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971.
The reaction of W6Br12, NaBr, and WO2Br2 in the presence of Br2 in a sealed silica tube yields Na[W2O2Br6] together with WOBr4 and WO2Br2 in the low temperature zone (temperature gradient 1030/870 K). Na[W2O2Br6] crystallizes orthorhombically in the space group Immm (no. 71) with a = 3.775 Å, b = 10.400 Å, c = 13.005 Å and Z = 2. Pairs of condensed trans-[WO2Br4] octahedra with a common Br2 edge form along [100] double chains [W2O4/2Br6]1– via the oxygen atoms. The mixed valent tungsten atoms are bonded to W2 pairs with a 2 c–3 e bond (d(W–W) = 2.946 Å, d(W–O) = 1.888 Å, d(W–Brb) = 2.537 Å, d(W–Brt) = 2.535 Å, ∢O–W–O = 177.4°, ∢Brb–W–Brb (endocyclic) = 109.0°). The Na+ cations connect the anionic double chains to form two-dimensional layers parallel (001), which interact by van der Waals forces. The cations are eightfold coordinated by a cube of the terminal Brt ligands of the polymeric anions (d(Na–Br) = 3.138 Å). Na[W2O2Br6] may be discussed as an intercalation compound of the oxide bromide WOBr3. 相似文献
972.
[(Cp*Fe)3{(η3-As3)Fe}As6] and [(Cp*Fe)3As6][FeCl3(THF)], Two New Ironarsenide Cluster Containing As6 and As3 Fragments The compounds [(Cp*Fe)3{(η3-As3)Fe}As6] ( 1 ) and [(Cp*Fe)3As6][FeCl3(THF)], ( 2 ) can be obtained in good yields through the reaction of As7(SiMe3)3 with FeCl2 and LiCp*. Both compounds have been characterized by mass spectroscopy and crystal structure analysis. The As7 nortricyclane frame of As7(SiMe3)3 is still recognizable in 1 . According to the Wade rules the cation of 2 has 20 valence electrons inside the clustercore. This leads to a structure very similar to closo-B9H92–. 相似文献
973.
Horst M. Sulzbach George Vacek Peter R. Schreiner John Morrison Galbraith Paul von R. Schleyer Henry F. Schaefer 《Journal of computational chemistry》1997,18(1):126-138
The five energetically lowest minima on the potential energy surface of N-acetyl-N′-methylalaninamide were optimized at the Becke3LYP/DZd level of theory to compare these density functional theory results with the literature findings at restricted Hartree-Fock/3-21G. While the relative energies are very similar, the amide moiety is predicted to be much more flexible at Becke3LYP/DZd. As a consequence, the three minima that favor a nonplanar amide group differ by up to 14° in their ϕ and ψ values between the two levels. To compare the change in the density functional NMR chemical shifts with respect to ϕ and ψ with experimental results, Becke3LYP/DZd was employed to optimize a structure for N-acetyl-N′-methylalaninamide at each 30° interval on the (ϕ, ψ) surface in the regions that correspond to the α helix and the β-pleated sheet and at each 60° interval elsewhere. The corresponding NMR chemical shielding surface was computed with the density functional program deMon. The resultant NMR chemical shielding surfaces for N and Cβ are in good agreement with the experiment, while the change in the NMR chemical shielding of C′ and Cα cannot be described only in terms of ϕ and ψ. The chemical shifts for those atoms also depend on the nonplanarity of the amide moiety. We evaluated this dependence for N-methylacetamide as a model system. Estimates of the parameters derived from N-methyl-acetamide allowed the NMR-shielding surfaces of C′ and Cα to be corrected for the nonplanar nitrogen influence. Although the effect is less pronounced with lower level theoretical geometries, due to the smaller degree of pyramidalization of the amide nitrogen, the (ϕ, ψ) NMR chemical shielding surfaces will need to be corrected. The agreement with the experiment was much better for the corrected surface of C′ when the nitrogen in the α helix had a nonplanar environment. © 1997 by John Wiley & Sons, Inc. 相似文献
974.
The reaction of AlCl3 with Li2PR (R = SiiPr3, SiMeiPr2) in a mixture of heptane and ether yields in the polycyclic compounds [(AlCl)4(μ3‐PR)2(μ‐PR)2(Et2O)2]( 1a : R = SiiPr3; 1b : SiMeiPr2) with a ladder‐shaped Al4P4 core. The coordination sphere of the outer aluminium atoms in these compounds is completed by ether ligands. In contrast, the reaction of AlCl3 with Li2PSiiPr3 in pure heptane yields in the formation of the hexagonal prismatic compound [(AlCl)6(μ3‐PSiiPr3)6]( 2 ). 1 and 2 were characterized by single crystal X‐ray diffraction analysis as well as by 31P{1H} and 27Al NMR spectroscopy. The structure determining effect of the solvent can be rationalized by quantumchemical calculations, which also show that the hexagonal prismatic structure is the most stable of the investigated oligomers in absence of ether. 相似文献
975.
