4,468 research outputs found

    Semileptonic Bc−→D∗0ℓνB_{c}^{-}\to D^{*0}\ell\nu transition in three--point QCD sum rules and HQET with gluon condensate corrections

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    Taking into account the gluon condensate contributions, the form factors of the semileptonic Bc−→D∗0ℓνB_c^- \to D^{*0}\ell\nu transition with l=τ,el=\tau, e are calculated in the framework of the three point QCD sum rules. The heavy quark effective theory limit of the form factors are also computed. The relevant total decay width as well as the branching ratio are evaluated and compared with the predictions of the other non-perturbative approaches.Comment: 27 Pages, 4 Figures and 4 Table

    Physics of B_c mesons

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    In the framework of potential models for heavy quarkonium the mass spectrum for the system (bˉc\bar b c) is considered. Spin-dependent splittings, taking into account a change of a constant for effective coulomb interaction between the quarks, and widths of radiative transitions between the (bˉc\bar b c) levels are calculated. In the framework of QCD sum rules, masses of the lightest vector Bc∗B_c^* and pseudoscalar BcB_c states are estimated, scaling relation for leptonic constants of heavy quarkonia is derived, and the leptonic constant fBcf_{B_c} is evaluated. The BcB_c decays are considered in the framework of both the potential models and the QCD sum rules, where the significance of Coulomb-like corrections is shown. The relations, following from the approximate spin symmetry for the heavy quarks in the heavy quarkonium, are analysed for the form factors of the semileptonic weak exclusive decays of BcB_c. The BcB_c lifetime is evaluated with the account of the corrections to the spectator mechanism of the decay, because of the quark binding into the meson. The total and differential cross sections of the BcB_c production in different interactions are calculated. The analytic expressions for the fragmentational production cross sections of BcB_c are derived. The possibility of the practical BcB_c search in the current and future experiments at electron-positron and hadron colliders is analysed.Comment: 81 page, latex, ihep.sty is required and attached in the end of the file after \end{document}, figures are not availabl

    The Kontsevich tetrahedral flow revisited

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    We prove that the Kontsevich tetrahedral flow PË™=Qa:b(P)\dot{\mathcal{P}} = \mathcal{Q}_{a:b} (\mathcal{P}), the right-hand side of which is a linear combination of two differential monomials of degree four in a bi-vector P\mathcal{P} on an affine real Poisson manifold NnN^n, does infinitesimally preserve the space of Poisson bi-vectors on NnN^n if and only if the two monomials in Qa:b(P)\mathcal{Q}_{a:b} (\mathcal{P}) are balanced by the ratio a:b=1:6a:b=1:6. The proof is explicit; it is written in the language of Kontsevich graphs.Comment: Talk given by AVK on 26 July 2016 at the Algebra, Geometry and Physics seminar in the Max Planck Institute for Mathematics (Bonn, Germany). 29 pages, 16 figure

    Two-particle decays of B_c meson into charmonium states

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    The factorization of hard and soft contributions into the hadronic decays of B_c meson at large recoils is explored in order to evaluate the decay rates into the S, P and D-wave charmonia associated with rho and pi. The constraints of approach applicability and uncertainties of numerical estimates are discussed. The mode with the J/psi in the final state is evaluated taking into account the cascade radiative electromagnetic decays of excited P-wave states, that enlarges the branching ratio by 20-25%.Comment: 13 pages, LaTeX axodraw-style, 1 figure, 2 table

    Phonon-assisted and magnetic field induced Kondo tunneling in single molecular devices

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    We consider the Kondo tunneling induced by multiphonon emission/absorption processes in magnetic molecular complexes with low-energy singlet-triplet spin gap and show that the number of assisting phonons may be changed by varying the Zeeman splitting of excited triplet state. As a result, the structure of multiphonon Kondo resonances may be scanned by means of magnetic field tuning.Comment: 7 pages, 6 figures. Shortened version of this paper will be published in the Proceedings of the International Conference "Phonons2007" (J. Phys: Conf. Series

    Universal Cocycles and the Graph Complex Action on Homogeneous Poisson Brackets by Diffeomorphisms

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    Abstract: The graph complex acts on the spaces of Poisson bi-vectors P by infinitesimal symmetries. We prove that whenever a Poisson structure is homogeneous, i.e. P = LV(3) w.r.t. the Lie derivative along some vector field (Formula presented.)., but not quadratic (the coefficients of P are not degree-two homogeneous polynomials), and whenever its velocity bi-vector (Formula presented.)., also homogeneous w.r.t. (Formula presented.). whenever (Formula presented.). is obtained using the orientation morphism (Formula presented.). from a graph cocycle (Formula presented.). vertices and 2n - 2 edges, then the (Formula presented.). is a Poisson cocycle. Its construction is uniform for all Poisson bi-vectors (Formula presented.). satisfying the above assumptions, on all finite-dimensional affine manifolds M. Still, if the bi-vector (Formula presented.). is exact in the respective Poisson cohomology, so there exists a vector field (Formula presented.). such that (Formula presented.)., then the universal cocycle (Formula presented.). does not belong to the coset of (Formula presented.). We illustrate the construction using two examples of cubic-coefficient Poisson brackets associated with the R-matrices for the Lie algebra (Formula presented.).</p

    Particle decay in false vacuum

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    We revisit the problem of decay of a metastable vacuum induced by the presence of a particle. For the bosons of the `master field' the problem is solved in any number of dimensions in terms of the spontaneous decay rate of the false vacuum, while for a fermion we find a closed expression for the decay rate in (1+1) dimensions. It is shown that in the (1+1) dimensional case an infrared problem of one-loop correction to the decay rate of a boson is resolved due to a cancellation between soft modes of the field. We also find the boson decay rate in the `sine-Gordon staircase' model in the limits of strong and weak coupling.Comment: 19 pages, 2 figure

    A Study of a Mini-drift GEM Tracking Detector

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    A GEM tracking detector with an extended drift region has been studied as part of an effort to develop new tracking detectors for future experiments at RHIC and for the Electron Ion Collider that is being planned for BNL or JLAB. The detector consists of a triple GEM stack with a small drift region that was operated in a mini TPC type configuration. Both the position and arrival time of the charge deposited in the drift region were measured on the readout plane which allowed the reconstruction of a short vector for the track traversing the chamber. The resulting position and angle information from the vector could then be used to improve the position resolution of the detector for larger angle tracks, which deteriorates rapidly with increasing angle for conventional GEM tracking detectors using only charge centroid information. Two types of readout planes were studied. One was a COMPASS style readout plane with 400 micron pitch XY strips and the other consisted of 2x10mm2 chevron pads. The detector was studied in test beams at Fermilab and CERN, along with additional measurements in the lab, in order to determine its position and angular resolution for incident track angles up to 45 degrees. Several algorithms were studied for reconstructing the vector using the position and timing information in order to optimize the position and angular resolution of the detector for the different readout planes. Applications for large angle tracking detectors at RHIC and EIC are also discussed.Comment: Submitted to the IEEE Transactions on Nuclear Scienc
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