Mercury(II) and methylmercury(II) complexes of novel sterically hindered thiolates: carbon-13 and mercury-199 NMR studies and the crystal and molecular structures of [MeHg(SC6H2-2,4,6-Pr-iso3)], [Hg(SC6H4-2-SiMe3)2], [Hg(2-SC5H3N-3-SiMe3)2], and [Hg{(2-SC6H4)2SiMe2}]2

1990 ◽  
Vol 29 (17) ◽  
pp. 3172-3181 ◽  
Author(s):  
Eric Block ◽  
Maria Brito ◽  
Michael Gernon ◽  
Deborah McGowty ◽  
Hyunkyu Kang ◽  
...  
ChemInform ◽  
1989 ◽  
Vol 20 (34) ◽  
Author(s):  
R. M. H. BANDA ◽  
I. G. DANCE ◽  
T. D. BAILEY ◽  
D. C. CRAIG ◽  
M. L. SCUDDER

1987 ◽  
Vol 42 (4) ◽  
pp. 387-394 ◽  
Author(s):  
Susanna Kerschl ◽  
Bernd Wrackmeyer ◽  
Detlef Männig ◽  
Heinrich Nöth ◽  
Rudolf Staudigl

Bis(triorganylstannyl)chalcogenides (O, S, Se) have been studied by 119Sn NMR in solution. In most cases the magnitude of the geminal coupling constants 2J(SnSn) are indicative of a bent arrangement SnXSn (X = O, S, Se). The exception is bis(tri-tert-butylstannyl)oxide for which the linear structure S n - O - S n as determined by X-ray diffraction in the solid state is preserved in solution. The trend of the coupling constants 2J(SnSn) depending on X and on the bond angle SnXSn suggests that 2J(SnOSn) > 0 and 2J(SnSSn), 2J(SnSeSn) <0. The X-ray diffraction study of bis(tribenzylstannyl)sulfide shows a bent arrangement (∢SnSSn 105.52(14)°) in contrast to the corresponding oxide.


1993 ◽  
Vol 71 (12) ◽  
pp. 2129-2138 ◽  
Author(s):  
Wolfgang Kliegel ◽  
Gottfried Lubkowitz ◽  
Steven J. Rettig ◽  
James Trotter

The syntheses of the sterically hindered N,N′-dihydroxyaminals; N,N′-bis(1-ethoxycarbonyl-1-methylethyl)-N,N′-dihydroxymethanediamine, 1b, and N,N′-bis(1,1-dimethylethyl)-N,N′-dihydroxymethanediamine, 1c, and their reactions with phenylboronic acid to yield the 1,3,5-trioxa-6,8-diaza-2,4-diboracyclooctanes 3 and 4, respectively, are described. Crystals of 1b are tetragonal, a = 18.413(1), c = 9.867(2) Å, Z = 8, space group I41; those of 3 are monoclinic, a = 20.420(4), b = 8.272(4), c = 17.851(5) Å, β = 117.34(1)°, Z = 4, space group C2/c; and those of 4 are monoclinic, a = 9.493(4), b = 16.202(4), c = 14.783(3) Å, β = 101.90(2)°, Z = 4, space group P21/c. The structures were solved by direct methods and were refined by full-matrix least-squares procedures to R = 0.034, 0.039, and 0.040 (Rw = 0.035, 0.034, and 0.036) for 1550, 1438, and 2187 reflections with I ≥ 3σ(F2), respectively. In the solid state, both 3 and 4 exhibit transannular [Formula: see text] interactions. In 3 there are two identical (by symmetry) interactions with [Formula: see text] Å that have estimated bond orders of 0.06, while the single transannular interaction in 4 has N—B = 1.953(3) Å and a bond order of about 0.3. The intermediate-strength transannular interaction in 4 is the first to be reported for this type of molecule.


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