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31.
H.J. Breunig E. Lork C.I. Ra? R.P. Wagner 《Journal of organometallic chemistry》2007,692(16):3430-3434
Syntheses and crystal structures of [tBu3SbCr(CO)5] (1), [tBu3BiM(CO)5] [M = Cr (2), W (3)] and [tBu3BiMnCp′(CO)2] (4) (Cp′ = η5-C5H4CH3) are reported. 相似文献
32.
Syntheses and Crystal Structures of [μ‐(Me3SiCH2Sb)5–Sb1,Sb3–{W(CO)5}2] and [{(Me3Si)2CHSb}3Fe(CO)4] – Two Cyclic Complexes with Antimony Ligands cyclo‐(Me3SiCH2Sb)5 reacts with [(THF)W(CO)5] (THF = tetrahydrofuran) to form cyclo‐[μ‐(Me3SiCH2Sb)5–Sb1,Sb3–{W(CO)5}2] ( 1 ). The heterocycle cyclo‐ [{(Me3Si)2CHSb}3Fe(CO)4] ( 2 ) is formed by an insertion reaction of cyclo‐[(Me3Si)2CHSb]3 and [Fe2(CO)9]. The crystal structures of 1 and 2 are reported. 相似文献
33.
34.
Reactions of R4Sb2 (R = Me, Et) with (Me3SiCH2)3M (M = Ga, In) and Crystal Structures of [(Me3SiCH2)2InSbMe2]3 and [(Me3SiCH2)2GaOSbEt2]2 The reaction of (Me3SiCH2)3In with Me2SbSbMe2 gives [(Me3SiCH2)2InSbMe2]3 ( 1 ) and Me3SiCH2SbMe2. [(Me3SiCH2)2GaOSbEt2]2 ( 2 ) is formed by the reaction of (Me3SiCH2)3Ga with Et2SbSbEt2 and oxygen. The syntheses and the crystal structures of 1 and 2 are reported. 相似文献
35.
DmitriV. Sevenard OlegG. Khomutov KazimirI. Pashkevich Enno Lork Gerd‐Volker Rschenthaler 《Helvetica chimica acta》2002,85(7):1960-1972
The 2‐acylcycloalkanones 1a – g and 3a – c , possessing a polyfluoroalkyl group, react with hydroxylamine regio‐ and stereoselectively to yield 4,5‐dihydroisoxazol‐5‐ols 2a – g and 4a – c , respectively, i.e., products of N‐addition to the oxo group at the cycloalkane ring (Schemes 1 and 2). The products 2 and 4 can be dehydrated under drastic conditions only (Schemes 3 and 4). The structure of one of the 4,5‐dihydroisoxazol‐5‐ols was confirmed by X‐ray crystal‐structure analysis. 相似文献
36.
Tetracarbonyl Chromium Complexes with Me2SbESbMe2 (E = O, S) and MeSb(SSbMe2)2 as Ligands Me2SbOSbMe2 reacts with nbdCr(CO)4 (nbd = norbornadiene) to form cyclo-[Me2SbOSbMe2Cr(CO)4]2 ( 1 ). The reaction of Me2SbSSbMe2 with nbdCr(CO)4 gives cis-[(Me2SbSSbMe2)2Cr(CO)4] ( 2 ), a complex stable only in solution. With excess nbdCr(CO)4 also cyclo[Me2SbSSbMe2Cr(CO)4]2 ( 3 ) and cyclo[MeSb(SSbMe2)2Cr(CO)4] ( 4 ) form in low yield. The crystal structures of 1 , 3 and 4 · nbdCr(CO)4 are reported. The novel ligand MeSb(SSbMe2)2 is formed by elimination of Me3Sb from Me2SbSSbMe2. 相似文献
37.
