Synthesis, x-ray crystal structure, and multinuclear NMR study of the dynamic behavior of tris[dihydrobis(1-pyrazolyl)borato]yttrium(III); a molecule with three three-center, two-electron bonds

1988 ◽  
Vol 27 (11) ◽  
pp. 1890-1896 ◽  
Author(s):  
Daniel L. Reger ◽  
Jeffrey A. Lindeman ◽  
Lukasz Lebioda
2004 ◽  
Vol 43 (10) ◽  
pp. 3189-3199 ◽  
Author(s):  
Ashwani Vij ◽  
William W. Wilson ◽  
Vandana Vij ◽  
Robert C. Corley ◽  
Fook S. Tham ◽  
...  

2001 ◽  
Vol 79 (2) ◽  
pp. 195-200 ◽  
Author(s):  
Gerald W Buchanan ◽  
Majid F Rastegar ◽  
Glenn PA Yap

Benzo-9-crown-3 ether trimerizes in the presence of FeCl3 and aqueous H2SO4 to produce tris(9-crown-3)triphenylene in 25.4% yield. This compound crystallizes in the monoclinic P21/c space group: a = 13.759(2) Å, b = 13.318(2) Å, c = 13.399(2) Å, β = 96.883(2)°, with Z = 4. The three 9-crown-3 ether units of the trimer possess different geometries and there is substantial deviation from coplanarity in the three aromatic rings. 13C NMR chemical shifts in the solid state are consistent with this lack of symmetry and are discussed in terms of the X-ray crystal-structure data.Key words: crown ether, trimerization, stereochemistry.


1996 ◽  
Vol 35 (25) ◽  
pp. 7316-7324 ◽  
Author(s):  
Vladimir I. Bakhmutov ◽  
Marc Visseaux ◽  
Denise Baudry ◽  
Alain Dormond ◽  
Philippe Richard
Keyword(s):  
X Ray ◽  

1997 ◽  
Vol 539 (1-2) ◽  
pp. 9-17 ◽  
Author(s):  
Giancarlo Gioia Lobbia ◽  
Patrizio Cecchi ◽  
Roberto Gobetto ◽  
Giuseppe Digilio ◽  
Riccardo Spagna ◽  
...  

2018 ◽  
Vol 96 (7) ◽  
pp. 646-652 ◽  
Author(s):  
C. Leroy ◽  
J.K. Schuster ◽  
T. Schaefer ◽  
K. Müller-Buschbaum ◽  
H. Braunschweig ◽  
...  

Beryllium-9 (9Be) quadrupolar coupling and chemical shift tensor data are reported for bis(1-(2,6-diisopropylphenyl)-3,3,5,5-tetramethylpyrrolidine-2-ylidene)beryllium (Be(CAAC)2). These are the first such data for beryllium in a linear dicoordinate environment. The 9Be quadrupolar coupling constant, 2.36(0.02) MHz, is the largest recorded in the solid state to date for this isotope. The span of the beryllium chemical shift tensor, 22(2) ppm, covers about half of the known 9Be chemical shift range, and the isotropic 9Be chemical shift, 32.0(0.3) ppm, is the largest reported in the solid state to our knowledge. DFT calculations reproduce the experimental data well. A natural localized molecular orbital approach has been used to explain the origins and orientation of the beryllium electric field gradient tensor. The single-crystal X-ray structure of a second polymorph of Be(CAAC)2 is also reported. Inspection of the powder X-ray diffraction data shows that the new crystal structure is part of the bulk product next to another crystalline phase. Therefore, experimental X-ray powder data for the microcrystalline powder sample and the SSNMR data do not fully match either the originally reported crystal structure (Arrowsmith et al. Nat. Chem. 2016, 8, 890–894) or the new polymorph. The ability of solid-state NMR and powder X-ray diffraction to characterize powdered samples was thus particularly useful in this work.


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