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Structure of a binuclear copper(II) complex with both μ-alkoxo and μ-formato bridges, [Cu2(C17H15N2O3)(HCOO)]

T. Kawata、Shigeru Ohba、Yoshihiro Nishida 等 4 位作者1993-12-15Acta Crystallographica Section C Crystal Structure Communications

The crystal structure of a binuclear copper(II) complex, μ-formato-1kO:2kO'-μ-2,2'-[1,3-(2-hydroxypropanediyl-1:2k 2 O)bis(nitrilomethylidyne)]diphenolato(3-)-1k 3 N,O:2k 2 N',O'-dicopper(II), [Cu 2 (L-sal)(HCOO)], H 3 (L-sal)=N,N'-bis(salicylidene)1,3-diamino-2-propanol, was determined by X-ray diffraction. The title…

Metal-Organic Frameworks: Synthesis and ApplicationsMetal complexes synthesis and propertiesMagnetism in coordination complexes

A lower bound on the loss of graphite by atomic oxygen attack at asymptotic energy

Lior Cohen1993-12-15The Journal of Chemical Physics

A method is devised to find a lower bound on the loss function of graphite in the oxygen high energy range where that function is expected to assume constant value. It requires obtaining a small ensemble of classical trajectories of oxygen on graphite and making static measurements of an oxygen on ethylene potential e…

Graphene research and applicationsElectron and X-Ray Spectroscopy TechniquesChemical and Physical Properties of Materials

Electronic band structure and bonding in Nb 3 O 3

Werner Schulz、Renata M. Wentzcovitch1993-12-15Physical review. B, Condensed matter

The local-density approximation is used to investigate the electronic and structural properties of ${\mathrm{Nb}}_{3}$${\mathrm{O}}_{3}$ and the reasons for its unusual defect rocksalt structure with 25% ordered vacancies. A tight-binding Hamiltonian is fitted to the energy bands which are compared to those of the hyp…

Semiconductor materials and devicesInorganic Chemistry and MaterialsElectronic and Structural Properties of Oxides

Argon incorporation in Si(100) by ion bombardment at 15–100 eV

W. M. Lau、I. Bello、L. J. Huang 等 6 位作者1993-12-15Journal of Applied Physics

Argon incorporation in Si(100) by low energy ion bombardment has been studied by polar angle dependent x-ray photoelectron spectroscopy and Rutherford backscattering spectroscopy. The bombardment was performed at 15, 20, and 100 eV in an ultrahigh vacuum chamber where a mass-separated argon ion beam with an energy spr…

Electron and X-Ray Spectroscopy TechniquesIon-surface interactions and analysisIntegrated Circuits and Semiconductor Failure Analysis

First-principles calculations of the structural properties, stability, and band structure of complex tetrahedral phases of germanium: ST12 and BC8

A. Mújica、R. J. Needs1993-12-15Physical review. B, Condensed matter

We report the results of a first-principles study of the structural properties, stability, and band structure of Ge in two complex tetrahedral phases: the ST12 phase (simple tetragonal with 12 atoms per unit cell) and the BC8 phase (body-centered cubic with 8 atoms per cell). We focus mainly on the ST12 phase, which i…

Metal and Thin Film MechanicsHigh-pressure geophysics and materialsBoron and Carbon Nanomaterials Research

Therapy of human ovarian carcinoma xenografts using doxorubicin encapsulated in sterically stabilized liposomes

Jan Vaage、Dorothy Donovan、E. Mayhew 等 5 位作者1993-12-15Cancer

BACKGROUND: This study compared the therapeutic effects of doxorubicin hydrochloride in saline and in sterically stabilized, long-circulating liposomes composed of hydrogenated soy phosphatidylcholine/cholesterol/polyethylene glycol-distearoyl-phosphatidyl-ethanolamine (Doxil). METHODS: The drug formulations were inje…

Nanoparticle-Based Drug DeliveryLipid Membrane Structure and BehaviorRNA Interference and Gene Delivery

Formation of microporous polymer fibers and oriented fibrils by precipitation with a compressed fluid antisolvent

David J. Dixon、Keith P. Johnston1993-12-15Journal of Applied Polymer Science

Abstract Polymer morphology is controlled over a continuum from microspheres to interconnected bicontinuous networks to fibers with a versatile new process: precipitation with a compressed fluid antisolvent. The results are explained qualitatively as a function of phase behavior, mass‐transfer pathways, and the format…