Irina Yu. Bagryanskaya Enno Lork Andrey V. Zibarev 《Journal of fluorine chemistry》2006,127(6):746-754
1,2,3,4,5-Pentafluorodiphenyl disulfide (1) was synthesized from C6F5SCl and C6H5SSiMe3 in quantitative yield. The homo-crystals of disulfide 1 and co-crystals of 1,1′,2,2′,3,3′,4,4′,5,5′-decafluorodiphenyl disulfide (2) with naphthalene (stoichiometry 1:2, complex 4) and diphenyl disulfide (3) with octafluoronaphthalene (stoichiometry 2:1, complex 5) were prepared followed by XRD characterization. In the crystal lattice of 1, face-to-face and face-to-edge PhH/PhF orientations of neighboring rings were observed together with face-to-edge PhF/PhF orientations. For the face-to-face PhH/PhF orientation, the large offset of PhH and PhF groups excludes their π-stacking interaction which is very non-typical of the field. The crystal lattice of 4 reveals standard π-stacking interactions of the arene-polyfluoroarene type. While in the lattice of 4 each PhF ring interacts alternating with naphthalenes, in 5 two disulfides 3 are bridged by one octafluoronaphthalene with only one of the PhH rings of each disulfide interacting with the polyfluoroarene π-system. The large offset of neighboring molecules excludes however their π-stacking interactions in complex 5. An attempt to prepare 2/3 co-crystals failed. 相似文献
38.
Joachim Krieger Enno Lenzmann Pierre Raphaël 《Archive for Rational Mechanics and Analysis》2013,209(1):61-129
We consider the focusing L 2-critical half-wave equation in one space dimension, $$i \partial_t u = D u - |u|^2 u$$ , where D denotes the first-order fractional derivative. Standard arguments show that there is a critical threshold ${M_{*} > 0}$ such that all H 1/2 solutions with ${\|u\|_{L^2} < M_*}$ extend globally in time, while solutions with ${\|u\|_{L^2} \geq M_*}$ may develop singularities in finite time. In this paper, we first prove the existence of a family of traveling waves with subcritical arbitrarily small mass. We then give a second example of nondispersive dynamics and show the existence of finite-time blowup solutions with minimal mass ${\|u_0\|_{L^2} = M_*}$ . More precisely, we construct a family of minimal mass blowup solutions that are parametrized by the energy E 0 > 0 and the linear momentum ${P_0 \in \mathbb{R}}$ . In particular, our main result (and its proof) can be seen as a model scenario of minimal mass blowup for L 2-critical nonlinear PDEs with nonlocal dispersion. 相似文献
39.
Raivo Stern Ivo Heinmaa Enno Joon Alexander A. Tsirlin Hiroyuki Nakamura Tsuyoshi Kimura 《Applied magnetic resonance》2014,45(11):1253-1260
We present low-temperature (low-T, sub-liquid-N2) high-speed high-resolution 29Si solid-state (cryoMAS) nuclear magnetic resonance studies on a model 2D-BEC quantum magnet BaCuSi2O6, known also as Han Purple. We observe broadened 29Si lines below the well-established 100 K structural phase transition confirming the existence of inhomogeneities at low temperatures. Interestingly, the low-T spectra of \({\mathrm{BaCuSi}}_{2}{\mathrm{O}}_{6}\) closely resemble those of the novel compound Ba2CoSi2O6Cl2 taken at room temperature. This suggests that the Co compound features structural modulations or inhomogeneities already at room temperature. The low-T crystal structure and magnetism of \({\mathrm{BaCuSi}}_{2}{\mathrm{O}}_{6}\) are more complex than previously believed, and deserve further investigation. 相似文献
40.
Maurizio Roczen Enno Malguth Martin Schade Andreas Schöpke Abdelazize Laades Michael Blech Orman Gref Thomas Barthel Jan Amaru Töfflinger Manfred Schmidt Hartmut S. Leipner Lars Korte Bernd Rech 《Journal of Non》2012,358(17):2253-2256
Two different growth mechanisms are compared for the fabrication of Si/SiO2 nanostructures on crystalline silicon (c-Si) to be used as hetero-emitter in high-efficiency solar cells: (1) The decomposition of substoichiometric amorphous SiOx (a-SiOx) films with 0 < x < 1.3 and (2) the dewetting of thin amorphous silicon (a-Si) layers.The grown layers are investigated with regard to their structural properties, their passivation quality for c-Si wafer substrates and their electrical properties in order to evaluate their suitability as a nanodot hetero-emitter. While by layer decomposition, no passivating nanodots could be formed, the dewetting process allows fabricating nanodot passivation layers at temperatures as low as 600 °C. The series resistance through Ag/[Si-nanodots in SiO2]/c-Si/Al structures for dewetting is similar to nanostructured silicon rich SiOx films. Still, a nanodot hetero-emitter which exhibits both a satisfying passivation of the substrate and induces a high band bending by doping at the same time could not be fabricated yet. 相似文献