around 425 nm ending at 550 nm. Luminescence experiments
(lexc = 450 nm) showed a large emission spectrum centred at
720 nm. A similar behaviour was observed for compounds 1a,b
and 2a,b. In the case of 3a and 3b, the two waxy solids were layered
between two glass slides and observed by optical microscopy under
either laser irradiation or cross-polarised light. Irradiation of the
samples at lexc = 405 nm induces a bright red luminescence in
both cases. Polarised optical microscopy (POM) is a powerful tool
to determine in a first attempt whether those compounds could
behave like mesomorphic material. In both cases, a promising
birefringent texture could be observed at 25 ◦C.† However,
unique, Rint = 0.068, R1 = 0.0565 (I > 2s(I)), wR2 = 0.1262 (all data),
GOF = 1.05 for 460 parameters.
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◦
both compounds decompose around 250 C before reaching the
clearing temperature.
We can therefore emphasise that neutral compounds 1a and 1b,
toward the directionality of their easy selective functionalisation,
constitute relevant neutral building blocks for the design of
new families of luminescent materials that may behave like
mesomorphic materials. Studies involving the grafting of other
type of mesogenic gallate-like derivatives on compounds 1a,b are
currently under way.
Acknowledgements
This work has been done in the frame of PECO-NEI no. 370
and ECO-NET 188452H programs. The authors thank ANR
(CLUSTSURF ANR-FI-071215–01-01). Y. Mironov thanks the
Russian Foundation for Basic Research and Fondation Langlios
(grant 08-03-00267).
6 B. K. Roland, W. H. Flora, N. R. Armstrong and Z. Zheng, C. R. Chim.,
2005, 8, 1798.
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2163.
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Notes and references
‡ Crystal data for [Re6S8(TBP)4(OH)2] (1a): M = 1948.51 g mol-1,
monoclinic, space group C2/m, a = 18.3921(5), b = 17.9940(6), c =
◦
3
˚
˚
9.1061(3) A, b = 105.9900(10) , V = 2897.04 (16) A , Z = 2, m(MoKa) =
12.803 mm-1, F(000) = 1784, T = 100(2) K, 18 854 total reflections, 3438
unique, Rint = 0.072, R1 = 0.0418 (I > 2s(I)), wR2 = 0.1035 (all data),
GOF = 1.154 for 125 parameters. Crystal data for [Re6Se8(TBP)4(OH)2]
12 L. Plasseraud, L. G. Cuervo, D. Guillon, G. Suess-Fink, R. De-
schenaux, D. W. Bruce and B. Donnio, J. Mater. Chem., 2002, 12,
2653.
(1b): M = 2296.5 g mol-1, monoclinic, space group◦C2/m, a = 18.3921(5),
13 E0¢ = (Epa + Epc)/2, where Epa and Epc are the anodic and cathodic
peak potentials, respectively. DEp = Epa - Epc.
3
˚
˚
b = 17.9940(6), c = 9.1061(3) A, b = 105.990(10) , V = 2897.04(16) A ,
Z = 2, m(MoKa) = 16.519 mm-1, F(000) = 2018, T = 100(2) K, 19 626
total reflections, 3691 unique, Rint = 0.071, R1 = 0.0381 (I > 2s(I)),
wR2 = 0.0867 (all data), GOF = 1.037 for 121 parameters. Crystal data
for [Re6S8(TBP)4(L1)2]·6CH2Cl2 (2a): M = 2846.43 g mol-1, triclinic, space
14 T. Yoshimura, K. Umakoshi, Y. Sasaki and A. G. Sykes, Inorg. Chem.,
1999, 38, 5557; T. Yoshimura, K. Umakoshi, Y. Sasaki, S. Ishizaka,
H.-B. Kim and N. Kitamura, Inorg. Chem., 2000, 39, 1765; A. Itasaka,
M. Abe, T. Yoshimura, K. Tsuge, M. Suzuki, T. Imamura and Y. Sasaki,
Angew. Chem., Int. Ed., 2002, 41, 463; L. F. Szczepura, M. K. Oh and
S. A. Knott, Chem. Commun., 2007, 4617.
¯
˚
group P1, a = 8.9903(5), b = 14.8782(7), c = 16.7235(8) A, a = 80.5000(2),
◦
3
˚
b = 109.340(2), g = 89.977(3) , V = 2163.48(19) A , Z = 1, m(MoKa) =
8.975 mm-1, F(000) = 1348, T = 100(2) K, 36 599 total reflections, 9829
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