Pickering emulsions and particle stabilizationPolymer Foaming and Composites

Calculated quasiparticle band gap of β-C3N4

Jennifer L. Corkill、Marvin L. Cohen1993-12-15Physical review. B, Condensed matter

The quasiparticle electronic band structure of ${\mathrm{C}}_{3}$${\mathrm{N}}_{4}$ carbon nitride in the \ensuremath{\beta}-${\mathrm{Si}}_{3}$${\mathrm{N}}_{4}$ structure is calculated using the GW approximation. The indirect band gap is predicted to be 6.4\ifmmode\pm\else\textpm\fi{}0.5 eV and the minimum direct ga…

Metal and Thin Film MechanicsSemiconductor materials and devicesDiamond and Carbon-based Materials Research

High-resolution electron-energy-loss spectroscopic study of epitaxially grown diamond (111) and (100) surfaces

T. Aizawa、Toshihiro Ando、Mutsukazu Kamo 等 4 位作者1993-12-15Physical review. B, Condensed matter

Diamond (111) and (100) surfaces have been investigated by low-energy electron diffraction and high-resolution electron-energy-loss spectroscopy (HREELS). Samples were boron-doped semiconducting diamond surfaces grown homoepitaxially on natural diamond by microwave-plasma-assisted chemical-vapor deposition. A dipole-a…

Advanced Chemical Physics StudiesDiamond and Carbon-based Materials ResearchAdvanced Electron Microscopy Techniques and Applications

Redetermination of the β-Ca2P2O7 structure

S. Boudin、A. Grandin、M.M. Borel 等 5 位作者1993-12-15Acta Crystallographica Section C Crystal Structure Communications

β Dicalcium diphosphate is composed of eclipsed P 2 O 7 groups linked through Ca 2+ cations. The P-Ob bonds involving the bridging O atoms arelonger [average 1.620 (5) A] than the others [average 1.517 (5) A]. As the «O 4 » tetrahedra are almost regular the displacement of the P atoms involves two sets of O-P-O angles…

Crystal Structures and PropertiesChemical Synthesis and CharacterizationX-ray Diffraction in Crystallography

Determination of cubic-tetragonal phase boundary in Zr1−XYXO2−X/2 solid solutions by Raman spectroscopy

Masatomo Yashima、Katsuya Ohtake、H. Arashi 等 5 位作者1993-12-15Journal of Applied Physics

Raman spectroscopy is found to be a powerful tool to determine the structural phase boundary between cubic (Fm3m) and tetragonal (P42/nmc) phase in arc-melted Zr1−XYXO2−X/2 (0.08≤X≤0.24) solid solution. The Raman peak intensity characteristic of the tetragonal phase at about 470 cm−1 decreases with the YO1.5 content X…

Advanced ceramic materials synthesisSemiconductor materials and devicesNuclear materials and radiation effects

Effects of particle shape and size distributions on the electrical and magnetic properties of nickel/polyethylene composites

Halit S. Göktürk、Thomas J. Fiske、Dilhan M. Kalyon1993-12-15Journal of Applied Polymer Science

Abstract Electrical and magnetic properties of composite materials prepared by incorporating various nickel‐based fillers of different shapes into polyethylene were investigated. The fillers used were nickel powders, nickel filamentary powders, nickel flakes, and nickel‐coated graphite fibers. The particle‐size distri…

Natural Fiber Reinforced CompositesElectromagnetic wave absorption materialsFiber-reinforced polymer composites

Spall strength of molybdenum single crystals

G. I. Kanel、С. В. Разоренов、A. V. Utkin 等 8 位作者1993-12-15Journal of Applied Physics

Spall strength measurements for commerical grade molybdenum and molybdenum single crystals were made in a wide range of load durations (∼10−9 s – 10−6 s) and intensities (∼5 – 100 GPa). Resistance to fracture of pure single crystals was found to exceed two times the spall strength of polycrystalline molybdenum and to…

Metal and Thin Film MechanicsEnergetic Materials and CombustionHigh-Velocity Impact and Material Behavior

