methane to 576 nm in THF. The solvatochromic behaviour of
the arsonium and stibonium betaines is almost identical to that
of the related phosphonium betaines 5 (E = P, Ar = Ph; X =
Cl, Br, or Ph) which we reported recently.15 There is currently
growing interest in the optical properties of organic derivatives
of the main group 15 elements.16,17
We thank the EPSRC National Mass Spectrometry Service
Centre, University of Wales, Swansea, for high resolution
FABMS determinations, and also Neotronics Scientific Ltd for
financial support.
Notes and References
† Author to whom crystallographic enquiries should be addressed.
‡ Crystal data: C31.5H23NOClSbBr2·CuI2, Mr = 1065.87, monoclinic,
space group P21/n, a = 9.259(5), b = 24.785(11), c = 15.100(7) Å, b =
98.998(2)°, U = 3422.6(3) Å3, Z = 4, Dc = 2.069 g cm23, m = 5.653
mm21, F(000) = 2000, crystal size 0.2 3 0.02 3 0.02 mm. Data were
collected at 160 K, with a wavelength of 0.6875 Å, on a Bruker (formerly
Siemens) SMART CCD area detector diffractometer, equipped with a
silicon(111) crystal monochromator and a palladium coated focussing
mirror on station 9.8 of the Daresbury SRS. w scans, with a frame increment
Fig. 1 Structure of the tetraarylstibonium cation with selected bond lengths
(Å) and angles (°) for cation and di-iodocuprate anion: Sb–N1 2.65(4), Sb–
C1 2.09(2), Sb–C7 2.13(2), Sb–C13 2.13(2), Sb–C19 2.114(14), C25–N1
1.28(2), Cu1–I1 2.508(2), Cu1–I2 2.576(2), Cu–Cu 2.732(4); C1–Sb–C7
106.7(7), C1–Sb–C13 119.2(6), C1–Sb–C19 113.6(6), C7–Sb–C13
102.0(7), C7–Sb–C19 101.4(6), C13–Sb–C19 115.9(6), C19–C24–C25
121.2(14), N1–C25–C24 118.9(13), N1–Sb–C1 83.9(7).
of 0.3°, were used to cover a hemisphere of reciprocal space, giving qmin
=
1.54° and qmax = 20.00° (index ranges 211 @ h @ 12, 226 @ k @ 32, 218
@ l @ 19). Corrections were applied to account for incident beam decay and
absorption effects. A solution was obtained via direct methods and refined
by full-matrix least-squares on F2. 3520 unique data were produced from
moiety shows a considerable distortion from the expected linear
arrangement as a result of a very short copper–copper
interaction (2.73 Å) with a second di-iodocuprate anion in the
11707 measured reflections (Rint = 0.0882). 389 parameters refined to R1
=
0.0573 and wR2 = 0.1253 [I > 2s(I)] with s = 1.057 and residual electron
densities of 0.967 and 21.124 e Å23. CCDC 182/984.
lattice. The stabilisation of poly[dihalocuprate( )] anions by
I
large phosphonium cations has been documented,10,11 but the
only stibonium salt involving a related anion is that of the
copper(II) complex, (SbPh4)2·Cu2Cl6.12 However the Cu–Cu
separation in this structure is much greater (3.394 Å) than that
1 J. Chatt and F. G. Mann, J. Chem. Soc., 1940, 1192; G. Doak and L. D.
Freedman, Organometallic Compounds of Arsenic, Antimony, and
Bismuth, Wiley Interscience, 1970, and references therein.
2 D. W. Allen, P. E. Cropper, P. G. Smithurst, P. R. Ashton and B. F.
Taylor, J. Chem. Soc., Perkin Trans. 1, 1986, 1989; D. W. Allen, I. W.
Nowell, L. A. March and B. F. Taylor, J. Chem. Soc., Perkin Trans. 1,
1984, 2523; D. W. Allen and P. E. Cropper, Polyhedron, 1990, 9,
129.
