2,049 research outputs found

    Whalesong

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    Vice chancellor speaks out: Beeton reviews year at university -- APEA employees nearly walk out -- Opinion -- Physical education facility planned for area near UAJ student housing -- Campus update -- Chess club holds tourneys -- Classified -- Arts -- The sports page: Ostling overall ski champ at Alyeska Ski Area -- Student government....: News and views from the United Students of UAJ -- F.Y.I. -- Suicide: a crisis of emotion -- Tel-med a free service for student

    An electron microscopic study of gas condensates in the system Mg-Si-O-H

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    Condensates of MgSiO_3 and SiO_2 from a gas formed by evaporation of enstatite at an H_2 pressure of 4.4×10^ bar and a temperature of 1525℃ by B. O. MYSEN and I. KUSHIRO (Am. Mineral. (in press), 1988) and I. KUSHIRO and B. O. MYSEN (Advances in Physical Geochemistry, New York, Springer (in press), 1988) were investigated with an analytical transmission electron microscope (ATEM), a scanning electron microscope (SEM) and an electron probe microanalyzer (EPMA). With decreasing temperature at an approximately constant total pressure the Mg/(Mg+Si) atomic ratio of the condensate (mixture of MgSiO_3 and SiO_2 polymorphs) decreases first, then increases, and finally reaches a constant value. This compositional change of the condensate is inconsistent with the equilibrium condensation model. The TEM studies suggest that metastable condensation of coesite and probably of protoenstatite and cristobalite took place. Coesite probably condensed by heterogeneous nucleation on protoenstatite. Fibrous quartz was also formed by heterogeneous nucleation on molybdenum fibers which condensed from a molybdenum vapor by a partial evaporation of a Knudsen cell used in the experiment. Heterogeneous nucleation might have played an important role in condensation process in the solar nebula. The texture of the experimental clinopyroxene condensate is different from that in interplanetary dust particles (J. P. BRADLEY et al., Nature, 301,473,1983)

    Unusual Low-Temperature Phase in VO2_2 Nanoparticles

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    We present a systematic investigation of the crystal and electronic structure and the magnetic properties above and below the metal-insulator transition of ball-milled VO2_2 nanoparticles and VO2_2 microparticles. For this research, we performed a Rietveld analysis of synchrotron radiation x-ray diffraction data, O KK x-ray absorption spectroscopy, V L3L_3 resonant inelastic x-ray scattering, and magnetic susceptibility measurements. This study reveals an unusual low-temperature phase that involves the formation of an elongated and less-tilted V-V pair, a narrowed energy gap, and an induced paramagnetic contribution from the nanoparticles. We show that the change in the crystal structure is consistent with the change in the electronic states around the Fermi level, which leads us to suggest that the Peierls mechanism contributes to the energy splitting of the a1ga_{1g} state. Furthermore, we find that the high-temperature rutile structure of the nanoparticles is almost identical to that of the microparticles.Comment: 7 pages, 8 figures, 2 table

    Prolongation on regular infinitesimal flag manifolds

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    Many interesting geometric structures can be described as regular infinitesimal flag structures, which occur as the underlying structures of parabolic geometries. Among these structures we have for instance conformal structures, contact structures, certain types of generic distributions and partially integrable almost CR-structures of hypersurface type. The aim of this article is to develop for a large class of (semi-)linear overdetermined systems of partial differential equations on regular infinitesimal flag manifolds MM a conceptual method to rewrite these systems as systems of the form ∇~(Σ)+C(Σ)=0\tilde\nabla(\Sigma)+C(\Sigma)=0, where ∇~\tilde\nabla is a linear connection on some vector bundle VV over MM and C:V→T∗M⊗VC: V\rightarrow T^*M\otimes V is a (vector) bundle map. In particular, if the overdetermined system is linear, ∇~+C\tilde\nabla+C will be a linear connection on VV and hence the dimension of its solution space is bounded by the rank of VV. We will see that the rank of VV can be easily computed using representation theory.Comment: 35 pages; typos corrected and minor changes, final version to appear in International Journal of Mathematic
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