4,685 research outputs found

    Investigating the central diffractive f0(980) and f2(1270) meson production at the LHC

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    The central diffractive production of mesons f0(980) and f2(1270) at the energy of CERN-LHC experiment on proton-proton collisions is investigated. The processes initiated by quasi-real photon-photon collisions and by central diffraction processes are considered. The role played by the photon-Odderon production channel is also studied. The cross sections for these distinct production channels are compared and analyzed.Comment: 7 pages, 4 tables. Final version to be published in Physical Review D. arXiv admin note: text overlap with arXiv:hep-ph/0508196, arXiv:hep-ph/0506101 by other author

    Controlled Contact to a C60 Molecule

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    The conductance of C60 on Cu(100) is investigated with a low-temperature scanning tunneling microscope. At the transition from tunneling to the contact regime the conductance of C60 adsorbed with a pentagon-hexagon bond rises rapidly to 0.25 conductance quanta G0. An abrupt conductance jump to G0 is observed upon further decreasing the distance between the instrument's tip and the surface. Ab-initio calculations within density functional theory and non-equilibrium Green's function techniques explain the experimental data in terms of the conductance of an essentially undeformed C60. From a detailed analysis of the crossover from tunneling to contact we conclude that the conductance in this region is strongly affected by structural fluctuations which modulate the tip-molecule distance.Comment: 4 pages, 3 figure

    Controlling the Kondo Effect in CoCu_n Clusters Atom by Atom

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    Clusters containing a single magnetic impurity were investigated by scanning tunneling microscopy, spectroscopy, and ab initio electronic structure calculations. The Kondo temperature of a Co atom embedded in Cu clusters on Cu(111) exhibits a non-monotonic variation with the cluster size. Calculations model the experimental observations and demonstrate the importance of the local and anisotropic electronic structure for correlation effects in small clusters.Comment: 4 pages, 4 figure

    D'atri spaces of type k and related classes of geometries concerning jacobi operators

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    In this article we continue the study of the geometry of kk-D'Atri spaces, % 1\leq k n1\leq n-1 (nn denotes the dimension of the manifold),, began by the second author. It is known that kk-D'Atri spaces, k1,k\geq 1, are related to properties of Jacobi operators RvR_{v} along geodesics, since she has shown that trRv{\operatorname{tr}}R_{v}, trRv2{\operatorname{tr}}R_{v}^{2} are invariant under the geodesic flow for any unit tangent vector vv. Here, assuming that the Riemannian manifold is a D'Atri space, we prove in our main result that trRv3{\operatorname{tr}}R_{v}^{3} is also invariant under the geodesic flow if k3 k\geq 3. In addition, other properties of Jacobi operators related to the Ledger conditions are obtained and they are used to give applications to Iwasawa type spaces. In the class of D'Atri spaces of Iwasawa type, we show two different characterizations of the symmetric spaces of noncompact type: they are exactly the C\frak{C}-spaces and on the other hand they are kk -D'Atri spaces for some k3.k\geq 3. In the last case, they are kk-D'Atri for all k=1,...,n1k=1,...,n-1 as well. In particular, Damek-Ricci spaces that are kk-D'Atri for some k3k\geq 3 are symmetric. Finally, we characterize kk-D'Atri spaces for all k=1,...,n1k=1,...,n-1 as the SC% \frak{SC}-spaces (geodesic symmetries preserve the principal curvatures of small geodesic spheres). Moreover, applying this result in the case of 4% -dimensional homogeneous spaces we prove that the properties of being a D'Atri (1-D'Atri) space, or a 3-D'Atri space, are equivalent to the property of being a kk-D'Atri space for all k=1,2,3k=1,2,3.Comment: 19 pages. This paper substitute the previous one where one Theorem has been deleted and one section has been adde

    New limits on "odderon" amplitudes from analyticity constraints

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    In studies of high energy pppp and pˉp\bar pp scattering, the odd (under crossing) forward scattering amplitude accounts for the difference between the pppp and pˉp\bar pp cross sections. Typically, it is taken as f=p4πDsα1eiπ(1α)/2f_-=-\frac{p}{4\pi}Ds^{\alpha-1}e^{i\pi(1-\alpha)/2} (α0.5\alpha\sim 0.5), which has Δσ,Δρ0\Delta\sigma, \Delta\rho\to0 as ss\to\infty, where ρ\rho is the ratio of the real to the imaginary portion of the forward scattering amplitude. However, the odd-signatured amplitude can have in principle a strikingly different behavior, ranging from having Δσ\Delta\sigma\tonon-zero constant to having Δσlns/s0\Delta\sigma \to \ln s/s_0 as ss\to\infty, the maximal behavior allowed by analyticity and the Froissart bound. We reanalyze high energy pppp and pˉp\bar pp scattering data, using new analyticity constraints, in order to put new and precise limits on the magnitude of ``odderon'' amplitudes.Comment: 13 pages LaTex, 6 figure
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