metal-organic compounds
parent atoms. The maximum and minimum electron densities (1.31
3
orientations of the isopropyl groups are limited by intramo-
lecular CÁ Á ÁS interactions. The butane solvent is not involved
in any interaction as there is no potential acceptor atom.
It is quite interesting to note that the molecular structure is
stabilized by intramolecular CÐHÁ Á Áꢀ interactions between
the aromatic H atoms of the PPh3 groups and the centroid
(Cg) of the chelate ring (atoms Au1, S1, C37 and S2)
Ê
Ê
and 1.46 e A ) were observed at distances of 1.05 and 0.89 A,
respectively, from the Au1 atom.
Data collection: SMART (Siemens, 1996); cell re®nement: SAINT
(Siemens, 1996); data reduction: SAINT; program(s) used to solve
structure: SHELXTL (Sheldrick, 1997); program(s) used to re®ne
structure: SHELXTL; molecular graphics: SHELXTL; software used
to prepare material for publication: SHELXTL and PLATON (Spek,
1990).
Ê
[C2Á Á ÁCg = 3.48, H2AÁ Á ÁCg = 2.68 A and C2ÐH2AÁ Á ÁCg =
ꢀ
Ê
145 ; C36Á Á ÁCg = 3.43, H36AÁ Á ÁCg = 2.72 A and C36Ð
H36AÁ Á ÁCg = 133ꢀ].
The authors would like to thank the Malaysian Government
and Universiti Sains Malaysia for research grant R&D No.
305/p®zik/610942. SSSR thanks the Universiti Sains Malaysia
for a Visiting Postdoctoral Fellowship. The authors thank
Professor A. L. Spek for valuable help in resolving the space-
group ambiguity.
Experimental
Sodium N,N0-diisopropyldithiocarbamate, Na(S2CNiPr2), dissolved in
H2O was added to gold trichloride at room temperature with stirring.
The brown reaction mixture was ®ltered and the ®ltrate was washed
with water and dried overnight in a vacuum. The brown solid
obtained was dissolved in butane. Triphenylphosphine was added at
353±363 K with stirring and the solution was re¯uxed for 4±5 h before
cooling. Single crystals of (I) suitable for X-ray analysis were grown
by slow evaporation at room temperature over a period of two weeks.
Supplementary data for this paper are available from the IUCr electronic
archives (Reference: SK1392). Services for accessing these data are
described at the back of the journal.
Crystal data
3
[Au(C7H14NS2)(C18H15P)2]ÁC4H10
Dx = 1.376 Mg m
Mo Kꢂ radiation
Cell parameters from 8192
re¯ections
Mr = 955.94
Monoclinic, P21=c
References
Ê
Ê
a = 12.0927 (2) A
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Dalton Trans. pp. 1099±1102.
b = 25.2129 (5) A
ꢃ = 1.57±28.35ꢀ
ꢄ = 3.378 mm
T = 293 (2) K
1
Ê
c = 15.4999 (3) A
ꢁ = 102.392 (1)ꢀ
V = 4615.70 (15) A
Z = 4
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3
Ê
Slab, colourless
0.42 Â 0.28 Â 0.12 mm
Data collection
Siemens SMART CCD area-
detector diffractometer
! scans
Absorption correction: empirical
(SADABS; Sheldrick, 1996)
Tmin = 0.331, Tmax = 0.687
31 290 measured re¯ections
11 360 independent re¯ections
5735 re¯ections with I > 2ꢅ(I)
Rint = 0.072
ꢃ
max = 28.26ꢀ
h = 16 ! 16
k = 29 ! 33
l = 20 ! 17
Re®nement
Re®nement on F2
R[F2 > 2ꢅ(F2)] = 0.052
wR(F2) = 0.119
S = 0.988
11 360 re¯ections
478 parameters
H-atom parameters constrained
w = 1/[ꢅ2(Fo2) + (0.0331P)2]
where P = (Fo2 + 2Fc2)/3
(Á/ꢅ)max = 0.001
Sheldrick, G. M. (1996). SADABS. University of GoÈttingen, Germany.
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Inc., Madison, Wisconsin, USA.
Spek, A. L. (1990). Acta Cryst. A46, C-34.
3
Ê
Áꢆmax = 1.31 e A
3
Ê
1.46 e A
Áꢆmin
=
Vogler, A. & Kunkely, H. (1988). Chem. Phys. Lett. 150, 135±137.
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3747±3752.
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3499±3503.
The butane solvent is disordered and so some atoms have a higher
atomic displacement parameter ratio. All H atoms were ®xed
geometrically at calculated distances and allowed to ride on their
ꢁ
940 Fangfang Jian et al. [Au(C7H14NS2)(C18H15P)2]ÁC4H10
Acta Cryst. (2000). C56, 939±940