5 research outputs found

    η−η′\eta-\eta^\prime mixing and the next-to-leading-order power correction

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    The next-to-leading-order O(1/Q4)O(1/Q^4) power correction for ηγ\eta\gamma and η′γ\eta^\prime\gamma form factors are evaluated and employed to explore the η−η′\eta-\eta^\prime mixing. The parameters of the two mixing angle scheme are extracted from the data for form factors, two photon decay widths and radiative J/ψJ/\psi decays. The χ2\chi^2 analysis gives the result: fη1=(1.16±0.06)fπ,fη8=(1.33±0.23)fπ,θ1=−9∘±3∘,θ8=−21.3∘±2.3∘f_{\eta_1}=(1.16\pm0.06)f_\pi, f_{\eta_8}=(1.33\pm0.23)f_\pi, \theta_1=-9^\circ\pm 3^\circ, \theta_8=-21.3^\circ\pm 2.3^\circ, where fη1(8)f_{\eta_{1(8)}} and θ1(8)\theta_{1(8)} are the decay constants and the mixing angles for the singlet (octet) state. In addition, we arrive at a stringent range for fη′c:−10f_{\eta^\prime}^c:-10 MeV≤fη′c≤−4\le f_{\eta^\prime}^c\le -4 MeV.Comment: 23 pages, 9 figures, To be publshied in Phys. Rev.

    Cosmological Backreaction from Perturbations

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    We reformulate the averaged Einstein equations in a form suitable for use with Newtonian gauge linear perturbation theory and track the size of the modifications to standard Robertson-Walker evolution on the largest scales as a function of redshift for both Einstein de-Sitter and Lambda CDM cosmologies. In both cases the effective energy density arising from linear perturbations is of the order of 10^-5 the matter density, as would be expected, with an effective equation of state w ~ -1/19. Employing a modified Halofit code to extend our results to quasilinear scales, we find that, while larger, the deviations from Robertson-Walker behaviour remain of the order of 10^-5.Comment: 15 pages, 8 figures; replaced by version accepted by JCA

    Jets and QCD: A Historical Review of the Discovery of the Quark and Gluon Jets and its Impact on QCD

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    The observation of quark and gluon jets has played a crucial role in establishing Quantum Chromodynamics [QCD] as the theory of the strong interactions within the Standard Model of particle physics. The jets, narrowly collimated bundles of hadrons, reflect configurations of quarks and gluons at short distances. Thus, by analysing energy and angular distributions of the jets experimentally, the properties of the basic constituents of matter and the strong forces acting between them can be explored. In this review, which is primarily a description of the discovery of the quark and gluon jets and the impact of their observation on Quantum Chromodynamics, we elaborate, in particular, the role of the gluons as the carriers of the strong force. Focusing on these basic points, jets in e+e− collisions will be in the foreground of the discussion and we will concentrate on the theory that was contemporary with the relevant experiments at the electron-positron colliders. In addition we will delineate the role of jets as tools for exploring other particle aspects in ep and \hbox{pp/ppˉpp/p\bar{p}} collisions  −  quark and gluon densities in protons, measurements of the QCD coupling, fundamental 2-2 quark/gluon scattering processes, but also the impact of jet decays of top quarks, and W ± , Z bosons on the electroweak sector. The presentation to a large extent is formulated in a non-technical language with the intent to recall the significant steps historically and convey the significance of this field also to communities beyond high energy physics
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