Sharing orbitals: Ultrafast excited state deactivations with different outcomes in bucky ferrocenes and ruthenocenes

被引:53
作者
Guldi, Dirk M. [1 ]
Rahman, G. M. Aminur
Marczak, Renata
Matsuo, Yutaka
Yamanaka, Masahiro
Nakamura, Eiichi
机构
[1] Univ Erlangen Nurnberg, Inst Phys & Theoret Chem, D-91058 Erlangen, Germany
[2] Japan Sci & Technol Agcy, ERATO, Nakamura Funct Carbon Cluster Project, Bunkyo Ku, Tokyo 1130033, Japan
[3] Univ Tokyo, Dept Chem, Bunkyo Ku, Tokyo 1130033, Japan
关键词
D O I
10.1021/ja061120v
中图分类号
O6 [化学];
学科分类号
0703 ;
摘要
We report on the singlet ground and singlet/triplet excited-state features of a series of bucky ferrocenes, bucky ruthenocenes, and respective reference compounds. In the bucky ferrocene conjugates, intimate contacts between the fullerenes and ferrocenes result in appreciable ground-state interactions-suggesting a substantial shift of charge density from the electron donor (i.e., ferrocene) to the electron acceptor (i.e., fullerene). In contrast, no prominent charge-transfer features were observed for the bucky ruthenocene conjugates. An arsenal of experimental techniques, ranging from fluorescence (i.e., steady state and time-resolved) and pump probe experiments (i.e., femtosecond and nanoseconds) to pulse radiolysis, were employed to examine excited-state interactions. In the excited states, bucky ferrocene conjugates are dominated by rapid charge separation reactions (0.8 +/- 0.1 ps) to yield metastable radical ion pairs. The radical ion pair lifetimes vary between 27 and 39 ps. No charge separation was, however, found in the corresponding bucky ruthenocence. Instead, an intrinsically faster excited-state deactivation (similar to 200 ps) evolves from the heavier ruthenium center-relative to iron. This effect is further augmented by the unfavorably shifted oxidation potential in ruthenocene of about 0.61 V, which in ruthenocene (-Delta G(ET) = -0.26 eV), in contrast to ferrocene (-Delta G(ET) = 0.35 eV), renders charge separation thermodynamically unfeasible.
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页码:9420 / 9427
页数:8
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