all instruments being equipped with monochromatic Mo-Kα
radiation, λ = 0.71073 Å. Using a single counter instrument in
2θ–θ scan mode, N unique reflections were measured within
the specified 2θmax limit, No with I > 3σ(I) being considered
‘observed’, Gaussian absorption corrections being applied
(structures 7–11). Data were also measured using a Bruker AXS
CCD instrument (structures 1, 2, 4–6, 12, 13) (2θmax = 58Њ),
Nt(otal) reflections within a full sphere being merged to N unique,
Rint as specified after ‘empirical’/multiscan absorption cor-
rection within the proprietary/preprocessing software, the
‘observed’ criterion applicable being F > 4σ( F ). Anisotropic
thermal parameter forms were refined in a full matrix context
for non-hydrogen atoms, (x, y, z, Uiso)H being constrained at
estimated values. Conventional residuals R, Rw (statistical
weights) on |F| are quoted at convergence. Neutral atom
complex scattering factors were employed within the Xtal 3.4
program system.14 Refinement in almost all determinations was
seriously impeded by disorder/‘thermal motion’/site occupancy
problems and ambiguities. Straightforward refinements are
noted as such! Pertinent results are given in the Figures and
Tables below; individual variations in procedure/difficulties/
idiosyncrasies are cited as ‘variata’. For the room temperature
determinations, 20% displacement ellipsoids are shown, for the
low temperature, 50%. Hydrogen atoms, where shown, have
arbitrary radii of 0.1 Å. Two structure determinations (3, 14)
at Pukyong National University were performed (by BJK)
at room temperature using four-circle diffractometer data
(Mo-Kα radiation), with data collection, cell refinement and
data reduction based on STOE proprietary software, while
the structure solution was obtained with SHELXS 9715 and the
structure refinement performed with SHELXL 97.15
[Cu(L1Ј)(OؒClO2ؒO)](∞|∞)ClO4 3. C8H22Cl2CuN4O8, M = 436.7.
STOE instrument, T ca. 293 K. Monoclinic, space group P21/n
(C52h, no. 14 (variant)), a = 9.567(2), b = 13.745(3), c = 12.562(3)
Å, β = 91.26(3)Њ, V = 1652 Å3, Dc (Z = 4) = 1.756 g cmϪ3
,
µMo = 16.9 cmϪ1, specimen 0.30 × 0.30 × 0.20 mm, ‘T’min,max
0.59, 0.81, N = 3780, No = 2774, R = 0.058, Rw = 0.14,
|∆ρmax| = 0.5 e ÅϪ3
=
.
Variata. The bridging perchlorate was modelled as dis-
ordered over two sites of equal occupancy.
[Cu(L1)Cl]ClO4 4. C9H24Cl2CuN4O4, M = 386.8. CCD
instrument, T ca. 300 K. Orthorhombic, space group Pnma
16
2h
(D , no. 62), a = 11.246(1), b = 9.373(2), c = 15.291(2) Å,
V = 1612 Å3, Dc (Z = 4) = 1.594 g cmϪ3, µMo = 17.0 cmϪ1
,
specimen 0.40 × 0.20 × 0.18 mm; ‘T’min,max = 0.75, 0.91,
Nt = 19214, N = 2235 (Rint = 0.022), No = 1847, R = 0.031,
Rw = 0.040; |∆ρmax| = 0.44 e ÅϪ3
.
Variata. (x, y, z, Uiso)H were refined throughout; the perchlor-
ate was modelled with O(22,23) disordered, site occupancies
0.72(1) and complements.
[H6L2]Cl6.2H2O 5. [(H3N(CH2)2NH2CH2C(Me2)CH2NH2-
CH2)2]Cl6ؒ2H2O ≡ C16H50Cl6N6O2, M = 571.3. CCD instrument,
T ca. 153 K. Monoclinic, space group P21/c , a = 7.0501(8),
b = 18.946(2), c = 11.005(1) Å, β = 105.383(1)Њ, V = 1417 Å3, Dc
(Z = 2) = 1.339 g cmϪ3, µMo = 6.3 cmϪ1, specimen 0.45 × 0.35 ×
0.30 mm, ‘T’min,max = 0.65, 0.96, Nt (CCD data) = 15638,
N = 3519 (Rint = 0.028), No = 3181, R = 0.026, Rw = 0.037,
|∆ρmax| = 0.47 e ÅϪ3
.
Variata. Refinement was straightforward, all hydrogen atoms
refining in (x, y, z, Uiso).
Cu(L1)(ClO4)2 ؍
[Cu(L1)(OؒClO2ؒO)](∞|∞)ClO4 1. C9H24Cl2-
CuN4O8, M = 450.8. CCD instrument, T ca. 153 K. Mono-
[{Cu(L3)(OH2)}2Cl][{Cu(L3)}2Cl][ClO4]6 6. C44H116Cl8Cu4-
N16O26, M = 1823.3. CCD instrument, T ca. 300 K. Mono-
clinic, space group C2/c (C62h, no. 15), a = 42.632(3),
b = 9.9729(8), c = 18.659(1) Å, β = 101.365(1)Њ, V = 7778 Å3, Dc
(Z = 4) = 1.557 g cmϪ3, µMo = 14.3 cmϪ1, specimen 0.40 × 0.25 ×
clinic, space group P21/c (C25h
,
no. 14), a = 13.791(1),
b = 9.1815(8), c = 27.573(2) Å, β = 90.524(2)Њ, V = 3491 Å3,
Dc (Z = 8) = 1.715 specimen
cmϪ3 µMo = 16.0 cmϪ1
g
,
,
0.45 × 0.40 × 0.36 mm, ‘T’min,max = 0.51, 0.75, Nt = 51632,
0.20 mm, ‘T’min,max = 0.70, 0.91, Nt = 34329, N = 9754 (Rint
=
N = 13588 (Rint = 0.036), No = 10597, R = 0.049, Rw = 0.059,
0.035), No = 5964, R = 0.043, Rw = 0.047, |∆ρmax| = 0.65 e ÅϪ3
.
|∆ρmax| = 1.6(1) e ÅϪ3
.
