509 research outputs found

    Optical propagation measurements at Emerson Lake, 1968

    Get PDF
    Optical propagation measurements in inhomogeneous atmosphere at Emerson Lake, California for optical propagation theory validity testin

    Relation between Light Cone Distribution Amplitudes and Shape Function in B mesons

    Full text link
    The Bakamjian-Thomas relativistic quark model provides a Poincar\'e representation of bound states with a fixed number of constituents and, in the heavy quark limit, form factors of currents satisfy covariance and Isgur-Wise scaling. We compute the Light Cone Distribution Amplitudes of BB mesons ϕ±B(ω)\phi_{\pm}^B(\omega) as well as the Shape Function S(ω)S(\omega), that enters in the decay BXsγB \to X_s \gamma, that are also covariant in this class of models. The LCDA and the SF are related through the quark model wave function. The former satisfy, in the limit of vanishing constituent light quark mass, the integral relation given by QCD in the valence sector of Fock space. Using a gaussian wave function, the obtained S(ω)S(\omega) is identical to the so-called Roman Shape Function. From the parameters for the latter that fit the BXsγB \to X_s\gamma spectrum we predict the behaviour of ϕ±B(ω)\phi_{\pm}^B(\omega). We discuss the important role played by the constituent light quark mass. In particular, although ϕB(0)0\phi_-^B(0) \not= 0 for vanishing light quark mass, a non-vanishing mass implies the unfamiliar result ϕB(0)=0\phi_-^B (0) = 0. Moreover, we incorporate the short distance behaviour of QCD to ϕ+B(ω)\phi_+^B (\omega), which has sizeable effects at large ω\omega. We obtain the values for the parameters Λˉ0.35\bar{\Lambda} \cong 0.35 GeV and λB11.43\lambda_B^{-1} \cong 1.43 GeV1^{-1}. We compare with other theoretical approaches and illustrate the great variety of models found in the literature for the functions ϕ±B(ω)\phi_{\pm}^B (\omega); hence the necessity of imposing further constraints as in the present paper. We briefly review also the different phenomena that are sensitive to the LCDA.Comment: 6 figure

    Relativistic quantum theories and neutrino oscillations

    Full text link
    Neutrino oscillations are examined under the broad requirements of Poincar\'e-invariant scattering theory in an S-matrix formulation. This approach can be consistently applied to theories with either field or particle degrees of freedom. The goal of this paper is to use this general framework to identify all of the unique physical properties of this problem that lead to a simple oscillation formula. We discuss what is in principle observable, and how many factors that are important in principle end up being negligible in practice.Comment: 21 pages, no figure

    Axial-vector mesons in a relativistic point-form approach

    Full text link
    The Poincare invariant coupled-channel formalism for two-particle systems interacting via one-particle exchange, which has been developed and applied to vector mesons in Ref. [1] is applied to axial vector mesons. We thereby extend the previous study of a dynamical treatment of the Goldstone-boson exchange by comparison with the commonly used instantaneous approximation to the case of orbital angular momentum l=1. Effects in the mass shifts show more variations than for the vector-meson case. Results for the decay widths are sizable, but comparison with sparse experimental data is inconclusive.Comment: 4 pages, 1 figur

    Rotational covariance and light-front current matrix elements

    Full text link
    Light-front current matrix elements for elastic scattering from hadrons with spin~1 or greater must satisfy a nontrivial constraint associated with the requirement of rotational covariance for the current operator. Using a model ρ\rho meson as a prototype for hadronic quark models, this constraint and its implications are studied at both low and high momentum transfers. In the kinematic region appropriate for asymptotic QCD, helicity rules, together with the rotational covariance condition, yield an additional relation between the light-front current matrix elements.Comment: 16 pages, [no number

    The Balian-Br\'ezin Method in Relativistic Quantum Mechanics

    Full text link
    The method suggested by Balian and Br\'ezin for treating angular momentum reduction in the Faddeev equations is shown to be applicable to the relativistic three-body problem.Comment: 14 pages in LaTe

    Spatial distributions in static heavy-light mesons: a comparison of quark models with lattice QCD

    Full text link
    Lattice measurements of spatial distributions of the light quark bilinear densities in static mesons allow to test directly and in detail the wave functions of quark models. These distributions are gauge invariant quantities directly related to the spatial distribution of wave functions. We make a detailed comparison of the recent lattice QCD results with our own quark models, formulated previously for quite different purposes. We find a striking agreement not only between our two quark models, but also with the lattice QCD data for the ground state in an important range of distances up to about 4/GeV. Moreover the agreement extends to the L=1 states [j^P=(1/2)^+]. An explanation of several particular features completely at odds with the non-relativistic approximation is provided. A rather direct, somewhat unexpected and of course approximate relation between wave functions of certain quark models and QCD has been established.Comment: 40 pages, 5 figures (version published in PRD

    First Order Relativistic Three-Body Scattering

    Get PDF
    Relativistic Faddeev equations for three-body scattering at arbitrary energies are formulated in momentum space and in first order in the two-body transition-operator directly solved in terms of momentum vectors without employing a partial wave decomposition. Relativistic invariance is incorporated within the framework of Poincare invariant quantum mechanics, and presented in some detail. Based on a Malfliet-Tjon type interaction, observables for elastic and break-up scattering are calculated up to projectile energies of 1 GeV. The influence of kinematic and dynamic relativistic effects on those observables is systematically studied. Approximations to the two-body interaction embedded in the three-particle space are compared to the exact treatment.Comment: 26 pages, 13 figure

    Space-like and time-like pion electromagnetic form factor and Fock state components within the Light-Front dynamics

    Get PDF
    The simultaneous investigation of the pion electromagnetic form factor in the space- and time-like regions within a light-front model allows one to address the issue of non-valence components of the pion and photon wave functions. Our relativistic approach is based on a microscopic vector meson dominance (VMD) model for the dressed vertex where a photon decays in a quark-antiquark pair, and on a simple parametrization for the emission or absorption of a pion by a quark. The results show an excellent agreement in the space like region up to -10 (GeV/c)2(GeV/c)^2, while in time-like region the model produces reasonable results up to 10 (GeV/c)2(GeV/c)^2.Comment: 74 pages, 11 figures, use revtex

    Baryon Current Matrix Elements in a Light-Front Framework

    Full text link
    Current matrix elements and observables for electro- and photo-excitation of baryons from the nucleon are studied in a light-front framework. Relativistic effects are estimated by comparison to a nonrelativistic model, where we use simple basis states to represent the baryon wavefunctions. Sizeable relativistic effects are found for certain transitions, for example, to radial excitations such as that conventionally used to describe to the Roper resonance. A systematic study shows that the violation of rotational covariance of the baryon transition matrix elements stemming from the use of one-body currents is generally small.Comment: 32 pages, LaTeX, 10 postscript figures, uses epsf.sty; figures uuencoded with uufiles (or available by request in .ps or hardcopy form
    corecore