Nt = 31495, N = 8234 (Rint = 0.025), No = 6797; R1(F) = 0.029,
wR2(F2) = 0.062 (A = 0.062, B = 0).
[M(2)(NO3)2]·2CH3OH C34H44N6O10M (M = Co, Zn, Cd).
Monoclinic, space group P21/n (C52h, No.14 (variant)), Z = 4
(x,y,z,Uiso)H refined for the Co, Cd adducts.
(i) [Co(2)(NO3)2]·2CH3OH. M = 755.7. a = 17.586(2), b =
9.1457(8), c = 23.063(2) Å, b = 100.249(2)°, V = 3480 Å3. Dc =
1.442 g cm−3. lMo = 5.6 cm−1; specimen: 0.30 × 0.14 × 0.11 mm;
‘T’min/max = 0.95. 2hmax = 58°; Nt = 64342, N = 9231 (Rint = 0.043),
No = 7094; R = 0.042, Rw = 0.048.
[Ni(3)](NO3)2·H2O C32H38N6NiO10, M = 709.4. Monoclinic,
space group P21/n, a = 11.013(4), b = 23.351(9), c = 12.836(5) Å,
b = 91.737(12)°, V = 3300 Å3. Dc (Z = 4) = 1.424 g cm−3. lMo
=
6.5 cm−1; specimen: 0.45 × 0.42 × 0.41 mm; ‘T’min/max = 0.90.
2hmax = 56.6°; Nt = 32067, N = 7807 (Rint = 0.018), No = 7274;
R1(F) = 0.074, Rw(F2) = 0.019 (A = 0.005, B = 8).
Variata. Difference map residues were modelled in terms of a
disordered water molecule oxygen, associated hydrogen atoms
not being located. The nitrate moieties also exhibit significant
disorder, the components being modelled as rigid bodies.
[Ni(5)](NO3)2·3CH3OH C42H54N6NiO11, M = 877.6.
Triclinic, space group P1, a = 9.498(1), b = 11.094(2), c =
21.743(3) Å, a = 92.006(3), b = 95.444(3), c = 111.507(3)°, V =
2116 Å3. Dc (Z = 2) = 1.378 g cm−3. lMo = 5.3 cm−1; specimen:
0.38 × 0.14 × 0.11 mm; Tmin,max (Gaussian correction) = 0.84,
0.95. 2hmax = 56.7°; Nt = 21470, N = 9931 (Rint = 0.034),
No = 8015; R1(F) = 0.035, wR2(F2) = 0.080 (A = 0.03, B = 0).
(ii) [Zn(2)(NO3)2]·2CH3OH. M = 762.2. a = 17.637(4), b =
9.133(2), c = 23.161(4) Å, b = 110.049(6)°, V = 3505 Å3. Dc =
1.444 g cm−3. lMo = 7.7 cm−1; specimen: 0.14 × 0.10 × 0.09 mm;
‘T’min/max = 0.85. 2hmax = 55°; Nt = 12819 (hemisphere), N = 8070
(Rint = 0.067), No = 5492; R = 0.055, Rw = 0.070.
(iii) [Cd(2)(NO3)2]·2CH3OH. M = 809.2. a = 17.693(2),
b = 9.338(1), c = 22.992(3) Å, b = 109.128(3)°, V = 3589 Å3.
Dc = 1.497 g cm−3. lMo = 6.7 cm−1; specimen: 0.28 × 0.18 ×
0.12 mm; ‘T’min/max = 0.87. 2hmax = 75°; Nt = 46795, N = 17963
(Rint = 0.033), No = 13449; R = 0.038, Rw = 0.047.
[Ag(2)]BF4 C32H36AgBF4N4O2, M = 703.3. Monoclinic,
space group P21/c (C52h, No.14), a = 9.427(1), b = 16.268(2),
c = 20.346(3) Å, b = 101.348(5)°, V = 3059 Å3. Dc (Z = 4) =
1.527 g cm−3. lMo = 7.2 cm−1; specimen: 0.35 × 0.18 × 0.11 mm;
‘T’min/max = 0.87. 2hmax = 60°; Nt = 38639, N = 8774 (Rint = 0.048),
No = 6659; R = 0.049, Rw = 0.061.
Computational study
The DFT computations were performed with the Amsterdam
Density Functional 1999.02 (ADF)17 program package on
a Silicon Graphics Origin 2000 computer (56 MIPS R10000
64-Bit CPU with 195 MHz and 17 GB Memory). All struc-
tures were optimised without imposing symmetry constraints.
The molecular orbitals were expanded in an uncontracted set
of Slater-type orbitals (STO’s) containing diffuse functions.
The basis is of triple-zeta quality, augmented with one or two
polarisation functions. The cores were treated by the frozen-
core approximation.18 The numerical integration was performed
using the procedure developed by Baerends et al.19 The Becke–
Perdew (BP86) functional was used for the calculations, this
uses Becke’s20 gradient correction for the local expression of the
exchange energy and Perdew’s21 gradient correction for the local
expression of the correlation energy. The convergence criteria for
the geometry optimisations, which use analytical derivatives,22
were set to 1 × 10−3 hartree for the changes in energy, 1 × 10−3
hartree Å−1 for the energy gradient, 1 × 10−3 Å for the changes
between old and new bond lengths, and 0.3° for changes in bond
and dihedral angles. All stationary points on the hypersurface
were characterised as true minima by frequency analysis.
