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L A Svensson 《Acta chemica Scandinavica》1972,26(7):2663-2669
365.
Stefan T. Norberg Göran Svensson Jörgen Albertsson 《Acta Crystallographica. Section C, Structural Chemistry》2001,57(3):225-227
A room-temperature structural model of titanium pyrophosphate, TiP2O7, has been determined from synchrotron X-ray data. The structure consists of TiO6 octahedra and PO4 tetrahedra sharing corners in a three-dimensional network. The PO4 tetrahedra form P2O7 groups connecting the TiO6 octahedra. The 3 × 3 × 3 superstructure differs substantially from the parent AB2O7 structure. The P—O—P bonding angles of the pyrophosphate group are between 141.21 (12) and 144.51 (13)° for those groups not located on the threefold axis. The individual TiO6 octahedra and PO4 tetrahedra are somewhat distorted. 相似文献
366.
O. Travnikova C. Miron M. Bssler R. Feifel M.N. Piancastelli S.L. Sorensen S. Svensson 《Journal of Electron Spectroscopy and Related Phenomena》2009,174(1-3):100
The present work aims at characterizing short-lived C1s(−1)π*(1) core-excited states of the OCS molecule based on the analysis of the vibrational fine structure and lineshape profiles of the high-resolution resonant Auger decay spectra recorded at the excitation energies along the C1s→π* resonance in the binding energy region 15–19 eV. Very different behavior in terms of lineshape and resonant enhancement is observed for the , and final states. This is explained by (1) the variation in the C–O bond lengths for the states involved in the electronic relaxation and (2) different contributions in terms of Mulliken population to the molecular orbitals determining the electronic character of the corresponding states. Since the final-state geometries are known from a number of previous experiments and ab initio calculations, the geometry of the C1s(−1)π*(1) intermediate states can be predicted in analogy with e.g. the N2, CO2 and N2O molecules. 相似文献
367.
N.M. Bulgakova A.V. Bulgakov J. Svensson E.E.B. Campbell 《Applied Physics A: Materials Science & Processing》2006,85(2):109-116
We consider the role of electric fields during metal-catalysed thermal chemical vapour deposition growth of carbon nanotubes and show that enhanced growth occurs from a negatively biased electrode. An electric field, applied externally to the growing tubes and/or generated as a result of electron emission or self-biasing, may strongly affect the carbon supply through the catalyst nanoparticle, enhancing the growth rate. Different aspects of the growth process are analysed: the nature of the nanoparticle catalysis, carbon dissolution kinetics, electron emission from the nanotube tips, charge transport in the nanotube–catalytic nanoparticle system and carbon drift and diffusion through the catalyst under the action of the electric field. A fundamental tenet for modelling of charge-transport dynamics during the nanotube growth process is proposed. PACS 81.07.De; 81.15.Gh 相似文献
368.
Electric field aligned, single-walled carbon nanotubes are grown between electrodes using thermal chemical vapour deposition (CVD) of methane. The growth occurs on a thin film layered catalyst of aluminium, iron and molybdenum patterned on top of electrodes. The nanotubes bridge 10 μm sized electrode gaps and have a typical diameter of less than 2 nm as measured by Raman spectroscopy and atomic force microscopy. We present electrical transport measurements on a directly grown nanotube which shows p-type semiconducting behaviour. 相似文献
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Bicyclic phenols of type 1 with annelated rings containing a N or an O heteroatom (X = N or O) as well as the ring opened analogs have been brominated and the product distribution determined. The results indicate that while most annelated rings have a directing effect to the ar-β position of the molecule, a 6-membered annelated ring is an exception and it facilitates substitution in the ar-α position. 相似文献