atom is disordered and thus has two orientations. A disordered
measurements showed a single peak at 6.871 ppm for complex
and a single peak at 6.496 ppm for complex 2. Elemental
analysis for complex 1, C Zn NO : C, 12.20%; H, 1.65%;
N, 3.48%; P, 15.74%. Calcd: C, 12.31%; H, 1.80%; N, 3.59%;
9 3
P, 15.91%. Elemental analysis for complex 2, C Zn NO P :
0
1
model of the zinc atom (Zn1 and Zn1 at 89.6% and 10.4%
occupancies, respectively) resulted in a lower R value (6.56%)
H
4 7
2
8
P
2
1
+
3
+
and a featureless residual (1.246 e A , 0.56 A from C1). The
disordered oxygen atoms, as well as C1 and C2 atoms were
refined with isotropic thermal parameters. All hydrogen atoms
were generated geometrically, assigned fixed isotropic thermal
parameters and included in the structure factor calculations.
Some of the data collection and refinement parameters are
summarized in Table 2. Important bond lengths and angles for
complexes 1 and 2 are listed in Table 1.
H
3 8
2
C, 8.33%; H, 1.74%; N, 3.15%; P, 21.96%. Calcd: C, 8.46%;
H, 1.88%; N, 3.29%; P, 21.84%.
Crystallography
Single crystals of complexes 1 and 2 were mounted on a Bruker
Smart CCD and reflections collected using MoKa radiation
CCDC reference numbers 187598 and 187599. See http:==
www.rsc.org=suppdata=nj=b2=b2020296n= for crystallographic
data in CIF format or other electronic format.
+
(
l ¼ 0.71069 A) and a graphite monochromator at 110(2) K.
The cell constants were indexed from reflections obtained from
0 frames collected with 10 s exposure per frame. A hemi-
sphere of data (1271 frames at 5 cm detector distance) was
6
Acknowledgements
collected by the narrow-frame method with scan widths of
ꢀ
0
.30 in o and exposure time of 30 s per frame. The first 50
We acknowledge with thanks the financial support from the
Robert A. Welch Foundation through Grant No. A673 and
the Department of Energy, Basic Sciences Division, through
Grant No. DOE 448071-00001.
frames were recollected at the end of data collection to assess
the stability of the crystal, and it was found that the decay in
intensity was less than 1%. The data were corrected for
Lorentz factor, polarization, air absorption and absorption
due to variations in the path length through the detector
faceplate. An empirical absorption correction based on the C
scan method was also applied.
References
1
(a) E. Stein, A. Clearfield and M. A. Subramanian, Solid State
Ionics, 1996, 83, 113; (b) G. Alberti and U. Costantino, in Com-
prehensive Suramolecular Chemistry, ed. J. M. Lehn, Pergamon-
Elsevier Science Ltd., London, 1996, p. 1; (c) A. Clearfield, Curr.
Opin. Solid State Mater. Sci., 1996, 1, 268; (d) A. Clearfield, Prog.
Inorg. Chem., 1998, 47, 371 (and references therein).
M. E. Thompson, Chem. Mater., 1994, 6, 1168.
G. Alberti and U. Costantino, in Comprehensive Supramolecular
Chemistry, ed. J. M. Lehn, Pergamon-Elsevier Science Ltd.,
London, 1996, p. 151.
The space group was determined to be either P6 (No. 169)
1
or P6
were solved using direct methods (SHELXTL) in space group
P6 (No. 169) and refined by least-square methods with atomic
coordinates and anisotropic thermal parameters for non-
5
(No. 170) for both complexes 1 and 2. Both structures
1
1
7
2
3
hydrogen atoms. Absolute structure parameters thus refined
are ꢂ0.04(3) and 0.04(3) for complexes 1 and 2, respectively.
5
Refinements of both structures using space group P6 (No.
1
70) resulted in higher final R
1
values (for observed data,
4
(a) B. Zhang and A. Clearfield, J. Am. Chem. Soc., 1997, 119, 2751;
(b) C. V. K. Sharma and A. Clearfield, J. Am. Chem. Soc., 2000,
122, 1558; (c) I. Lukes, J. Kotek, P. Vojtisek and P. Hermann,
Coord. Chem. Rev., 2001, 216–217, 287; (d ) A. Clearfield, D. M.
Poojary, B. Zhang, B. Zhao and A. Derecskei-Kovacs, Chem.
Mater., 2000, 12, 2745.
0
.0573 and 0.0784, for complexes 1 and 2, respectively) and
very large absolute structure parameters [0.738(4) and 0.939(4),
respectively, for complexes 1 and 2]. Hence P6 (No. 169) was
1
used for all refinements of both structures. All atoms in com-
plex 1 are well behaved. However, disorder problems exist for
some atoms in complex 2. An ordered model gave large ther-
mal parameters for Zn1, O1, O5 and O6, and also a residual of
5
6
(a) B. Zhang, D. M. Poojary, A. Clearfield and G.-Z. Peng, Chem.
