ADVERTISEMENT RETURN TO ISSUEPREVArticleNEXTFullerene-bound dendrimers: soluble, isolated carbon clustersK. L. Wooley, C. J. Hawker, J. M. J. Frechet, F. Wudl, G. Srdanov, S. Shi, C. Li, and M. KaoCite this: J. Am. Chem. Soc. 1993, 115, 21, 9836–9837Publication Date (Print):October 1, 1993Publication History Published online1 May 2002Published inissue 1 October 1993https://pubs.acs.org/doi/10.1021/ja00074a075https://doi.org/10.1021/ja00074a075research-articleACS PublicationsRequest reuse permissionsArticle Views743Altmetric-Citations159LEARN ABOUT THESE METRICSArticle Views are the COUNTER-compliant sum of full text article downloads since November 2008 (both PDF and HTML) across all institutions and individuals. These metrics are regularly updated to reflect usage leading up to the last few days.Citations are the number of other articles citing this article, calculated by Crossref and updated daily. Find more information about Crossref citation counts.The Altmetric Attention Score is a quantitative measure of the attention that a research article has received online. Clicking on the donut icon will load a page at altmetric.com with additional details about the score and the social media presence for the given article. Find more information on the Altmetric Attention Score and how the score is calculated. Share Add toView InAdd Full Text with ReferenceAdd Description ExportRISCitationCitation and abstractCitation and referencesMore Options Share onFacebookTwitterWechatLinked InRedditEmail Other access optionsGet e-Alertsclose Get e-Alerts
A one-pot reaction cascade performed with two different star polymers, each containing a different catalytic group confined in its core, was demonstrated. Star polymers containing p-toluenesulfonic acid 3 and an amine moiety 6 were prepared by free-radical polymerization of styrene/DVB/1/2 and styrene/DVB/4/5, respectively. These star polymers were applied to a one-pot reaction cascade of 7 with 8 (3-catalyzed deprotection of a dimethyl acetal group and 6-catalyzed Baylis-Hillman reaction) to give 9 in 65% yield with the formation of 10 in 34% yield.
Abstract A direct boundary element procedure is presented to determine the impedance matrix for a three‐dimensional foundation supported on an infinitely‐long canyon of uniform cross‐section cut in a homogeneous half‐space. The uniform cross‐section of the canyon permits analytical integration along the canyon axis leading to a series of two‐dimensional boundary problems involving Fourier transforms of the full‐space Green's functions. Solution of these two‐dimensional boundary problems leads to a dynamic flexibility influence matrix which is inverted to determine the impedance matrix. The accuracy of the procedure is demonstrated by comparison with previous solutions for a surface‐supported, square foundation and results obtained by a three‐dimensional boundary element method (BEM) for a foundation of finite‐width supported on an infinitely‐long canyon. Compared with the three‐dimensional BEM, the present method requires less computer storage and is more accurate and efficient. The foundation impedance matrix determined by this procedure can be incorporated in a substructure method for earthquake analysis of arch dams.
Lead halide materials have seen a recent surge of interest from the photovoltaics community following the observation of surprisingly high photovoltaic performance, with optoelectronic properties similar to GaAs. This begs the question: What is the limit for the efficiency of these materials? It has been known that under 1-sun illumination the efficiency limit of crystalline silicon is ∼29%, despite the Shockley–Queisser (SQ) limit for its bandgap being ∼33%: the discrepancy is due to strong Auger recombination. In this article, we show that methyl ammonium lead iodide (MAPbI3) likewise has a larger than expected Auger coefficient. Auger nonradiative recombination decreases the theoretical external luminescence efficiency to ∼95% at open-circuit conditions. The Auger penalty is much reduced at the operating point where the carrier density is less, producing an oddly high fill factor of ∼90.4%. This compensates the Auger penalty and leads to a power conversion efficiency of 30.5%, close to ideal for the MA...
We report the isolation and characterization of arylpalladium cyanide complexes that undergo reductive elimination to form arylnitriles. The rates of reductive elimination from a series of arylpalladium cyanide complexes reveal that the electronic effects on the reductive elimination from arylpalladium cyanide complexes are distinct from those on reductive reductive eliminations from arylpalladium alkoxo, amido, thiolate, and enolate complexes. Arylpalladium cyanide complexes containing aryl ligands with electron-donating substituents undergo reductive elimination of aromatic nitriles faster than complexes containing aryl ligands with electron-withdrawing substituents. In addition, the transition state for the reductive elimination of the aromatic nitrile is much different from that for reductive eliminations that occur from most other arylpalladium complexes. Computational studies indicate that the reductive elimination of an arylnitrile from Pd(II) occurs through a transition state more closely related in structure and electronic distribution to that for the insertion of CO into a palladium-aryl bond.