3,779 research outputs found

    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

    Phase operators, phase states and vector phase states for SU(3) and SU(2,1)

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    This paper focuses on phase operators, phase states and vector phase states for the sl(3) Lie algebra. We introduce a one-parameter generalized oscillator algebra A(k,2) which provides a unified scheme for dealing with su(3) (for k < 0), su(2,1) (for k > 0) and h(4) x h(4) (for k = 0) symmetries. Finite- and infinite-dimensional representations of A(k,2) are constructed for k < 0 and k > 0 or = 0, respectively. Phase operators associated with A(k,2) are defined and temporally stable phase states (as well as vector phase states) are constructed as eigenstates of these operators. Finally, we discuss a relation between quantized phase states and a quadratic discrete Fourier transform and show how to use these states for constructing mutually unbiased bases
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