Structure of the laser host material LiYF4

E. Garcia、R. R. Ryan1993-12-15Acta Crystallographica Section C Crystal Structure Communications

Lithium yttrium tetrafluoride, LiYF 4 , M r =171.8, tetragonal, I4 4 /a, a=5.164 (1), c=10.741 (2) A, V=286.5 (1) A 3 , Z=4, D x = 3.99 g cm -3 , λ(Mo Kα)=0.7107 A, μ=204 cm -1 , F(000)=312, T=295 K, R=0.015 for 156 unique observed [F>4σ(F)] reflections. The scheelite (CaWO 4 ) structure is confirmed. Lithium is locat…

Luminescence Properties of Advanced MaterialsCrystal Structures and PropertiesInorganic Fluorides and Related Compounds

Transport in polyaniline near the critical regime of the metal-insulator transition

Reghu Menon、C.O. Yoon、D. Moses 等 5 位作者1993-12-15Physical review. B, Condensed matter

Critical behavior of the electrical conductivity near the disorder-induced metal-insulator (MI) transition has been observed in polyaniline (PANI) doped with camphor sulfonic acid (CSA). The temperature dependence of the resistivity (\ensuremath{\rho}) depends on the degree of disorder present in the PANI-CSA films. I…

Organic Electronics and PhotovoltaicsAdvanced Sensor and Energy Harvesting MaterialsConducting polymers and applications

Stretched-exponential decay of the luminescence in porous silicon

Lorenzo Pavesi、Matteo Ceschini1993-12-15Physical review. B, Condensed matter

An experimental study of the luminescence time decay in porous silicon as a function of temperature, excitation, and observation energies is reported. The decay line shape is well described by a stretched exponential for a variety of experimental conditions. A hierarchy of waiting times for carrier hopping, of intersi…

Semiconductor materials and devicesSilicon Nanostructures and PhotoluminescenceNanowire Synthesis and Applications

Nitrogen doping of highly tetrahedral amorphous carbon

V.S. Veerasamy、Jun Yuan、G.A.J. Amaratunga 等 7 位作者1993-12-15Physical review. B, Condensed matter

Successful control of the conductivity of tetrahedrally bonded amorphous carbon (ta-C) by incorporation of N during film growth is reported. N is introduced into the films during growth by injecting ${\mathrm{N}}_{2}$ gas into a plasma stream formed by a carbon cathodic vacuum arc. X-ray-photoemission-spectroscopy stu…

Metal and Thin Film MechanicsSemiconductor materials and devicesDiamond and Carbon-based Materials Research

Structure of siloxene and layered polysilane ( Si 6 H 6 )

J. R. Dahn、B. M. Way、E FULLER 等 4 位作者1993-12-15Physical review. B, Condensed matter

Powder-x-ray-diffraction measurements on siloxene and calculations of the diffraction patterns for the three commonly proposed structures of siloxene (${\mathrm{Si}}_{6}$${\mathrm{H}}_{6}$${\mathrm{O}}_{3}$) clearly show that only a structure with silicon layers is ever observed. The formation of siloxene from ${\math…

Luminescence Properties of Advanced MaterialsAdvanced ceramic materials synthesisSilicon Nanostructures and Photoluminescence

Electronic effects in scanning tunneling microscopy: Moiré pattern on a graphite surface

Zhao Rong、P. J. C. Kuiper1993-12-15Physical review. B, Condensed matter

We observed by scanning tunneling microscopy (STM) a hexagonal superlattice on graphite with a period of 66 \AA{}. Direct measurement of the angle between lattice vectors confirmed that the superlattice is a Moir\'e pattern caused by a 2.1\ifmmode^\circ\else\textdegree\fi{} rotation of the topmost (0001) plane with re…

Graphene research and applicationsQuantum and electron transport phenomenaSurface and Thin Film Phenomena

Variation of optical gaps in perovskite-type 3dtransition-metal oxides

T. Arima、Y. Tokura、J. B. Torrance1993-12-15OpenAlex

The optical study of trivalent 3d transition-metal-oxide compounds (RM${\mathrm{O}}_{3}$) with the perovskitelike structure has revealed the variation of their electronic structure with the 3d element (M) as well as the A-site rare-earth element (R). The crossover of the gap nature from the Mott type to charge-transfe…

Perovskite Materials and ApplicationsMagnetic and transport properties of perovskites and related materialsTransition Metal Oxide Nanomaterials