metal-organic compounds
Table 1
Selected geometric parameters (A, ).
comprises more than half the structures, the biphenyl rings are
relatively ¯at, with torsion angles of 2±38ꢁ. These structures
are constrained by virtue of a direct bond between S atoms
(i.e. disul®de), or by a single S, O or Se atom bridging between
the 6- and 60-positions of the biphenyl rings. Another subset of
structures contains metal chelates (M = Mo, Ni, Pd, Rh, Ti, Cu
and Ru), with torsion angles of 59±87ꢁ. If there are bulky
groups opposite the S atoms, i.e. in the 6- and 60-positions, the
torsion angles between the phenyl rings tend to be ꢀ90ꢁ.
Finally, there are a few structures that contain bulky groups
bonded to the S atoms (e.g. sulfonates), and the torsion angle
can be as high as 116ꢁ. Complex (I) appears to fall into this last
category. The (triphenylphosphine)gold units coordinated to
sulfur are very bulky, and the torsion angle between the
phenyl rings opens up to 119ꢁ in order to minimize inter-
actions between the triphenylphosphine rings. Inspection of
(I) also reveals that the Au atoms appear to be drawn
together, leading to a signi®cant bending of the PÐAuÐS
angles [170.24 (5) and 169.52 (5)ꢁ]. However, as noted
above, the long distance between the Au atoms precludes a
typical gold±gold bonding interaction. Comparison with
other structures shows that signi®cant bending is observed
when short gold±gold, gold±metal or gold±heteroatom
interactions are present [e.g. AuÐAu (Davila et al., 1993;
Crespo et al., 1997), AuÐIr (Rio et al., 2001), AuÐOs (Leung
et al., 1998), AuÐN (Vincert et al., 2001; Wilton-Ely et al.,
2002) and AuÐS (Wilton-Ely et al., 2001; Kuz'mina et al.,
1993)]. These observations suggest the possibility that auro-
philicity, even at these long distances, may in¯uence the solid-
state structure. In recent work, Pyykko and co-workers
(Pyykko & Tamm, 1998; Pyykko, 2004) estimated the auro-
philic energy as a function of the AuÁ Á ÁAu distance, and at
ꢁ
Ê
Au1ÐP1
Au1ÐS1
Au2ÐP2
Au2ÐS2
P1ÐC19
P1ÐC25
2.2605 (14)
2.3020 (13)
2.2565 (13)
2.3024 (13)
1.804 (6)
P1ÐC13
P2ÐC31
P2ÐC43
P2ÐC37
S1ÐC1
1.823 (5)
1.806 (5)
1.819 (5)
1.823 (5)
1.777 (5)
1.779 (5)
1.820 (5)
S2ÐC12
P1ÐAu1ÐS1
P2ÐAu2ÐS2
170.24 (5)
169.52 (5)
C1ÐS1ÐAu1
C12ÐS2ÐAu2
111.05 (17)
107.15 (17)
S1ÐAu1ÐAu2ÐS2
95.62 (5)
P1ÐAu1ÐAu2ÐP2
86.23 (5)
Data collection
Bruker SMART 1K CCD
diffractometer
! scans
Absorption correction: multi-scan
(SADABS; Sheldrick, 1996)
Tmin = 0.319, Tmax = 0.756
10 002 independent re¯ections
6889 re¯ections with I > 2ꢄ(I)
Rint = 0.066
ꢂmax = 28.3ꢁ
h = 26 ! 26
k = 13 ! 13
42 287 measured re¯ections
l = 26 ! 25
Re®nement
Re®nement on F2
R[F2 > 2ꢄ(F2)] = 0.037
wR(F2) = 0.071
S = 1.00
10002 re¯ections
w = 1/[ꢄ2(F2o) + (0.026P)2
+ 4.627P]
where P = (F2o + 2Fo2)/3
(Á/ꢄ)max = 0.002
3
Ê
Áꢅmax = 1.00 e A
3
Ê
0.92 e A
Extinction correction: SHELXL97
488 parameters
H-atom parameters constrained
Áꢅmin
=
Extinction coef®cient: 0.00011 (3)
Ê
H atoms were positioned geometrically (CÐH = 0.95 A) and
treated as riding, with Uiso(H) values of 1.2Ueq(C). The ®nal differ-
ence map was featureless, the highest residual electron-density peaks
Ê
being approximately 0.9 A from the Au atoms.
Ê
3.9 A, a gold±gold interaction is estimated to be around
3 kJ mol 1. This is about one-tenth of the strength of a typical
strong gold±gold interaction. Other weak interactions, such as
CÐHÁ Á ÁF, which are estimated to be signi®cantly weaker than
a typical OÁ Á ÁH hydrogen bond, have been shown to be
important features for stabilizing crystal structures (Howard et
al., 1996; Thalladi et al., 1998; Lee et al., 2000).
Data collection: SMART (Bruker, 1997); cell re®nement: SAINT
(Bruker, 1997); data reduction: SAINT; program(s) used to solve
structure: SHELXTL (Siemens, 1994); program(s) used to re®ne
structure: SHELXTL; molecular graphics: SHELXTL; software used
to prepare material for publication: SHELXTL.
The authors acknowledge support from both the NSF,
International Programs (grant No. CHE-98-10077), and the
Russian Foundation for Basic Research (grant Nos. 00-03-
32840 and 03-03-32716). Data were collected through the Ohio
Crystallographic Consortium, funded by the Ohio Board of
Regents 1995 Investment Fund (grant No. CAP-075), located
at the University of Toledo Instrumentation Center in A&S,
Toledo, OH 43606, USA.
Experimental
Complex (I) was synthesized by reaction of ClAuPPh3 (910 mg,
1.84 mmol) and 1,10-biphenyl-2,20-dithiol (200 mg, 0.92 mmol) in the
presence of trimethylbenzylammonium chloride (68 mg, 0.36 mmol)
and K2CO3 (500 mg, 3.62 mmol) in a tetrahydrofuran/methanol
solution. Crystals suitable for X-ray analysis were grown from Et2O/
CH2Cl2 and were obtained as colorless plates.
Supplementary data for this paper are available from the IUCr electronic
archives (Reference: FR1487). Services for accessing these data are
described at the back of the journal.
Crystal data
[Au2(C12H8S2)(C18H15P)2]
Mr = 1134.78
Monoclinic, P21=c
Mo Kꢁ radiation
Cell parameters from 6392
re¯ections
References
ꢂ = 2.5±28.3ꢁ
Ê
Ê
a = 20.0310 (4) A
1
b = 10.2199 (2) A
ꢃ = 7.40 mm
T = 150 (2) K
Allen, F. H. (2002). Acta Cryst. B58, 380±388.
Ê
c = 20.0399 (3) A
Boer, B. de, Meng, H., Perepichka, D., Zheng, J., Frank, M., Chabal, Y. & Boa,
Z. (2003). Langmuir, 19, 4272±4284.
Bondi, A. (1964). J. Phys. Chem. 68, 441±451.
Bruker (1997). SAINT (Version 5.A06) and SMART (Version 5.051). Bruker
AXS Inc., Madison, Wisconsin, USA.
ꢀ = 96.303 (2)ꢁ
V = 4077.67 (13) A
Plate, colorless
0.20 Â 0.10 Â 0.04 mm
3
Ê
Z = 4
Dx = 1.848 Mg m
3
ꢂ
Acta Cryst. (2004). C60, m440±m442
Scott A. Larkin et al.
[Au2(C12H8S2)(C18H15P)2] m441