Bond Formation and Coupling between Germyl and Bridging Germylene Ligands in Dinuclear Palladium(I) Complexes

The dinuclear palladium(I) complexes [L(Ar2HGe)Pd(μ‐GeAr2)2Pd(GeHAr2)L] (Ar=Ph, p‐Tol; L=PMe3, tBuNC) contain terminal germyl and bridging germylene ligands with the experimentally observed Ge⋅⋅⋅Ge bond lengths of 2.8263(4) Å (L=PMe3) and 2.928(1) Å (L=tBuNC), which are close to the longest GeGe bo...

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Published in:Angewandte Chemie International Edition Vol. 54; no. 9; pp. 2679 - 2683
Main Authors: Tanabe, Makoto, Omine, Shumpei, Ishikawa, Naoko, Osakada, Kohtaro, Hayashi, Yoshihiro, Kawauchi, Susumu
Format: Journal Article
Language:English
Published: Weinheim WILEY-VCH Verlag 23-02-2015
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Edition:International ed. in English
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Summary:The dinuclear palladium(I) complexes [L(Ar2HGe)Pd(μ‐GeAr2)2Pd(GeHAr2)L] (Ar=Ph, p‐Tol; L=PMe3, tBuNC) contain terminal germyl and bridging germylene ligands with the experimentally observed Ge⋅⋅⋅Ge bond lengths of 2.8263(4) Å (L=PMe3) and 2.928(1) Å (L=tBuNC), which are close to the longest GeGe bond reported to date [2.714(1) Å]. Significant Ge⋅⋅⋅Ge interactions between the germylene and germyl ligands (PMe3 complexes > tBuNC complexes) are supported by DFT calculations, Wiberg bond indices (WBI), and natural bond orbital (NBO) analyses. Exchanging tBuNC for PMe3 ligands increases the Ge⋅⋅⋅Ge interaction, and simultaneously activates two PdGe bonds. Adding the chelating diphosphine 1,2‐bis(diethylphosphino)ethane (depe) to the PMe3 complexes results in the intramolecular coupling of germyl and germylene ligands followed by extrusion of a digermane. Cooperation of two metal centers: Electron‐donating auxiliary ligands of the dipalladium(I) complexes promote coupling of the bridging germylene (GeAr2) and terminal germyl (GeAr2H) ligands. The Ge⋅⋅⋅Ge bonding interaction of the dipalladium intermediate is enhanced by an electron‐donating PMe3 ligand which activates PdGe and PdPd bonds.
Bibliography:Grants-in-Aid for Scientific Research - No. 24350027; No. 25410061
This work was financially supported by Grants-in-Aid for Scientific Research (No. 24350027) and (No. 25410061) from the Ministry of Education, Culture, Sports, Science and Technology of Japan. The numerical calculations were carried out on the TSUBAME 2.5 supercomputer at the Tokyo Institute of Technology, Tokyo (Japan), and on the supercomputer at the Research Center for Computational Science, Okazaki (Japan).
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Ministry of Education, Culture, Sports, Science and Technology of Japan
ArticleID:ANIE201411041
This work was financially supported by Grants‐in‐Aid for Scientific Research (No. 24350027) and (No. 25410061) from the Ministry of Education, Culture, Sports, Science and Technology of Japan. The numerical calculations were carried out on the TSUBAME 2.5 supercomputer at the Tokyo Institute of Technology, Tokyo (Japan), and on the supercomputer at the Research Center for Computational Science, Okazaki (Japan).
ObjectType-Article-1
SourceType-Scholarly Journals-1
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content type line 23
ISSN:1433-7851
1521-3773
DOI:10.1002/anie.201411041