8 R. P. Thummel, V. Hegde and Y. Jahng, Inorg. Chem., 1989, 28,
pyridyl groups being the same, and with the corresponding
groups in each molecule being identical. Three sets of sub-
sidiary coordinates, all with z = 0, were used to define the differ-
ent types of planar groups present, and each group in the two
molecules was defined by transformation of the appropriate set
of subsidiary coordinates to a local axial system, refineable for
rotation and translation. Appropriate x and y coordinates for
the subsidiary atoms were refined, and planarity was main-
tained by keeping z = 0 in all cases. Corresponding intergroup
distances were slack-constrained to approach equality, but
there were no constraints on rotations between groups in the
molecules. Hydrogen atoms were included in positions calcu-
lated each cycle. Thermal motions were refined using 12-
parameter TL rigid-body models for the groups, with the
centres of libration of the peripheral groups fixed at their points
of attachment to the central ring. The central ring showed no
significant librational motion. Hydrogen atom thermal motions
were included in the appropriate group.
3264; M. Beley, J.-P. Collin, J.-P. Sauvage, H. Sugihara, F. Heisel and
A. Miehé, J. Chem. Soc., Dalton Trans., 1991, 3157; C. R. Hecker,
A. K. I. Gushurst and D. R. McMillin, Inorg. Chem., 1991, 30, 538;
E. Amouyal, M. Mouallem-Bahout and G. Calzaferri, J. Phys.
Chem., 1991, 95, 7641; E. Amouyal and M. Mouallem-Bahout,
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V. Balzani, E. C. Constable and A. M. W. Cargill Thompson, Inorg.
Chem., 1995, 34, 2759.
9 W. R. McWhinnie and J. D. Miller, Adv. Inorg. Chem. Radiochem.,
1969, 12, 135.
10 E. C. Constable, Prog. Inorg. Chem., 1994, 42, 67; J.-P. Sauvage,
J.-P. Collin, J. C. Chambron, S. Guillerez, C. Coudret, V. Balzani,
F. Barigelletti, L. De Cola and L. Flamigni, Chem. Rev., 1994, 94,
993; E. C. Constable, in Transition Metals in Supramolecular Chem-
istry, eds. L. Fabbrizzi and A. Poggi, Kluwer, Dordrecht, 1994,
p. 81; A. Harriman and J.-P. Sauvage, Chem. Soc. Rev., 1996, 41;
A. Harriman and R. Ziessel, Chem. Commun., 1996, 1707.
11 (a) E. C. Constable, A. M. W. Cargill Thompson, P. Harveson,
L. Macko and M. Zehnder, Chem. Eur. J., 1995, 1, 360; (b) E. C.
Constable and P. Harveson, Chem. Commun., 1996, 33; (c) E. C.
Constable and P. Harveson, Chem. Commun., 1996, 1821; (d) D.
Armspach, M. Cattalini, E. C. Constable, C. E. Housecroft and
D. Phillips, Chem. Commun., 1996, 1823; ( f ) E. C. Constable and
R. A. Fallahpour, J. Chem. Soc., Dalton Trans., 1996, 2389; (e) B.
Whittle, S. R. Batten, J. C. Jeffery, L. H. Rees and M. D. Ward,
J. Chem. Soc., Dalton Trans., 1996, 4249.
For [CuL1 ][PF6]2, hydrogen atoms were included in calcu-
2
lated positions and assigned thermal parameters equal to those
of the atom to which they were bonded. Positional and aniso-
tropic thermal parameters for the non-hydrogen atoms were
refined using full-matrix least squares.
For both structures, reflection weights used were 1/σ2(Fo),
12 E. C. Constable and A. M. W. Cargill Thompson, J. Chem. Soc.,
Dalton Trans., 1992, 3467; 1995, 1615.
¹
2
2
²
with σ(Fo) being derived from σ(Io) = [σ (Io) ϩ (0.04Io) ] . The
2
2
¹
13 M. P. O’Niel, M. P. Niemczyk, W. A. Svec, D. Gosztola, G. L. Gains
III and M. R. Wasielewski, Science, 1992, 257, 63; M. Ohkohchi,
A. Takahashi, N. Mataga, T. Okada, A. Osuka, H. Yamada and
K. Maruyama, J. Am. Chem. Soc., 1993, 115, 12 137; A. Osuka,
S. Nakajima, T. Okada, S. Taniguchi, K. Nozaki, T. Ohno, I. Yama-
zaki, Y. Nishimura and N. Mataga, Angew. Chem., Int. Ed. Engl.,
1996, 35, 92; C. A. Hunter and R. K. Hyde, Angew. Chem., Int.
Ed. Engl., 1996, 35, 1936; M. P. Debreczeny, W. A. Svec and M. R.
Wasielewski, Science, 1996, 274, 584.
14 G. M. Bower and L. W. Frost, J. Polym. Sci., Part A, 1963, 1, 3135;
F. Higashi, S.-I. Ogata and Y. Aoki, J. Polym. Chem. Ed., 1982, 20,
2081; H. M. Gajiwala and R. Zand, Macromolecules, 1993, 26, 5976.
15 G. D. Storrier and S. B. Colbran, J. Chem. Soc., Dalton Trans., 1996,
2185.
²
weighted residual is defined as RЈ = (Σw∆ /ΣwFo ) . Atomic scat-
tering factors and anomalous dispersion parameters were from
ref. 32. Structure solutions were by MULTAN 8033 and refine-
ments used RAELS for L1 and BLOCKLS, a local version of
ORFLS,34 for [CuL1 ][PF6]2; ORTEP II 20 running on a Mac-
2
intosh IIcx was used for the structural diagrams, and a DEC
Alpha-AXP workstation was used for calculations.
CCDC reference number 186/597.
Acknowledgements
Support from the Australian Research Council is gratefully
acknowledged.
16 W. Spahni and G. Calzaferri, Helv. Chim. Acta, 1984, 67, 450.
17 E. Campaigne, W. E. Budd and G. F. Schaefer, Org. Synth., 1963,
Coll. Vol. II, 225.
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Received 23rd April 1997; Paper 7/02778H
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J. Chem. Soc., Dalton Trans., 1997, Pages 3011–3028