58,838 research outputs found

    Quasi-Inclusive and Exclusive decays of BB to η′\eta'

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    We consider the effective Hamiltonian of four quark operators in the Standard Model in the exclusive and quasi-inclusive decays of the type B→K(∗)η′B\to K^{(*)} \eta^{\prime}, B→η′XsB\to \eta' X_s, where XsX_s contains a single Kaon. Working in the factorization assumption we find that the four quark operators can account for the recently measured exclusive decays B→η′(η)KB\to \eta^{\prime}(\eta) K and B→KπB\to K \pi for appropriate choice of form factors but cannot explain the large quasi-inclusive rate.Comment: Calculation of B→KπB \to K \pi added and the correct BSW form factors have been used. Latex 13 papges, 1 figur

    Convergence of Adaptive Finite Element Approximations for Nonlinear Eigenvalue Problems

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    In this paper, we study an adaptive finite element method for a class of a nonlinear eigenvalue problems that may be of nonconvex energy functional and consider its applications to quantum chemistry. We prove the convergence of adaptive finite element approximations and present several numerical examples of micro-structure of matter calculations that support our theory.Comment: 24 pages, 12 figure

    Constraints on the phase γ\gamma and new physics from B→KπB\to K\pi Decays

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    Recent results from CLEO on B→KπB\to K\pi indicate that the phase γ\gamma may be substantially different from that obtained from other fit to the KM matrix elements in the Standard Model. We show that γ\gamma extracted using B→Kπ,ππB\to K\pi, \pi\pi is sensitive to new physics occurring at loop level. It provides a powerful method to probe new physics in electroweak penguin interactions. Using effects due to anomalous gauge couplings as an example, we show that within the allowed ranges for these couplings information about γ\gamma obtained from B→Kπ,ππB\to K \pi, \pi\pi can be very different from the Standard Model prediction.Comment: Revised version with analysis done using new data from CLEO. RevTex, 11 Pages with two figure

    Concurrence of superposition

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    The bounds on concurrence of the superposition state in terms of those of the states being superposed are studied in this paper. The bounds on concurrence are quite different from those on the entanglement measure based on von Neumann entropy (Phys. Rev. Lett. 97, 100502 (2006)). In particular, a nonzero lower bound can be provided if the states being superposed are properly constrained.Comment: 4 page

    Topological phase due to electric dipole moment and magnetic monopole interaction

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    We show that there is an anologous Aharonov-Casher effect on a neutral particle with electric dipole moment interacting with a magnetic filed produced by magnetic monopoles.Comment: 8 page

    Tachyon field inspired dark energy and supernovae constraints

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    The tachyon field in cosmology is studied by applying the generating function method to obtain exact solutions. The equation of state parameter of the tachyon field is w=−1+ϵϕ2˙w=-1+\epsilon\dot{\phi^2}, which can be expressed as a function in terms of the redshift zz. Based on these solutions, we propose some tachyon-inspired dark energy models to explore the properties of the corresponding cosmological evolution. The explicit relations between Hubble parameter and redshift enable us to test the models with SNe Ia data sets easily. In the current work we employ the SNe Ia data with the parameter A\mathcal{A} measured from the SDSS and the shift parameter R\mathcal{R} from WMAP observations to constrain the parameters in our models.Comment: 6 pages, 2 figures; v2: accepted by IJMP

    Bˉ0→π+X\bar B^0 \to \pi^+ X in the Standard Model

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    In this paper we investigate the possibility of studying B→πB\to \pi form factor using the semi-inclusive decays Bˉ0→π++Xq\bar B^0 \to \pi^+ + X_q. In general B→PXB\to PX semi-inclusive decays involve several hadronic parameters. But for Bˉ0→π+Xq\bar B^0 \to \pi^+ X_q decays we find that in the factorization approximation, the only unknown hadronic parameters are the form factors F0,1B→πF^{B\to \pi}_{0,1}. Therefore these form factors can be studied in Bˉ0→π+Xq\bar B^0 \to \pi^+ X_q decays. Using theoretical model calculations for the form factors the branching ratios for Bˉ0→π+Xd(ΔS=0)\bar B^0 \to \pi^+ X_d(\Delta S = 0) and Bˉ0→π+Xs(ΔS=−1)\bar B^0 \to \pi^+ X_s (\Delta S = -1), with the cut Eπ>2.1E_{\pi} > 2.1 GeV, are estimated to be in the ranges of (3.1∼4.9)×10−5(F1B→π(0)/0.33)2(3.1\sim 4.9) \times 10^{-5}(F^{B\to \pi}_1(0)/0.33)^2 and (2.5∼4.2)×10−5(F1B→π(0)/0.33)2(2.5\sim 4.2)\times 10^{-5}(F_1^{B\to \pi}(0)/0.33)^2, respectively, depending on the value of γ\gamma. The combined branching ratio for Bˉ0→π+(Xd+Xs)\bar B^0 \to \pi^+ (X_d+ X_s) is about 7.4×10−5(F1B→π(0)/0.33)27.4\times 10^{-5} (F^{B\to \pi}_1(0)/0.33)^2 and is insensitive to γ\gamma. We also discuss CP asymmetries in these decay modes.Comment: RevTex 8 pages and two figure

    Anomalous Phase Transition in Strained SrTiO3_3 Thin Films

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    We have studied the cubic to tetragonal phase transition in epitaxial SrTiO3_3 films under various biaxial strain conditions using synchrotron X-ray diffraction. Measuring the superlattice peak associated with TiO6_6 octahedra rotation in the low temperature tetragonal phase indicates the presence of a phase transition whose critical temperature is a strong function of strain, with TC_C as much as 50K above the corresponding bulk temperature. Surprisingly, the lattice constants evolve smoothly through the transition with no indication of a phase change. This signals an important change in the nature of the phase transition due to the epitaxy strain and substrate clamping effect. The internal degrees of freedom (TiO6_6 rotations) have become uncoupled from the overall lattice shape.Comment: 4 pages, 3 figures, REVTeX
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