M. Gorlov, A. Fischer, L. Kloo
Table 1 Crystallographic data and results of the structure determi-
nations of Pd[GaBr4]2 and Pd[GaI4]2.
Table 3 Selected bond lengths/pm and angles/deg in the structures
of 1 and 2
Pd[GaBr4]2
Pd[GaI4]2
Pd[GaBr4]2
Pd[GaI4]2
Lattice constants
aϭ1267(2) pm
bϭ808(1) pm
cϭ722(1) pm
βϭ94.5(1)°
736(2)
4.00
885.1
aϭ1363(1) pm
bϭ849.9(4) pm
cϭ756.6(7) pm
βϭ95.38(3)°
873(1)
4.80
1261.1
Pd Ϫ Br(1)
246.0(3)
242.9(3)
228.7(4)
227.5(4)
242.9(3)
89.1(1)
90.9(1)
90.5(2)
113.0(1)
111.2(1)
Pd Ϫ I(1)
261.2(2)
262.0(3)
249.0(4)
246.5(4)
262.0(3)
90.8(1)
89.2(1)
90.4(1)
113.1(1)
111.3(1)
115.1(1)
Gaiii Ϫ Br(1i)
Gaiii Ϫ I(1i)
Gaiii Ϫ Br(2iii)
Gaiii Ϫ I(2iii)
Gaiii Ϫ Br(3iii)
Gaiii Ϫ I(3iii)
Cell volume/106 pm3
Density(cal.)/g·cmϪ3
Formula weight
Number of formula units
Crystal system, space group
Temperature
Gaiii Ϫ Br(1iii)
Gaiii Ϫ I(1iii)
Br(1) Ϫ Pd Ϫ Br(1iii)
Br(1i) Ϫ Pd Ϫ Br(1iii)
Br(1i) Ϫ Ga Ϫ Br(1iii)
Br(1i) Ϫ Ga Ϫ Br(2iii)
Br(1i) Ϫ Ga Ϫ Br(3iii)
I(1) Ϫ Pd Ϫ I(1iii)
I(1i) Ϫ Pd Ϫ I(1iii)
I(1i) Ϫ Ga Ϫ I(1iii)
I(1i) Ϫ Ga Ϫ I(2iii)
I(1i) Ϫ Ga Ϫ I(3iii)
I(2iii) Ϫ Ga Ϫ I(3iii)
2
monoclinic, C2/m (No. 12)
299 K
299 K
Bruker-Nonius KappaCCD
Ag-Kα, λϭ56.085 pm
Diffractometer
Br(2iii) Ϫ Ga Ϫ Br(3iii) 115.4(2)
Radiation
Absorption coefficient/cmϪ1
θmax
141.4
21.4
96.1
19.0
the bromogallate was used as starting model for refinement. All
atoms were refined on F2 using anisotropic thermal parameters
for all atoms [18]. Table 1 summarizes the results of the structure
determinations, Table 2 the atomic positions and Table 3 selected
bond lengths.
no. of reflections
1888
606, 0.067
433
2043
528, 0.062
411
no. of independent reflections, Rint
no. of reflections with I>2σ(I)
number of parameters
R(obs. reflections)
R(all reflections)
wR2
GooF
32
32
0.0428
0.0712
0.0997a)
1.133
0.0358
0.0551
0.0824b)
1.136
Further details of the crystal structure investigations can be ob-
tained from the Fachinformationszentrum Karlsruhe, 76344 Eg-
genstein-Leopoldshafen, Germany, (Fax: ϩ49(7247)808-666, e-
mail: crysdata@fiz-karlsruhe.de) on quoting the depository num-
bers CSD-413 229 (Pd[GaBr4]2) and CSD-413 230 (Pd[GaI4]2).
largest difference peaks
0.66/Ϫ0.92
0.85/Ϫ0.85
a) wϭ[σ2Fo2ϩ(0.0208P)2 ϩ 10.6 P]Ϫ1 where Pϭ(Fo2ϩ2Fc2)/3
b) wϭ[σ2Fo2ϩ(0.0277P)2 ϩ 16.2 P]Ϫ1 where Pϭ(Fo2ϩ2Fc2)/3
Table 2 Atomic positions and isotropic displacement parameters B/
104 pm2 of the atoms in the structure of Pd[GaBr4]2 and Pd[GaI4]2.
