Fig. 3 Ball–and–stick representations of the X–ray structure of the cationic
4+ 9
rectangle [3] . There is a crystallographic inversion centre at the centre of
the rectangle. Top view (A) shows the cationic tetramer with a basic
numbering scheme. Bottom view (B) shows an edge-on view with four
closest anions of the intervening layers. Selected distances (Å) and angles
+
Fig. 4 An illustration (left) of [Ag(1)] units linked head-to-tail into a 1D
polymer. A ball-and-stick representation (right) of the X–ray structure of the
n+
1
D helical polymer {[4]}
n
Selected distances (Å) and angles (°):
(°): Ag(1)…Ag(1)A 11.22, Ag(2)…Ag(2)A 5.87, Ag(1)…Ag(2) 6.34,
Ag(1)…Ag(1)A 6.02, Ag(1)–N(1) 2.347(3), Ag(1)–N(2) 2.204(3), Ag(1)–
N(3) 2.374(3), Ag(1)–O(1) 2.468(3), Ag(1)–O(2) 2.810(3), N(1)–Ag(1)–
N(2)A 134.4(1), N(1)–Ag(1)–N(3) 70.0(1), N(2)A–Ag(1)–N(3), 126.6(1)
N(1)–Ag(1)–O(1) 90.4(1), N(2)A–Ag(1)–O(1) 129.4(1), N(3)–Ag(1)–O(1)
4.8(1), N(1)–Ag(1)–O(2) 110.3(1), N(2)A–Ag(1)–O(2) 89.7(1), N(3)–
Ag(1)–O(2) 130.5(1), O(1)–Ag(1)–O(2) 46.3(1).
Ag(1)…Ag(2)A 6.33, Ag(1)–N(2) 2.423(5), Ag(1)–N(3) 2.335(5), Ag(1)–
N(5) 2.378(5), Ag(1)–N(6) 2.413(5), Ag(2)–N(1) 2.203(5), Ag(2)–N(4)
2
.206(5), N(2)–Ag(1)–N(3) 69.5(2), N(2)–Ag(1)–N(5) 110.5(2), N(2)–
Ag(1)–N(6) 154.2(2), N(3)–Ag(1)–N(5) 174.9(2), N(3)–Ag(1)–N(6)
08.7(2), N(5)–Ag(1)–N(6) 69.0(2), N(1)–Ag(2)–N(4)A 171.7(2).
8
1
not possible to form a strictly square planar [M(2,2A-bipy)
2
]n+
(
2402 reflections, I > 2sI), R
= 1.134. {[3][CF SO ]} : C40
P-1, a = 10.127(1), b = 10.453(1), c = 13.504(2) Å, a = 81.403(2), b =
2
= 0.2352, wR
2
= 0.2396, (all data), GoF(F2)
4 12 12 12 4
F N O S , M = 1656.5, triclinic,
complex without some degree of tetrahedral distortion even
8
3
3
4
H28Ag
when the metal ion strongly prefers this geometry. The linear
two-coordinate geometry at Ag(2) defines the short side of the
3
7
1
wR
2.533(2), g = 89.410(2)°, U = 1347.3(3) Å , T = 293(2) K, Z = 1, m =
rectangle. This Ag…Ag distance is spanned by bridging
2
1
.699 mm , 5794 independent reflections (Rint = 0.0091). R
1
= 0.0486,
= 0.1422,
2
CF
3
SO
3
anions and is probably the reason why a rectangle is
1
= 0.0539, (3834 reflections, I > 2sI), R
2
= 0.1365, wR
AgN
2
preferred with this anion; contacts are Ag(2)…O(6) 2.57,
2
(all data), GoF(F ) = 1.068. {[4][NO
]}
3 n
C
9
H
7
4 3
O , M = 327.1,
Ag(1)…O(2) 2.83, Ag(2)…O(4) 2.59 Å.