The compounds [(Me3SiO)8Te2O2] ( 1 ) and [(Me4Si2O2)3Te] ( 2 ) have been prepared in good yields through Bronsted acid‐base reaction of Te(OH)6 with Me3SiNEt2 and Me4Si2(NEt2)2, respectively. They have been characterised by multinuclear NMR spectroscopy and single crystal X‐ray diffraction analyses. The formation of dinuclear 1 is the result of fast intermolecular condensation of two partially silylated orthotelluric acid units during the esterification process. Its structure consists of two edge‐fused TeO6‐octahedra, bearing a four‐membered Te2O2 ring as central motif. In contrast, the main structural feature of chiral 2 is a TeO6 octahedron which is fully silylated by three bidentate 1,1,2,2‐tetramethyldisilanediyl units, resulting in a racemic mixture. The metastability of 2 is remarkable since the Te(+ 6) center usually acts as a strong oxidation reagent toward the Si–Si bond in disilanes. 1 and 2 represent potential starting compounds for molecular TexOy aggregates as hybrid components for new glasses by sol‐gel procedure. 相似文献
976.
Gunther Mair Hans Georg von Schnering Michael Wrle Reinhard Nesper 《无机化学与普通化学杂志》1999,625(7):1207-1211
Li2B6 is formed from the elements as transparent red microcrystalline compound (Li : B = 1 : 3; Mo crucible in closed Nb ampoule; 1723 K; 4 h). Single crystals are grown from a lithium silicide melt with large Li excess at 1923 K. Li2B6 is a semiconductor with electron as well as Li+ ionic conductivity which dominates above 600 K. Microcrystalline samples react with H2O liberating gases and forming a brownish amorphous product, but larger crystals are not very sensitive. – Li2B6 crystallizes tetragonally in a new tP16 structure type which is a variant of the CaB6 structure (a = 5.975 Å, c = 4.189 Å; Z = 2; space group P4/mbm). The [B62–] net of the polymeric octahedro-anion is slightly distorted to give space for the insertion of a (32434) net of the Li+ cations in the cavities (d(B–B)endo = 1.766 Å; d(B–B)exo = 1.720 Å; d(Li–B) = 2.363 Å; d(Li–Li) = 3.094 Å). The incomplete occupancy of the Li position (80%) and the electron density at a further position (20%) indicate the mobility of the Li+ cations. 相似文献
977.
Inspection games in arms control 总被引:1,自引:0,他引:1
Rudolf Avenhaus Morton Canty D. Marc Kilgour Bernhard von Stengel Shmuel Zamir 《European Journal of Operational Research》1996,90(3):383
An inspection game is a mathematical model of a situation in which an inspector verifies the adherence of an inspectee to some legal obligation, such as an arms control treaty, where the inspectee may have an interest in violating that obligation. The mathematical analysis seeks to determine an optimal inspection scheme, ideally one which will induce legal behavior, under the assumption that the potential illegal action is carried out strategically; thus a non-cooperative game with two players, inspector and inspectee, is defined. Three phases of development in the application of such models to arms control and disarmament may be identified. In the first of these, roughly from 1961 through 1968, studies that focused on inspecting a nuclear test ban treaty emphasized game theory, with less consideration given to statistical aspects associated with data acquisition and measurement uncertainty. The second phase, from 1968 to about 1985, involves work stimulated by the Treaty on the Non-Proliferation of Nuclear Weapons (NPT). Here, the verification principle of material accountancy came to the fore, along with the need to include the formalism of statistical decision theory within the inspection models. The third phase, 1985 to the present, has been dominated by challenges posed by such far-reaching verification agreements as the Intermediate Range Nuclear Forces Agreement (INF), the Treaty on Conventional Forces in Europe (CFE) and the Chemical Weapons Convention (CWC), as well as perceived failures of the NPT system in Iraq and North Korea. In this connection, the interface between the political and technical aspects of verification is being examined from the game-theoretic viewpoint. 相似文献
978.
979.
M. Vogel G. Birkl M. S. Ebrahimi D. von Lindenfels A. Martin G. G. Paulus W. Quint S. Ringleb Th. Stöhlker M. Wiesel 《Hyperfine Interactions》2015,230(1-3):65-71
We present two Penning trap experiments concerned with different aspects of the physics of extreme electromagnetic fields, the ARTEMIS experiment designed for bound-electron magnetic moment measurements in the presence of the extremely strong fields close to the nucleus of highly charged ions, and the HILITE experiment, in which well-defined ion targets are to be subjected to high-intensity laser fields. 相似文献
980.
This paper assesses the potential of the average gray-level (AVGL) from ultrasonographic (B-mode) images to estimate temperature changes in time and space in a non-invasive way. 相似文献