The last several years have produced some key advances in the area of alkene and alkyne metathesis by high oxidation state alkylidene and alkylidyne complexes along with new applications in organic and polymer chemistry. In this review we cover some of these developments and applications. The first part of this review concerns developments in catalyst synthesis and new catalysts. The second part concerns notable applications in organic and polymer chemistry. We discuss only high oxidation state alkylidene and alkylidyne chemistry of relevance to alkene or alkyne metathesis reactions and favor studies in the homogeneous phase.

Fluorinated amino acids can have dramatic effects on protein stability and protein-protein interactions due to the unique stereoelectronic properties of fluorine. Previous approaches to assessing their properties have mainly focused on helical systems, even though fluoro-amino acids are known to exhibit lower intrinsic helix propensities than their hydrocarbon analogues. Fluorination of specific b-sheet positions within globular proteins has been shown to have a stabilizing effect, suggesting that fluorinated amino acids may generally be well suitable for modulating non-helical structures. Still, fluorinated amino acids have rarely been studied in amyloid forming peptides, which take on a characteristically high cross-b-sheet content. Here, we examine the substitution of natural amino acids within an amyloid forming model peptide by amino acids that contain different stoichiometries of fluorine in their side chains. This approach enables a systematic evaluation of the impact of fluorine on amyloid formation. We have investigated the impact of size, hydrophobicity and secondary structure propensities of the fluorinated amino acids on the amyloid formation process. The structure of the model peptide is based on an engineered coiled coil folding motif that was designed to provide an a-helical starting structure that can fold into b-sheet rich amyloids under controlled conditions. Substitution with fluorinated amino acids was accomplished for two neighboring valine residues that play a key role in the structural transition. The resulting peptides show an unexpected folding behavior as a consequence of the interplay of stereoelectronic effects, helix propensity, hydrophobicity and position of the particular substitution within the amyloid forming system.

Thin semiconductor CuInSe 2 and CuInS 2 films (CIS) with bandgap values (E g ) of around 1.04 eV (for selenide) and 1.5 eV (for sulfide) represent an important class of the currently developed light absorbers for solar energy harvesting. [1,2] Conversion efficiencies of 12±13 % were achieved on large area modules, [1] whereas close to 18 % was achieved with laboratory cells, [3] indicating a large potential for CIS-derived photovoltaic materials. For their preparation, a broad range of physical [1±3] and electrochemical deposition routes [4] are available. Typically, CIS films are created via a rapid thermal sintering of elemental Cu, In and Se layers evaporated on Mo-coated glass substrates. The photovoltaic cell is then completed by overcoating the CIS-macrograins with a thin CdS buffer layer and a metal± organic chemical vapor deposition derived, transparent Al/ ZnO window electrode. In this contribution, we address a low cost colloidal route to nanocrystalline ZnO/CIS bilayers on indium tin oxide (ITO) glass. For the film deposition, concentrated coating colloids, with size-quantized CuInS 2 particles were developed. It is well-established that size quantization in semiconductors (i.e. increasing bandgap energy with decreasing semiconductor dimension) takes place at particle dimensions smaller than the Wannier±Mott (WM) exciton of the corresponding macroscopic bulk phase.[5] By knowledge of the high frequency dielectric constant, e ¥ , and the reduced effective exciton mass, m = 1/(m ±1 e + m ±1 h ), one can calculate the WM-exciton Bohr radius according to R B = (e ¥ /m)´a B , with a B being the Bohr radius of the hydrogen atom. Taking the CIS bulk values [6] of e ¥ = 11, m e = 0.16 and m h = 1.3, we calculated the WM-exciton size to be 8.1 nm, which predicts a blue shift in the optical absorption threshold (below 826 nm = 1240/1.5 eV) for CIS-particle sizes below 8 nm. Figure 1 shows changes in the optical absorption spectrum during the CIS condensation. Condensation was induced on addition of bis(trimethylsilyl)sulfide to a mixture of Cu(I)±P(OPh) 3 and In(III)±P(OPh) 3 complexes (Cu/ In = 1) in Ar saturated acetonitrile (for details see Experimental).At sulfide concentrations~25 % (with respect to the present metals), the absorption spectrum exhibits a shoulder located at 370 nm that is strongly blue-shifted with respect to the bulk crystals (a gap energy difference of more than 2 eV). On further addition of the sulfide source (50 %), the absorption shoulder shifts from 370 nm to 400 nm, and the optical density rises due to increasing particle concentration. Under stoichiometric conditions (100 % S corresponds to the Cu:In:S stoichiometry of 1:1:2), a steep tail is observed with the absorption onset located near 580 nm.A remarkable dynamic color change accompanies this condensation process which can be seen with the naked eye. On each dropwise addition of the sulfide source, the color of the reacting solution rapidly changes from colorless to yellow to orange to red and becomes colorless or yellow agai...

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