1
monoclinic, P2 /n, a = 5.432(2), b = 10.860(5), c = 18.009(8) Å, b =
2
2) with
3
21
Since two different anions (BF
4
and CF
3
SO
3
98.486(6)°, U = 1050.7(8) Å , T = 289(2) K, Z = 4, m = 1.920 mm
4381 independent reflections (Rint = 0.0200). R = 0.0279, wR = 0.0299,
1490 reflections, I > 2sI), R = 0.0741, wR = 0.0764 (all data), GoF(F )
1.085. Data were collected on a Bruker APEX CCD instrument and
,
different shapes and arguably (slightly) different coordinating
abilities gave two very different shaped aggregates it was of
interest to examine the effect of using a coordinating oxyanion
such as nitrate. A compound with a 1+1 metal to ligand ratio was
1
1
2
(
=
2
2
solutions performed using the SHELXTL 5.03 Program Library, Bruker
Analytical Instrument Division, Madison, WI, USA, 1997. CCDC numbers
1
prepared from AgNO
the X-ray structure revealed that for AgNO
formed was a linear 1D helical coordination polymer
[4][NO ]} . Each molecule of ligand 1 propagates an [ML]
chain by alternately chelating and bridging to two different
3
and 1 in MeNO
2
. As shown in Fig. 4(B),
91503, 191504, 191505. See http://www.rsc.org/suppdata/cc/b2/
3
the complex
b206989j/ for crystallographic data in CIF or other electronic format.
{
3
n
n
1 G. H. Swiegers and T. J. Malefetes, Chem. Rev., 2000, 100, 3483.
2 E. Bejan, H. Aït-Haddou, J.-C. Daran and G. G. A. Balavoine, Synthesis,
1996, 1012.
Ag(
Ag(
I
) ions. The remainder of the coordination sphere of each
) ion is occupied by 2 O atoms from a nitrate ion. This
3
H. Aït-Haddou, E. Bejan, J.-C. Daran, G. G. A. Balavoine, F. Berruyer-
Penaud, L. Bonazzola, H. Smaoui-Chaabouni and E. Amouyal, J. Chem.
Soc., Dalton Trans., 1999, 3095.
C. Janiak, L. Uehlin, H-P. Wu, P. Klüfers, H. Piotrowski and T. G.
Scharmann, J. Chem. Soc., Dalton Trans., 1999, 3121.
F. Bodar-Houillon, T. Humbert, A. Marsura, J.-B. Regnouf de Vains, O.
Dusausoy, N. Bouhmaida, N. E. Ghermani and Y. Dusausoy, Inorg.
Chem., 1995, 34, 5205.
I
infinite 1D motif is, of course, one of two alternate ways of
linking 90° corners; the head-to-tail version as illustrated in Fig.
4
5
4
(A).
We thank the Natural Sciences and Engineering Research
Council of Canada for financial support of this research.
6
7
M. Schröder, Coord. Chem. Rev., 2001, 222, 1555.
The mean deviation from a least-squares plane that included all of the
Notes and references
† 1
to assign structure. Only crystalline material was isolated and data crystals
selected randomly from the bulk. Crystal data, {[2][BF ]}
28Ag 12, M = 1407.4, triclinic, P-1, a = 7.841(2), b =
.214(2), c 17.007(3) Å, a 102.984(3), b 94.837(3), g
01.366(3)°, U = 1163.1(4) Å , T = 289(2) K, Z = 1, m = 1.768 mm
067 independent reflections (Rint = 0.0179). R = 0.0712, wR = 0.0724,
H NMR spectra (VT, MeNO
-d
) showed no features that could be used
non-H atoms of the cation was; 0.0927 Å for square [2] and 0.2887 Å
4+
2
3
for rectangle [3]4
+
.
4
4
:
8 A. Hazell, O. Simonson and O. Wernberg, Acta Crystallogr. Sect. C:
Cryst. Struct. Commun., 1986, C42, 1707.
9 Ball-and-stick diagrams were prepared using DIAMOND – Visual
Crystal Structure Information System CRYSTAL IMPACT, Postfach
1251, D-53002 Bonn.
36
C H
4 4 16
B F N
9
1
4
=
=
=
=
,
3
21
1
1
CHEM. COMMUN., 2002, 2484–2485
2485