Abstract
Two conjugated organometallic oligomers of the type (-C[triple bond]CPt(L)(2)C[triple bond]C(ZnP)-)(n) and model compounds [PhC[triple bond]CPt(L)(2)C[triple bond]C(ZnP)C[triple bond]CPt(L)(2)C[triple bond]CPh] with L = tri(n-butyl)-phosphine and ZnP = zinc(II)(10,20-bis(Ar)porphyrine) (Ar = mesityl (Mes; P1 and M1) or 3,4,5-trihexadecyloxyphenyl (P2 and M2)) were synthesized and characterized ((1)H and (31)P NMR, HRMS, elemental analysis, IR, GPC, and TGA). GPC indicates that P1 and P2 exhibit respectively approximately 6 and approximately 3 units with a polydispersity of 1.4. M1 was also characterized by X-ray crystallography. The Pt...Pt separation in M1 is 1.61 nm, which makes P1 approximately 9.6 nm long. The spectral measurements show that the absorption and photoluminescence spectra of M1, M2, P1, and P2 are remarkably red-shifted. For example, the low energy Q-band is observed at 677 +/- 1 nm in comparison with their precursors HC[triple bond]C(ZnP)C[triple bond]CH, L1 and L2 (Ar = mesityl (Mes; L1) or 3,4,5-trihexadecyloxyphenyl (L2)), both at 298 and 77 K, for which the Q-band is observed at 622 nm. The photophysical parameters, fluorescence lifetimes (tau(F)), and quantum yields (Phi(F)) show a slight decrease by a factor of approximately 2 (at most 3) following the trend L1 approximately L2 > M1 approximately M2 > P1 approximately P2, a trend explained by a combination of the heavy atom effect and an increase in internal conversion rate due to the increase in oligomer dimension. This small variation of the photophysical data for materials of a few nm in dimension contrasts with the larger change in tau(P), phosphorescence lifetimes of the Pt-containing unit in the (-C(6)H(4)C[triple bond]CPt(L)(2)C[triple bond]C-CC(6)H(4)(ZnP)-)(n) oligomers with n = 3, 6, and 9 reported earlier (Liu, L.; Fortin, D.; Harvey, P. D. Inorg. Chem. 2009, 48, 5891-5900). In this later case, tau(P) decreased by steps of an order of magnitude as n increased from 3 to 6 to 9. This decrease was explained by a T(1) energy transfer from the Pt unit (donor) to MP (acceptor) in combination with an excitonic process (energy delocalization). Because of the full conjugation in P1 and P2, these oligomers behave as distinct molecules, and no energy transfer occurs. These properties make these materials suitable candidates for photocell applications.
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