3 N. R. Champness and W. Levason, Coord. Chem. Rev., 1994, 133, 115;
G. A. Bowmaker, R. D. Hart, E. N. de Silva, B. W. Skelton and A. H.
White, Aust. J. Chem., 1997, 50, 553; G. A. Bowmaker, R. D. Hart and
A. H. White, Aust. J. Chem., 1997, 50, 567.
in the di-iodocuprate(
with other di-iodocuprate(
I
) counter-ion discussed here. Comparison
I
) anions crystallizing in the same
manner shows the Cu–Cu separation to be somewhat greater
than in our example (average = 2.95 Å).13,14
Treatment of the salts 2 (E = As or Sb; Ar = Ph; X = Cl, Br,
or Ph), dissolved in dichloromethane, with aqueous sodium
hydroxide solution, resulted in a marked colour change from
yellow to red-purple with formation of the related betaines 5,
4 D. W. Allen, J. P. L. Mifflin, M. B. Hursthouse and K. M. A. Malik, to
be published.
5 D. W. Allen and P. E. Cropper, J. Organomet. Chem., 1992, 435,
203.
X
O–
6 R. J. Cernik, W. Clegg, C. R. A. Catlow, G. Bushnell-Wye, J. V.
Flaherty, G. N. Greaves, I. D. Burrows, D. J. Taylor, S. J. Teat and M.
Hamichi, J. Synchrotron Rad., 1997, 4, 279.
CH
N
X
7 A. Bondi, J. Phys. Chem., 1964, 68, 441.
8 G. Ferguson, C. Glidewell, D. Lloyd and S. Metcalfe, J. Chem. Soc.,
Perkin Trans. 2, 1988, 731.
+
EAr3
5
9 L-J. Baker, C. E. F. Rickard and M. J. Taylor, J. Chem. Soc., Dalton
Trans., 1995, 2895.
10 S. Andersson, M. Hakansson and S. Jagner, Inorg. Chim. Acta, 1993,
209, 195.
11 A. Pfitzner and D. Schmitz, Z. Anorg. Allg. Chem., 1997, 623, 1555.
12 A. Bencini, D. Gatteschi and C. Zanchini, Inorg. Chem., 1985, 24,
704.
13 H. Hartl, I. Brudgam and F. Mahdjour-Hassan-Abadi, Z. Naturforsch.,
Teil B, 1985, 40, 1032.
14 M. Hofer and H. Hartl, Z. Anorg. Allg. Chem., 1992, 45, 612.
15 D. W. Allen and X. Li, J. Chem. Soc., Perkin Trans. 2, 1997, 1099
16 C. Lambert, S. Stadler, G. Bourhill and C. Brauchle, Angew. Chem., Int.
Ed. Engl., 1996, 35, 644.
17 C. Lambert, E. Schmalzlin, K. Meerholz and C. Brauchle, Chem. Eur.
J., 1998, 4, 512.
which were subsequently isolated and purified by trituration
with diethyl ether. Again, 1H and 13C NMR spectra were
consistent with the proposed structures, showing some sig-
nificant chemical shift changes compared to the parent salts.
Under FABMS conditions, cationic molecular ions were again
observed. Conversion to the betaines resulted in a significant
shift of the visible absorption maximum to longer wavelength.
Thus, e.g. lmax for the salt 2 (E = Sb; Ar = Ph; X = Cl, Y =
CuI2) in dichloromethane was observed at 358 nm, whereas for
the related betaine 5 in the same solvent, lmax = 536 nm.
Significantly, in view of the potential link with non-linear
optical properties, the betaines exhibited negative solvatochro-
mism, the visible absorption maximum moving to longer
wavelength on moving to a solvent of lower polarity. In the case
of the above betaine, lmax moved from 536 nm in dichloro-
Received in Cambridge, UK, 23rd July 1998; 8/05759A
2116
Chem. Commun., 1998