Synthesis and solution behaviour of stable mono-, di- and trinuclear Pd(II) complexes of 2,5-pyridinedihydroxamic acid: X-ray crystal structure of a novel Pd(II) hydroxamato complex

2012 ◽  
Vol 380 ◽  
pp. 291-300 ◽  
Author(s):  
Darren M. Griffith ◽  
Linda Bíró ◽  
James A. Platts ◽  
Helge Müller-Bunz ◽  
Etelka Farkas ◽  
...  
1990 ◽  
Vol 31 (18) ◽  
pp. 2641-2642 ◽  
Author(s):  
W. Moene ◽  
M. Schakel ◽  
G.J.M. Hoogland ◽  
F.J.J. de Kanter ◽  
G.W. Klumpp ◽  
...  

2000 ◽  
Vol 78 (12) ◽  
pp. 1613-1619 ◽  
Author(s):  
Robyn E Boeré ◽  
René T Boeré ◽  
Jason Masuda ◽  
Gotthelf Wolmershäuser

The reaction of N,N'-bis(2,6-diisopropylphenyl)carbodiimide with lithium 2,6-diisopropylanilide, quenching with water and recrystallization from heptane produces the symmetric guanidine [DipNH]2C=NDip which crystallizes in the triclinic system, space group P[Formula: see text], a = 10.6513(11), b = 10.8997(11), c = 16.2961(17) Å, α = 80.524(12), β = 78.921(13), γ = 70.060(12)°, V = 1735.2(3) Å3, Z = 2. The molecule crystallizes with three perpendicular 2,6-diisopropylphenyl groups, which surround and shield the central CN3 unit, and provide (almost) three-fold symmetry around the central atom. Its dynamic solution behaviour has been studied by VT NMR between -90 and +180°C, and is consistent with three distinct barriers to N-CAr rotation. Preliminary estimates of the Gibbs free energy of activation for the lower two barriers are 56 ± 2 and 73 ± 2 kJ mol–1. Reaction of the title compound with Mo(CO)6 in refluxing n-heptane produces [DipNH]2C=NDip·Mo(CO)3, a complex in which Mo(CO)3 is η6-coordinated to one of the diisopropylphenyl rings.Key words: crystal structure, diisopropylaniline, guanidine, bulky ligands.


Polyhedron ◽  
2002 ◽  
Vol 21 (23) ◽  
pp. 2361-2367 ◽  
Author(s):  
Concepción López ◽  
Amparo Caubet ◽  
Sonia Pérez ◽  
Ramon Bosque ◽  
Xavier Solans ◽  
...  

2000 ◽  
Vol 3 (6) ◽  
pp. 303-306 ◽  
Author(s):  
G Annibale ◽  
P Bergamini ◽  
V Bertolasi ◽  
M Cattabriga ◽  
V Ferretti

Author(s):  
H.-J. Cantow ◽  
H. Hillebrecht ◽  
S. Magonov ◽  
H. W. Rotter ◽  
G. Thiele

From X-ray analysis, the conclusions are drawn from averaged molecular informations. Thus, limitations are caused when analyzing systems whose symmetry is reduced due to interatomic interactions. In contrast, scanning tunneling microscopy (STM) directly images atomic scale surface electron density distribution, with a resolution up to fractions of Angstrom units. The crucial point is the correlation between the electron density distribution and the localization of individual atoms, which is reasonable in many cases. Thus, the use of STM images for crystal structure determination may be permitted. We tried to apply RuCl3 - a layered material with semiconductive properties - for such STM studies. From the X-ray analysis it has been assumed that α-form of this compound crystallizes in the monoclinic space group C2/m (AICI3 type). The chlorine atoms form an almost undistorted cubic closed package while Ru occupies 2/3 of the octahedral holes in every second layer building up a plane hexagon net (graphite net). Idealizing the arrangement of the chlorines a hexagonal symmetry would be expected. X-ray structure determination of isotypic compounds e.g. IrBr3 leads only to averaged positions of the metal atoms as there exist extended stacking faults of the metal layers.


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