Variata. (x, y, z, Uiso) were refined for all hydrogen atoms
except those associated with the water molecule which were
not located. Perchlorates 4,5 were modelled as rotationally
disordered about Cl(n)–O(n1), O(n2–4) having site occupancies
refining to 0.79(1), 0.81(1) and complements respectively.
(These values are so similar that the disorder may be con-
certed.) Three quarters of a sphere of data were measured.
Variata. (x, y, z, Uiso) were refined for all hydrogen atoms.
Anionic perchlorate oxygen atoms (O(42–44)) were modelled as
a pair of rotationally disordered components about Cl–O(41),
site occupancies 0.5; perchlorate 1 within the polymer was
modelled with the coordinated oxygen atoms O(11,12) ordered,
albeit with elongated displacement envelopes, while the remain-
ing ClO2 component was disordered over two sets of sites,
occupancies 0.5. 2θmax was 68Њ. Since there is, not infrequently,
interest in the temperature-dependent behaviour of copper()
structures, we note that in this particular case a preliminary
determination was undertaken at room temperature (T ca. 300
K) (wherein the perchlorate disorder was not resolved). Cu–N
(room, low temperature) did not differ significantly at the
3σ level; Cu–O differed rather more but, even so, by no more
than 0.02 Å. Data for the room temperature determination are
deposited. (Cell dimensions etc.: a = 13.887(1), b = 9.2532(9),
c = 27.778(3) Å, β = 90.634(2)Њ, V = 3569 Å3, R, Rw = 0.052,
0.069 for Nt = 40411, N = 8745 (Rint = 0.023), No = 6577
(2θmax = 58Њ), |∆ρmax| = 0.88(3) e ÅϪ3).
[Co(HL5)(en)Cl]Cl3ؒH2O 7. C9H29Cl4CoN6O, M = 438.1.
Single-counter instrument, T ca. 295 K. Triclinic, space group
1
¯
P1 (Ci, no. 2), a = 11.265(4), b = 10.177(2), c = 8.382(2) Å,
α = 97.91(2), β = 97.51(3), γ = 107.01(2)Њ, V = 895 Å3, Dc
(Z = 2) = 1.625 g cmϪ3, µMo = 15.6 cmϪ1, specimen 0.48 × 0.26 ×
0.41 mm, Tmin,max = 0.52, 0.69, 2θmax = 65Њ, N = 6056, No =
5347, R = 0.031, Rw = 0.041, |∆ρmax| = 1.25 e ÅϪ3
.
Variata. Refinement was straightforward, all hydrogen atoms
refining in (x, y, z, Uiso).
[H8L8]Cl8ؒ7.5H2O 8. C17H67Cl8N8O7.5, M = 787.4. Single
counter instrument, T ca. 295 K. Monoclinic, space group C2/c,
a = 21.636(6), b = 17.446(5), c = 10.360(4) Å, β = 94.82(3)Њ,
[Cu(L1Ј)(OClO3)2] 2. C8H22Cl2CuN4O8, M = 436.7. CCD
instrument, T ca. 153 K. Monoclinic, space group P21 (C 22, no.
4), a = 8.368(1), b = 24.884(4), c = 8.508(1) Å, β = 114.917(3)Њ,
V = 3897 Å3, Dc (Z = 4) = 1.342 g cmϪ3, µMo = 6.2 cmϪ1
,
specimen 0.32 × 0.55 × 0.65 mm, Tmin,max = 0.77, 0.83,
N(hemisphere) = 9154, N = 4439 (Rint = 0.033), No = 3142,
V = 1607 Å3, Dc (Z = 4) = 1.805 g cmϪ3, µMo = 17.4 cmϪ1
,
R = 0.057, Rw = 0.060, |∆ρmax| = 0.69 e ÅϪ3
.
specimen 0.12 × 0.10 × 0.06 mm, ‘T’min,max = 0.74, 0.89, Nt =
Variata. (x, y, z, Uiso)H were refined for the ligand; hydrogen
atoms were located in difference maps for O(1–3) and included
in the refinement with constrained parameters. Other residues
O(4–6) were modelled as oxygen atoms only, occupancy 0.5,
0.25, 0.25, ‘Cl(5)’ also having occupancy 0.5 (caveat: cf. O),
with high ‘thermal motion’ evident among Cl(4,5), O(1–4).
16230, N = 4227 (Rint = 0.047), No = 3150, R = 0.042,
Rw = 0.041, |∆ρmax| = 0.6(1) e ÅϪ3
.
Variata. An initial refinement of xabs with ‘Friedel pair’ data
preserved distinct gave a value of ca. 0.5. Accordingly, the
data were merged.
J. Chem. Soc., Dalton Trans., 2001, 707–722
711