Standard deviations are given in parentheses.
References
[1] H.-U. Blaser, A. Indolese, A. Schnyder, H. Steiner, M. Studer,
J. Mol. Cat. 2001, 173, 3.
atom
Wyckoff
position
x
y
z
B
[2] D. A. Atwood, Coord. Chem. Rev. 1998, 176, 407.
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69, 2067.
Pd[GaBr4]2:
Pd
Ga
Br(1)
Br(2)
Br(3)
2a
4i
8j
4i
4i
0
0
0
0
3.36(4)
3.69(4)
4.36(3)
5.80(6)
5.60(5)
0.2108(2)
0.1155(1)
0.1660(2)
0.3876(2)
0.3319(2)
0.1507(2)
0.6329(3)
0.2957(3)
0.2136(2)
0
0
Pd[GaI4]2:
Pd
Ga
I(1)
I(2)
[7] L. Werner, H. Schaefer, H. U. Huerter, B. Krebs, Z. Anorg.
Allg. Chem. 1981, 482, 19.
[8] M. Gorlov, A. Fischer, L. Kloo, Inorg. Chim. Acta. 2003,
350, 449.
2a
4i
8j
4i
4i
0
0
0
0
2.31(5)
2.68(5)
3.03(3)
4.09(4)
3.92(4)
0.2087(2)
0.11461(7)
0.1609(1)
0.3877(1)
0.3397(3)
0.1477(1)
0.6490(2)
0.3135(2)
0.2184(1)
0
0
I(3)
[9] K. Brodersen, G. Thiele and H. Gaedcke, Z. Anorg. Allg.
Chem. 1966, 348, 162.
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101, 2771.
Raman spectroscopy
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in press.
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1980, 462, 49.
Raman spectra were recorded with a Bio-Rad FTS 6000 spec-
trometer equipped with a low-power Nd:YAG laser (λ ϭ 1064 nm)
and a liquid-nitrogen-cooled, solid state Ge diode detector. A reso-
lution of 4 cmϪ1 was used.
[15] A. J. M. Duisenberg, Reflections on Area Detectors, Thesis,
Utrecht, The Netherlands, 1998.
Structure determinations
Due to the extreme sensitivity towards humidity, crystals of all
compounds were sealed inside glass capillaries in a dry nitrogen
atmosphere. Diffraction data were collected on a Bruker-Nonius
KappaCCD diffractometer. Crystals of both compound turned out
to be twinned in the same way. The twinning element is a 180°
rotation around (0 0 1). Using EvalCCD, sufficient diffraction data
from one twin domain could be obtained in both cases [15]. Nu-
merical absorption corrections were applied [16]. All atoms could
be located using direct methods [17]. In the case of the iodogallate,
[16] W. Herrendorf, H. Bärnighausen: HABITUS, a program for
numerical absorption correction, Universities of Karlsruhe
and Giessen, Germany, 1997.
[17] G. M. Sheldrick, SHELXS97, a program for crystal structure
solution, University of Göttingen, Germany, 1997.
[18] G. M. Sheldrick, SHELXL97, a program for crystal structure
refinement, University of Göttingen, Germany, 1997.
[19] K. Brandenburg, DIAMOND 2.1e, Crystal Impact GbR,
Bonn, Germany, 2001.
326
2004 WILEY-VCH Verlag GmbH & Co. KGaA, 69451 Weinheim
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Z. Anorg. Allg. Chem. 2004, 630, 324Ϫ326