Synthesis of [Ag{NCAgCN}({(o-MeOC6H4O)P(l-NtBu)-
jP}2)2]∞ (4). A mixture of 1 (196 mg, 0.44 mmol) and AgCN
(58.4 mg, 0.44 mmol) in acetonitrile (25 cm3) was stirred under
reflux conditions for 6 h. The reaction mixture was cooled to
room temperature, concentrated to 10 cm3 under reduced pressure
and stored at −30 ◦C for a day to give a white crystalline product
(226 mg, 89%). Mp 110–112 ◦C. C23H32N3O4P2Ag (584.3): calcd C
47.27, H 5.51, N 7.19; found: C 47.32, H 5.47, N 7.47%. IR (KBr
Acknowledgements
We are grateful to the Department of Science and Technology
(DST), New Delhi for funding through grant SR/S1/IC-05/2003.
PC thanks CSIR for Research Fellowship. JTM thanks the
Louisiana Board of Regents through grant LEQSF(2002-03)-
ENH-TR-67 for purchase of the Bruker APEX CCD diffrac-
tometer and the Chemistry Department of Tulane University for
support of the X-ray laboratory.
1
disk, cm−1): 2143 [m(C≡N)]. H NMR (400 MHz, acetone-d6):
dH = 7.35–6.89 (m, 8 H, Ph), 3.86 (s, 6 H, OMe), 1.44 (s, 18 H,
1
tBu) ppm. 31P{ H} NMR (161 MHz, acetone-d6): dP = 137.2 (br
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X-Ray crystallography
Crystals of 2 and 4 were mounted in a Cryoloop with a drop
of Paratone oil and placed in the cold nitrogen stream of the
Kryoflex low temperature attachment of a Bruker Smart APEX
CCD diffractometer. Full spheres of intensity data were collected
as follows: for 2, three sets of 400 scans in x (0.5◦ per scan at
u = 0, 90 and 180◦) and two sets of 800 scans in u (0.45◦ per
scan at x = −30 and 210◦); for 4, three sets of 606 scans in
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collected using the SMART software package16 and these were
reduced to F2 values with the SAINT+ software17 which also
performed a global refinement of unit cell parameters using 7372
(for 2) and 8660 (for 4) reflections chosen from the full data set.
The crystal of 2 proved to be twinned and the integration of
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of SAINT+ using the two-component orientation file prepared
by CELL_NOW18 and with the cell parameters of the second
domain on the twin constrained to be identical to those of the
first domain. Multiple measurements of equivalent reflections
provided a basis for empirical absorption corrections (using the
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group 222 but with the exclusion of those reflections for which
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structures were solved by direct methods and refined by full-
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suite.21 For 2, the small size of the crystal resulted in there
being little useful diffraction data beyond 2h = 49.2◦ so with a
limited amount of high order data it was not feasible to carry
out a refinement of the light atoms with unrestricted anisotropic
displacement parameters. Instead, they were restrained to approx-
imate isotropic behavior. In the case of 4, two of the tert-butyl
groups are rotationally disordered over two resolved sites while
one of the P–O–R groups is also disordered. All three disordered
groups were refined subject to restraints that they approximate
idealized geometries. Details of the disorder are provided in the
CIF. Hydrogen atoms were placed in calculated positions (C–H =
˚
˚
0.95 A (aromatic rings) and 0.98 A (methyl groups)) and included
as riding contributions with isotropic displacement parameters
1.2 (aromatic) or 1.5 (methyl) times those of the attached carbon
atoms.
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CCDC reference numbers 641238 (2) and 641239 (4). For
crystallographic data in CIF or other electronic format see DOI:
10.1039/b704303a
This journal is
The Royal Society of Chemistry 2007
Dalton Trans., 2007, 2957–2962 | 2961
©