R. Srinivasan, S. Tragl, H.-J. Meyer
fused in evacuated silica tubes and heated in a commercial (Carbol-
ite) furnace up to temperatures between 500 and 650 °C, using
heating and cooling durations of about 24 h.
Table 1 Crystallographic details and structure refinement data of
La O(CN ) .
2 2 2
Space group (no.), Z
Unit cell dimension (in A)
C2/c (15), 4
La
Li
from La
limed) [15]. LaOCl was synthesized according to [6], and Li
2
O(CN
(CN ). LaCl
(Ventron, 99.9 %) and NH
2
)
2
was synthesized from mixtures of LaCl
was obtained by the ammonium chloride route
Cl (Merck, 99.8 %, sub-
2
(CN )
3
, LaOCl, and
˚
a ϭ 13.530(2), b ϭ 6.250(1),
c ϭ 6.1017(9), β ϭ 104.81(2)°
498.9(1)
4.978
373.88
transparent colourless, needle shaped
0.1 x 0.04 x 0.04
STOE, IPDS
2
2
3
˚
3
O
3
4
Cell volume (in A )
2
Density calc. (in g cmϪ3)
Molecular weight (in g·molϪ1)
Crystal appearance
2
was synthesized as described in [4]. The purity of all phases was
controlled by X-ray powder diffraction.
3
Crystal size (in·mm )
Diffractometer
Radiation, Temperature
α
Mo-K (λ ϭ 71.073 pm),
graphite monochromator, 293(2) K
Synthesis of La O(CN )
2
2 2
Range: θ
Range: h, k, l
Data correction
µ (in mm
Unique reflections
Collected reflections
0 0
(F > 2σ(F ))
Parameters refined
R indices (all data)
Final R indices [I > 2σ(I)]
GooF (all reflections)
Res. peak: max.; min. (in e/A ) 3.17; Ϫ1.19
5.27 to 30.35°
Ϫ19 Յ h Յ 19, Ϫ8 Յ k Յ 8, Ϫ8 Յ l Յ 8
La
2
O(CN
2
)
2
was first obtained as a minor phase, when mixtures
Lorentz, polarisation and absorption
16.78
734
Ϫ1
with different stoichiometries of LaCl
in silica ampoules at 500Ϫ650 °C. The oxygen contamination may
have been due to water or oxygen impurities of the employed LaCl
or from the wall of the silica tube. Yields were increased, when
oxygen sources were introduced into the reaction externally. There-
3
and Li
2
(CN
2
) were reacted
)
4289
3
42 (all atoms refined anisotropically)
R1 ϭ 0.0283, wR2 ϭ 0.0679
R1 ϭ 0.0266, wR2 ϭ 0.0671
1.141
a)
a)
fore, a homogeneous mixture of LaCl
reacted in a 1:1:2 molar ratio at 650 °C and yielded a light brown
powder, later known to be La O(CN , besides LiCl.
3 2 2
, LaOCl, and Li (CN ) was
˚
3
2
2 2
)
a)
2ϪF
2)2 / (Σw(F
2 2 1/2
R1 ϭ ΣʈF
o
Η Ϫ ΗF
c
ʈ / ΣΗF
o
Η; wR2 ϭ [Σw(F
o
c
o
) )]
LaCl
3
ϩ LaOCl ϩ 2 Li
2
(CN
2
) Ǟ La
2
O(CN
2
)
2
ϩ 4 LiCl
(1)
Table 2 Atomic coordinates and isotropic-equivalent displacement
parameters (in A ) for La O(CN ) .
2 2 2
La O(CN )
2
2 2
appeared quite stable against air and water, so that
˚
2
water could even be used to wash off LiCl from the product.
