Reaction of sulfur dioxide with the unsaturated triosmium-platinum clusters Os3Pt(.mu.-H)2(CO)10(PR3) (R = c-C6H11, C6H5). X-ray crystal structure of Os3Pt(.mu.-H)2(.mu.-SO2)(CO)10(PCy3)

1989 ◽  
Vol 8 (7) ◽  
pp. 1665-1673 ◽  
Author(s):  
Paul. Ewing ◽  
Louis J. Farrugia
ChemInform ◽  
1988 ◽  
Vol 19 (30) ◽  
Author(s):  
B. BEAGLEY ◽  
O. EL-SAYRAFI ◽  
G. A. GOTT ◽  
D. G. KELLY ◽  
C. A. MCAULIFFE ◽  
...  

ChemInform ◽  
2010 ◽  
Vol 22 (6) ◽  
pp. no-no
Author(s):  
S. G. BOTT ◽  
A. D. BURROWS ◽  
O. J. EZOMO ◽  
M. F. HALLAM ◽  
J. G. JEFFREY ◽  
...  

2001 ◽  
Vol 3 (1) ◽  
pp. 41-48 ◽  
Author(s):  
Dietrich Döpp

The known light induced reactions of sulfonamides and sultams are in most (but not all) cases initiated by S–N homolysis. Sulfur dioxide release may be a consequence of this primary process. In the author's laboratory three hitherto unexplored photoreactions of saccharin-derived sultams have been investigated: (i) a novel formal oxygen shift from sulfur to nitrogen generating upto now unknown cyclic N-hydroxysulfinamides; (ii) a condensative dimerization of 2,3-dihydro-1,2- benzoisothiazole 1,1-dioxide generating a new cleft molecule, and (iii) a facile allylic skeletal rearrangement of a pyrrolo-anellated dihydro- 1,2-benzoisothiazole. At least in the latter two cases an initial S–N-homolysis seems to be vital for the processes observed, whereas in the first case some ambiguity remains with respect to the first step. Scope and limitations are discussed and rationales for the conversions observed are presented, with special emphasis on structure proof by X-ray crystal structure determinations. All reactions discussed have to be treated within the wider context of current sulfonamide and sultam photochemistry.


1986 ◽  
Vol 5 (3) ◽  
pp. 519-525 ◽  
Author(s):  
Jos. Terheijden ◽  
Gerard. Van Koten ◽  
W. Pim. Mul ◽  
Derk J. Stufkens ◽  
Fred. Muller ◽  
...  

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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