[Ag(4)]PF6 C39H42AgF6N4O2P, M = 851.6. Monoclinic,
space group P21/c, a = 10.362(1), b = 17.501(3), c = 20.358(3) Å,
b = 90.094(2)°, V = 3692 Å3. Dc (Z = 4) = 1.532 g cm−3. lMo
=
6.6 cm−1; specimen: 0.30 × 0.15 × 0.10 mm; ‘T’min/max = 0.89.
2hmax = 58°; Nt = 43278, N = 9393 (Rint = 0.032), No = 7121;
R = 0.040, Rw = 0.049.
Variata. The anion was modelled as rotationally disordered
about the PF(1,2) line, F(3–6) modelled over two sets of sites,
occupancies refining to 0.816(5) and complement. Disorder is
also observed in the cation, the silver atom being modelled over
two sets of sites, occupancies refining to 0.9081(7) and comple-
ment; no associated components of disorder in the ligand were
resolvable.
[Ag(5)]BF4 C39H42AgBF4N4O2, M = 793.5. Triclinic,
space group P1 (C1i, No. 2), a = 10.807(2), b = 11.020(2),
c = 16.153(2) Å, a = 73.702(2), b = 78.784(2), c = 72.043(2)°,
V = 1744 Å3. Dc (Z = 2) = 1.511 g cm−3. lMo = 6.4 cm−1;
specimen: 0.13 × 0.10 × 0.065 mm; ‘T’min/max = 0.87. 2hmax = 53°;
Nt = 16914, N = 7069 (Rint = 0.032), No = 5778; R = 0.042,
Rw = 0.048.
Syntheses
[Ag(6)]PF6·CH3CN C46H48AgF6N4O2P·CH3CN, M = 982.8.
Monoclinic, space group P21/c, a = 15.995(2), b = 16.038(2),
c = 17.855(3) Å, b = 95.680(2)°, V = 4558 Å3. Dc (Z = 4) =
1.432 g cm−3. lMo = 5.5 cm−1; specimen: 0.80 × 0.22 × 0.04 mm;
The syntheses of 110,23 have been described previously.
Cobalt(II), nickel(II), zinc(II), and cadmium(II) nitrate com-
plexes of 2. The required hydrated metal(II) nitrate in methanol
(1.31 mL, 0.200 M) was added to a solution of 2 in methanol
(3.00 mL, 0.0872 M). The respective solutions were filtered
and crystallisation of the corresponding metal complexes were
induced by diffusion of diethyl ether vapour into each solution.
In each case, the product was removed by filtration and dried
under vacuum over phosphorus pentoxide. In most instances, in
separate experiments, crystals suitable for X-ray crystallography
were grown by slow diffusion of diethyl ether vapour into a
methanol or acetonitrile solution of the respective complexes.
‘T’min/max = 0.87. 2hmax = 58°; Nt = 53765, N = 11682 (Rint
=
0.039), No = 8704; R = 0.039, Rw = 0.043. (x,y,z,Uiso)H (ligand)
were refined.
[Cu(6)(OH)]PF6·2H2O C46H49CuF6N4O3P·2H2O, M =
15
2h
950.5. Orthorhombic, space group Pbca (D , No. 61) a =
16.347(4), b = 20.768(5), c = 24.865(6) Å, V = 8442 Å3. Dc
(Z = 8) = 1.496 g cm−3. lMo = 6.4 cm−1; specimen: 0.38 ×
0.32 × 0.10 mm; ‘T’min/max = 0.81. 2hmax = 50°; Nt = 55561, N =
7400 (Rint = 0.075), No = 5000; R = 0.068, Rw = 0.095.
Variata. Difference map residues were modelled in terms of
oxygen atoms, tentatively assigned as hydroxide (coordinated)
or (lattice) water; associated hydrogen atoms were not resolved.
The following determinations were undertaken with the
following general variations in procedure: the refinement was
executed using SHELXL-97,16 Gaussian absorption correction
being applied in two instances, as indicated; reflection weights
[Co(2)(NO3)2]·0.5CH3OH·0.5H2O. Yield 52% [Found
(CoLNO3)+, m/z 629.1 (ES) C32H36CoN5O5 requires 629.2]
(Found:C,54.2;H,5.4;N,11.8.Calc.forC32H36CoN6O8·0.5CH3-
OH·0.5H2O:C, 54.47; H, 5.49; N, 11.73%).
2
were (r2(Fo ) + AP2 + BP)−1, P = (Fo2 + 2Fc2)/3 (A,B cited
[Ni(2)(NO3)2]·CH3OH·3H2O. Yield 62% [Found (NiL −
H)+, m/z 565.3 (ES) C32H35N4NiO2 requires 565.2] (Found: C,
51.2; H, 6.1; N, 10.8. Calc. for C32H36N6NiO8·CH3OH·3H2O: C,
50.98; H, 5.96; N, 10.81%).
below). R1(F), wR2(F2) are quoted.
[Ni(2)(NO3)2]·CH3CN·H2O C34H41N7NiO9, M = 750.5.
Monoclinic, space group P21/n, a = 18.416(4), b = 8.693(2),
c = 23.139(5) Å, b = 109.485(4)°, V = 3492 Å3. Dc (Z = 4) =
1.427 g cm−3. lMo = 6.2 cm−1; specimen: 0.33 × 0.31 × 0.22 mm;
Tmin,max (Gaussian correction) = 0.80, 0.89. 2hmax = 56.5°;
[Zn(2)(NO3)2]·1.5CH3OH·2.5H2O. Yield 43% [Found
(ZnL − H)+, m/z 571.3 (ES) C32H35N4O2Zn requires 571.2]
D a l t o n T r a n s . , 2 0 0 4 , 3 7 1 5 – 3 7 2 6
3 7 1 7