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81.
82.
A series of ruthenium(II) complexes bearing redox-active o-benzoquinonediimines (o-bqdi) was synthesized and characterized. Reactions of [RuCl(bdmpza)(η4-cod)] (bdmpza = bis(3,5-dimethylpyrazol-1-yl)acetato; cod = 1,5-cyclooctadiene) and 1,2-benzenediamines such as o-phenylenediamine (o-pdaH2), 4,5-difluoro-1,2-benzenediamine (o-pdaF2), 4,5-dichloro-1,2-benzenediamine (o-pdaCl2), and 4,5-dimethoxy-1,2-benzenediamine (o-pda(OMe)2) afforded [RuCl(bdmpza)(o-bqdiX2)] (X = H, 1; X = F, 2; X = Cl, 3; X = OMe, 4).  相似文献   
83.
Upon diastereodifferentiating the [2+2] photocycloaddition of ethylene to a series of p‐substituted (?)‐8‐phenylmenthyl cyclohexenonecarboxylates, the diastereoselectivity was critically controlled by the nature of the substituent introduced to the chiral auxiliary, and the p‐nitro‐substituted substrate afforded the cycloadducts in 90 % diastereomeric excess (de) and with 97 % isolated yield. Detailed experimental and theoretical conformation analyses revealed that the stacking interaction of the aromatic auxiliary with the cyclohexenone moiety plays the decisive role in determining the substrate conformation and is, therefore, responsible for the dramatic enhancement of the de. Of particular interest, the product de was directly related to the ellipticity of the substrate, enabling us to “predict” the de prior to photoirradiation.  相似文献   
84.
A novel polyhydroxylated 18-membered analogue of antimycin A3 was synthesized. Our synthesis commenced with Boc-l-threonine and was achieved by way of one-pot homocoupling/ring-closing olefin metathesis reaction cascade and Sharpless asymmetric dihydroxylation. The analogue exhibited a greater anticancer activity against HeLa cells, breast MDA-MB-231 cells, and prostate PC-3 cells compared to the original antimycin A3.  相似文献   
85.
86.
New ruthenium(II) complexes having a tetradentate ligand such as tris(2-pyridylmethyl)amine (TPA), tris[2-(5-methoxycarbonyl)pyridylmethyl]amine [5-(MeOCO)3-TPA], tris(2-quinolylmethyl)amine (TQA), or bis(2-pyridylmethyl)glycinate (BPG) have been prepared. The reaction of the ligand with [RuCl2(Me2SO)4] resulted in a mixture of trans and cis isomers of the chloro(dimethyl sulfoxide-kappaS)ruthenium(II) complexes containing a TPA or a BPG, whereas a trans(Cl,N(amino)) isomer was selectively obtained for 5-(MeOCO)3-TPA and TQA. The trans and cis isomers of the [RuCl(TPA)(Me2SO)]+ complex were easily separated by fractional recrystallization. The molecular structures of trans- and cis(Cl,N(amino))-[RuCl(TPA)(Me2SO)]+ complexes and the trans(Cl,N(amino))-[RuCl{5-(MeOCO)3-TPA}(Me2SO)]+ complex have been determined by X-ray structural analyses. The reaction of TPA with [RuCl2(PhCN)4] gave a single isomer of the chloro(benzonitrile)ruthenium(II) complex, whereas the bis(benzonitrile)ruthenium(II) complex was obtained with BPG. The cis(Cl,N(amino))-[RuCl(TPA)(Me2SO)]+ complex is thermodynamically much less stable than the trans isomer and isomerizes in dimethyl sulfoxide at 65-100 degrees C. Oxygenation of alkanes catalyzed by these ruthenium(II) complexes has been examined. The chloro(dimethyl sulfoxide-kappaS)ruthenium(II) complexes with TPA and its derivatives using m-chloroperbenzoic acid as a cooxidant showed high catalytic ability. Adamantane was efficiently and selectively oxidized to give 1-adamantanol up to 88%. The chloro(dimethyl sulfoxide-kappaS)ruthenium(II) complex with 5-(MeOCO)3-TPA was found to be the most active catalyst among the complexes examined.  相似文献   
87.
A novel photoactivated artificial muscle model unit is reported. Here we show that organic/inorganic hybrid nanosheets reversibly slide horizontally on a giant scale and the interlayer spaces in the layered hybrid structure shrink and expand vertically by photoirradiation. The sliding movement of the system on a giant scale is the first example of an artificial muscle model unit having much similarity with that in natural muscle fibrils. In particular, our layered hybrid molecular system exhibits a macroscopic morphological change on a giant scale (~1500 nm) relative to the molecular size of ~1 nm by means of a reversible sliding mechanism.  相似文献   
88.

UV excitation for several Eu 2+ -doped melilite crystals, Eu 2+ :Ca 2 Al 2 SiO 7 (CASM), Eu 2+ :CaSrAl 2 SiO 7 (CSASM), and Eu 2+ :Sr 2 Al 2 SiO 7 (SASM) produces long-lasting phosphorescence (1-10 2 v s) from Eu 2+ ions besides the intrinsic Eu 2+ luminescence. The distribution of the radiative decay rates is due to the recombination of distant pairs of trapped electrons and holes in the crystals. The intensities of the phosphorescence for these crystals were measured as functions of temperature and time. The most intense phosphorescence was obtained from the Eu 2+ : SASM crystal. The decay curves measured for Eu 2+ :SASM below 400 v K fit t m n ( n h 1). This fact shows that the recombination of the distant pairs occurs through tunneling below 400 v K. The temperature dependence of the intensities integrated in a time domain obeys the Arrhenius's equation with two thermal activation energies including radiative and non-radiative processes. These results suggest that holes and electrons recombine radiatively at Eu 2+ sites in the SASM crystal through thermal hopping and tunneling. On the other hand, Eu 2+ :CASM and Eu 2+ :CSASM show different behavior on the decay curves at low temperatures, satisfying t m n ( n >1). This discrepancy may be removed by several electron and/or hole centers with different trapping energy levels.  相似文献   
89.
A practical method for synthesizing chiral α-amino phosphonic acid derivatives was developed. Readily available and stable N-o-nitrophenylsulfenyl (Nps) imino phosphonate was utilized as a substrate for a highly enantioselective Friedel–Crafts-type addition of indole or pyrrole nucleophiles catalyzed by chiral phosphoric acid. The resulting adduct was easily converted into N-9-fluorenylmethyloxycarbonyl (Fmoc) amino phosphonic acid, which is useful for synthesizing peptides containing an amino phosphonic acid.  相似文献   
90.
One of the most striking results is the large elliptic flow (v 2) at RHIC. Detailed mass and transverse momentum dependence of elliptic flow are well described by ideal hydrodynamic calculations for p T<1 GeV/c, and by parton coalescence/recombination picture for p T=2–6 GeV/c. The systematic error on v 2 is dominated by so-called “non-flow effects”, which are correlations other than flow, such as resonance decays and jets. It is crucial to understand and reduce the systematic error from non-flow effects in order to understand the underlying collision dynamics. In this paper, we present the centrality dependence of v 2 with respect to the first harmonic event plane at ZDC-SMD (v 2{ZDC-SMD}) in Au + Au collisions at  GeV. A large rapidity gap (|Δη|>6) between midrapidity and the ZDC-SMD could enable us to minimize possible non-flow contributions. We compare the results of v 2{ZDC-SMD} with v 2{BBC}, which is measured by event plane determined at |η|=3.1–3.9. Possible non-flow contributions in those results will be discussed.  相似文献   
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