1,050 research outputs found

    Condensation of Excitons in Cu2O at Ultracold Temperatures: Experiment and Theory

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    We present experiments on the luminescence of excitons confined in a potential trap at milli-Kelvin bath temperatures under cw-excitation. They reveal several distinct features like a kink in the dependence of the total integrated luminescence intensity on excitation laser power and a bimodal distribution of the spatially resolved luminescence. Furthermore, we discuss the present state of the theoretical description of Bose-Einstein condensation of excitons with respect to signatures of a condensate in the luminescence. The comparison of the experimental data with theoretical results with respect to the spatially resolved as well as the integrated luminescence intensity shows the necessity of taking into account a Bose-Einstein condensed excitonic phase in order to understand the behaviour of the trapped excitons.Comment: 41 pages, 23 figure

    D-Branes on ALE Spaces and the ADE Classification of Conformal Field Theories

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    The spectrum of D2-branes wrapped on an ALE space of general ADE type is determined, by representing them as boundary states of N=2 superconformal minimal models. The stable quantum states have RR charges which precisely represent the gauge fields of the corresponding Lie algebra. This provides a simple and direct physical link between the ADE classification of N=2 superconformal field theories, and the corresponding root systems. An affine extension of this structure is also considered, whose boundary states represent the D2-branes plus additional D0-branes.Comment: 12p, harvmac, minor corrrections and ref adde

    Holonomy from wrapped branes

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    Compactifications of M-theory on manifolds with reduced holonomy arise as the local eleven-dimensional description of D6-branes wrapped on supersymmetric cycles in manifolds of lower dimension with a different holonomy group. Whenever the isometry group SU(2) is present, eight-dimensional gauged supergravity is a natural arena for such investigations. In this paper we use this approach and review the eleven dimensional description of D6-branes wrapped on coassociative 4-cycles, on deformed 3-cycles inside Calabi-Yau threefolds and on Kahler 4-cycles.Comment: 1+8 pages, Latex. Proceedings of the Leuven workshop, 2002. v2: Corrected typos in equations (4)-(8

    First Dark Matter Search Results from a Surface Run of the 10-L DMTPC Directional Dark Matter Detector

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    The Dark Matter Time Projection Chamber (DMTPC) is a low pressure (75 Torr CF4) 10 liter detector capable of measuring the vector direction of nuclear recoils with the goal of directional dark matter detection. In this paper we present the first dark matter limit from DMTPC. In an analysis window of 80-200 keV recoil energy, based on a 35.7 g-day exposure, we set a 90% C.L. upper limit on the spin-dependent WIMP-proton cross section of 2.0 x 10^{-33} cm^{2} for 115 GeV/c^2 dark matter particle mass.Comment: accepted for publication in Physics Letters

    Coset Construction of Spin(7),G2Spin(7), G_2 Gravitational Instantons

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    We study Ricci-flat metrics on non-compact manifolds with the exceptional holonomy Spin(7),G2Spin(7), G_2. We concentrate on the metrics which are defined on RĂ—G/H{\bf R} \times G/H. If the homogeneous coset spaces G/HG/H have weak G2G_2, SU(3) holonomy, the manifold RĂ—G/H{\bf R} \times G/H may have Spin(7),G2Spin(7), G_2 holonomy metrics. Using the formulation with vector fields, we investigate the metrics with Spin(7)Spin(7) holonomy on RĂ—Sp(2)/Sp(1),RĂ—SU(3)/U(1){\bf R}\times Sp(2)/Sp(1), {\bf R}\times SU(3)/U(1). We have found the explicit volume-preserving vector fields on these manifold using the elementary coordinate parameterization. This construction is essentially dual to solving the generalized self-duality condition for spin connections. We present most general differential equations for each coset. Then, we develop the similar formulation in order to calculate metrics with G2G_2 holonomyComment: 29 pages, no figure; (v2) Errors are corrected ; (v3) Some explanations are added. More general differential equations for SU(3)/U(1) coset are give
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