Mater., 1996, 8, 1333; (b) D. M. Poojary and A. Clearfield,
J. Organomet. Chem., 1996, 512, 237; (c) D. M. Poojary, B. Zhang
and A. Clearfield, Angew. Chem., Int. Ed. Engl., 1994, 33, 2324.
B. Zhang, D. M. Poojary and A. Clearfield, Inorg. Chem., 1998,
37, 249.
+
3
+
3
After splitting O1, O5 and O6 atoms into two orientations (O1,
.5 e A , which is 1.50 A from Zn1. The R
1
was about 8.0%.
0
0
0
O1 , O5, O5 , O6 and O6 ) with 50% occupancy for each site),
the R value was lowered to 7.5%, but the residual around Zn1
7
8
J.-G. Mao and A. Clearfield, Inorg. Chem., 2002, 41, 2319.
S. O. H. Gutschke, D. J. Price, A. K. Powell and P. T. Wood,
Angew. Chem., Int. Ed., 1999, 38, 1088.
1
remained as high as before. Careful examination of the
environment around the residual peak indicate it also had a
tetrahedral geometry. At this point, we realized that the Zn1
9
0
M. Galanski, B. K. Keppler and B. Nuber, Angew. Chem., Int. Ed.
Engl., 1995, 34, 1103.
C. V. K. Sharma and A. Clearfield, J. Am. Chem. Soc., 2000, 122,
1
4
394.
Table 2 Crystal data and structure refinement for complexes 1 and 2
11 C. V. K. Sharma, A. Clearfield, A. Cabeza, M. A. G. Aranda and
S. Bruque, J. Am. Chem. Soc., 2001, 123, 2885.
Complex
1
C
2
C
12 A. Cabeza, X. Ouyang, C. V. K. Sharma, M. A. G. Aranda,
S. Bruque and A. Clearfield, Inorg. Chem., 2002, 41, 2325.
13 (a) D. M. Poojary, B. Zhang and A. Clearfield, J. Am. Chem. Soc.,
1997, 119, 12550; (b) B. Zhang, D. M. Poojary and A. Clearfield,
Inorg. Chem., 1998, 37, 1844; (c) J. G. Mao, Z. Wang and A.
Clearfield, Inorg. Chem., 2002, accepted.
14 (a) Q. Wang, X. Wu, W. Zhang, T. Sheng, P. Lin and J. Li, Inorg.
Chem., 1999, 38, 2223; (b) L. S. White, P. V. Nilsson, L. H.
Pignolet and L. Que Jr., J. Am. Chem. Soc., 1984, 106, 8312; (c) D.
Dakternieks, G. Dyson, R. Tozer and E. R. T. Tiekink, J.
Organomet. Chem., 1993, 458, 29; (d ) S. H. Whitlow, Inorg. Chem.,
1973, 12, 2286.
Empirical formula
M
Crystal system
4
H
7
Zn NO
2
8
P
2
3 8 2 9 3
H Zn NO P
389.79
Hexagonal
P6 (No. 169)
8.0677(12)
27.283(6)
1537.9(5)
6
110(2)
5.021
3597
425.75
Hexagonal
P6 (No. 169)
8.3553(8)
26.657(4)
1611.6(3)
6
110(2)
4.952
9968
Space group
1
1
+
a=A
+
c=A
U=A
+
3
Z
T=K
ꢂ1
m(Mo-Ka)=mm
Reflections collected
Independent reflections
R
1851
0.0764
1380
0.0443
0.0941
0.0686
0.1030
2599
0.0716
2599
0.0656
0.1132
0.0918
0.1269
15 (a) T. Shibahara, H. Hattori and H. Kuroya, J. Am. Chem. Soc.,
1984, 106, 2710; (b) O. P. Gladkikh, T. N. Polynova, M. A. Porai-
Koshits and N. D. Mitrofanova, Koord. Khim., 1990, 16, 758; (c)
N.-H. Dung, B. Viossal, A. Busnot, J. M. G. Perez, S. G. Garcia
and J. N. Gutierrez, Inorg. Chem., 1988, 27, 1227; (d) H. Kobayashi,
T. Shibahara and N. Uryu, Bull. Chem. Soc. Jpn., 1990, 63, 799.
16 W. Clegg, A. K. Powell and M. J. Ware, Acta Crystallogr., Sect. C,
int
Observed reflections [I > 2s(I)]
a
R
1
a
wR [I > 2s(I)]
2
a
1
R (all data)
a
wR
2
(all data)
1
984, 40, 1822.
a
2
2 2
2 2 1=2
) ] }
R
1
¼ SkF j ꢂ jF
o
o
k=SjF
o
j, wR
2
¼ {Sw[(F
o
) ꢂ (F
o
) ] =Sw[(F
o
.
17 G. M. Sheldrick, SHELXTL, Crystallographic Software Package,
version 5.1, Bruker-AXS, Madison, WI, 1998.
1
014
New J. Chem., 2002, 26, 1010–1014