyze the spectral moments of the V-A two-point correlation function. Using all known short-distance constraints and the most recent experimental data from tau decays, we determine the lowest spectral moments, trying to assess the uncertainties associated with the so-called violations of quark-hadron duality. We have generated a large number of 'acceptable' spectral functions, satisfying all conditions, and have used them to extract the wanted hadronic parameters through a careful statistical analysis. We obtain accurate values for the ChPT couplings L10 and C87, and a realistic determination of the dimension six and eight contributions in the operator product expansion, O6=(-5.4^{+3.6}_{-1.6})*10^-3 GeV^6 and O8=(-8.9^{+12.6}_{-7.4})*10^-3 GeV^8, showing that the duality-violation effects have been usually underestimated in previous literature

    Massive Pions, Anomalies and Baryons in Holographic QCD

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    We consider a holographic model of QCD, obtained by a very simple modification of the original construction, which describes at the same time the pion mass, the QCD anomalies and the baryons as topological solitons. We study in detail its phenomenological implications in both the mesonic and baryonic sectors and compare with the observations.Comment: 31 pages, 2 figures; v2: Version published in Nucl. Phys.

    Masses and couplings of vector mesons from the pion electromagnetic, weak, and \pi\gamma transition form factors

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    We analyse the pion electromagnetic, charged-current, and Ï€Îł\pi\gamma transition form factors at timelike momentum transfers qq, q2=s≀1.4q^2=s\le 1.4 GeV2^2, using a dispersion approach. We discuss in detail the propagator matrix of the photon-vector-meson system and define certain reduced amplitudes, or vertex functions, describing the coupling of this system to final states. We then apply the derived analytic expressions to the analysis of the recent e+e−→π+π−e^+e^-\to \pi^+\pi^-, τ−→π−π0Μτ\tau^-\to \pi^-\pi^0\nu_\tau, and e+e−→π0Îłe^+e^-\to \pi^0\gamma data. We find the reduced amplitudes for the coupling of the photon and vector mesons to two pseudoscalars to be constant, independent of ss, in the range considered, indicating a "freezing" of the amplitudes for s≀1s\le 1 GeV. The fit to the form factor data leads to the following values of the Breit-Wigner resonance masses m_{\rho^-}=775.3\pm 0.8 MeV, m_{\rho^0}=773.7\pm 0.6 MeV and m_\omega=782.43\pm 0.05 MeV, where the errors are only statistical.Comment: revtex, 23 page

    Issues in determining alpha_s from hadronic tau decay and electroproduction data

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    We discuss some key issues associated with duality-violating and non-perturbative OPE contributions to the theoretical representations of light quark current-current two-point functions and relevant to precision determinations of alpha_s from hadronic tau decay and electroproduction cross-section data. We demonstrate that analyses with an explicit representation of duality-violating effects are required to bring theoretical errors in such extractions under control, motivating the accompanying paper in these proceedings, which presents the results of such an analysis.Comment: 5 pages, 4 figures. Prepared for the Proceedings of the International Workshop on e+e- collisions from Phi to Psi (PHIPSI11), Sep. 19-22, 2011, BINP, Novosibirsk, Russi

    Remark on the perturbative component of inclusive τ\tau-decay

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    In the context of the inclusive τ\tau-decay, we analyze various forms of perturbative expansions which have appeared as modifications of the original perturbative series. We argue that analytic perturbation theory, which combines renormalization-group invariance and Q2Q^2-analyticity, has significant merits favoring its use to describe the perturbative component of τ\tau-decay.Comment: 5 pages, ReVTEX, 2 eps figures. Revised paper includes clarifying remarks and corrected references. To be published in Phys. Rev.

    Griffiths-McCoy singularities in random quantum spin chains: Exact results through renormalization

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    The Ma-Dasgupta-Hu renormalization group (RG) scheme is used to study singular quantities in the Griffiths phase of random quantum spin chains. For the random transverse-field Ising spin chain we have extended Fisher's analytical solution to the off-critical region and calculated the dynamical exponent exactly. Concerning other random chains we argue by scaling considerations that the RG method generally becomes asymptotically exact for large times, both at the critical point and in the whole Griffiths phase. This statement is checked via numerical calculations on the random Heisenberg and quantum Potts models by the density matrix renormalization group method.Comment: 4 pages RevTeX, 2 figures include

    The effect of rare regions on a disordered itinerant quantum antiferromagnet with cubic anisotropy

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    We study the quantum phase transition of an itinerant antiferromagnet with cubic anisotropy in the presence of quenched disorder, paying particular attention to the locally ordered spatial regions that form in the Griffiths region. We derive an effective action where these rare regions are described in terms of static annealed disorder. A one loop renormalization group analysis of the effective action shows that for order parameter dimensions p<4p<4 the rare regions destroy the conventional critical behavior. For order parameter dimensions p>4p>4 the critical behavior is not influenced by the rare regions, it is described by the conventional dirty cubic fixed point. We also discuss the influence of the rare regions on the fluctuation-driven first-order transition in this system.Comment: 6 pages RevTe

    Phase separation in supersolids

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    We study quantum phase transitions in the ground state of the two dimensional hard-core boson Hubbard Hamiltonian. Recent work on this and related models has suggested ``supersolid'' phases with simultaneous diagonal and off-diagonal long range order. We show numerically that, contrary to the generally held belief, the most commonly discussed ``checkerboard'' supersolid is thermodynamically unstable. Furthermore, this supersolid cannot be stabilized by next near neighbour interaction. We obtain the correct phase diagram using the Maxwell construction. We demonstrate the ``striped'' supersolid is thermodynamically stable and is separated from the superfluid phase by a continuous phase transition.Comment: 4 pages, 4 eps figures, include
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