In a separate attempt, the same mixture (total mass: 225 mg) was
combined with a LiCl-KCl mixture (29 mg) and reacted similarly
as in reaction (1). The mixture was heated in a sealed copper am-
poule at 600 °C for ten days before being cooled down slowly to
a
Atom
Wyckoff
position
x
y
z
U
eq
La1
O1
N1
N2
C1
8 f
4 e
8 f
8 f
8 f
0.10072(2)
0
0.2915(3)
0.0923(3)
0.1530(3)
0.21443(3)
0.0260(6)
0.3423(7)
0.6174(6)
0.2739(6)
0.07542(4)
0.0096(1)
0.0118(8)
0.0143(6)
0.0133(7)
0.0111(8)
3
/
4
0.2473(6)
0.9698(6)
0.6112(8)
300 °C first and then to room temperature. From this reaction well
developed needle-shaped colourless crystals were grown and after-
wards selected for X-ray single crystal diffraction studies.
a
U
eq is defined as one-third of the trace of the orthogonalized Uij tensor.
X-ray Diffraction
˚
Table 3 Bond lengths (in A) and N-C-N bond angle (in °) in
La O(CN ) .
2 2 2
All phase analyses were done by X-ray powder diffraction. The
powder patterns were recorded on a StadiP diffractometer (STOE,
Darmstadt), using germanium monochromated Cu-Kα1 radiation
La1ϪO1
La1ϪO1
La1ϪN1
La1ϪN1
La1ϪN1
La1ϪN2
2.409(2)
2.448(2)
2.650(4)
2.756(3)
2.811(4)
2.595(4)
La1ϪN2
La1ϪN2
C1ϪN1
C1ϪN2
N1ϪC1ϪN2
2.655(3)
2.762(4)
1.227(6)
1.233(6)
176.1(5)
˚
(
λ ϭ 1.540598 A) and a position sensitive X-ray detector (opening
angle: 2θ ϭ 6°). The powdered samples of La O(CN were
2
2 2
)
washed in ethanol, dried overnight, and placed in between two my-
lar foils for the X-ray powder pattern measurement. Routine analy-
ses were done in the 2θ range between 10 and 60°. As a new struc-
ture was evident from the powder pattern, a measurement in the
2
θ range of 5Ϫ130° was performed with step increments of 0.2°
Some crystallographic data and measurement parameters are pro-
vided in Table 1. The atomic positions along with the isotropic-
equivalent displacement parameters are given in Table 2. Selected
bond distances and the N-C-N bond angle are shown in Table 3.
Details on the crystal structure investigations can be obtained from
the Fachinformationszentrum Karlsruhe, Germany, D-76344 Egg-
enstein-Leopoldshafen (fax: (ϩ49)7247-808-666; e-mail: crysdat-
a@fiz-karlsruhe.de) on quoting the depository number 391255 for
and exposure periods of 120 seconds. The powder pattern was inde-
xed using Louer’s algorithm (DICVOL) consistent with a C-centred
monoclinic cell (a ϭ 13.507(2) A, b ϭ 6.2432(9) A, c ϭ 6.1002(7) A,
β ϭ 104.833(8)°, V ϭ 497.3(2) A ) for 75 selected peaks. The com-
position of the title compound was first derived from a Rietveld
˚
˚
˚
˚
3
2 2 2
refinement. The refined composition of La O(CN ) was the key
information for the straight forward synthesis. In favour of the bet-
ter accuracy, we here present the single crystal structure refinement
studies only.
2 2 2
La O(CN ) .
2 2 2
Suitable colourless transparent single crystals of La O(CN ) were
selected under a microscope and mounted on the tips of glass fibres
for X-ray diffraction studies. Single crystal measurements were per-
Results and Discussion
formed on an IPDS (STOE, Darmstadt) X-ray diffractometer
As La
O (CN ) is known for a long time, the new La2-
2 2 2
˚
α
using graphite monochromated Mo-K radiation (λ ϭ 0.71073 A).
O(CN ) represents the second composition in this system.
2
2
720
© 2005 WILEY-VCH Verlag GmbH & Co. KGaA, 69451 Weinheim
zaac.wiley-vch.de
Z. Anorg. Allg. Chem. 2005, 631, 719Ϫ722