TY - JOUR
T1 - Synthesis and photoinduced electron transfer processes of rotaxanes bearing [60]fullerene and zinc porphyrin
T2 - Effects of interlocked structure and length of axle with porphyrins
AU - Sandanayaka, Atula S.D.
AU - Watanabe, Nobuhiro
AU - Ikeshita, Kei Ichiro
AU - Araki, Yasuyuki
AU - Kihara, Nobuhiro
AU - Furusho, Yoshio
AU - Ito, Osamu
AU - Takata, Toshikazu
PY - 2005/2/24
Y1 - 2005/2/24
N2 - Three rotaxanes, with axles with two zinc porphyrins (ZnPs) at both ends penetrating into a necklace pending a C60 moiety, were synthesized with varying interlocked structures and axle lengths. The intra-rotaxane photoinduced electron transfer processes between the spatially positioned C 60 and ZnP in rotaxanes were investigated. Charge-separated (CS) states (ZnṖ+, C60̇-) rotaxane are formed via the excited singlet state of ZnP ( 1ZnP*) to the C60 moiety in solvents such as benzonitrile, THF, and toluene. The rate constants and quantum yields of charge separation via 1ZnP* decrease with axle length, but they are insensitive to solvent polarity. When the axle becomes long, charge separation takes place via the excited triplet state of ZnP (3ZnP*). The lifetime of the CS state increases with axle length from 180 to 650 ns at room temperature. The small activation energies of charge recombination were evaluated by temperature dependence of electron-transfer rate constants, probably reflecting through-space electron transfer in the rotaxane structures.
AB - Three rotaxanes, with axles with two zinc porphyrins (ZnPs) at both ends penetrating into a necklace pending a C60 moiety, were synthesized with varying interlocked structures and axle lengths. The intra-rotaxane photoinduced electron transfer processes between the spatially positioned C 60 and ZnP in rotaxanes were investigated. Charge-separated (CS) states (ZnṖ+, C60̇-) rotaxane are formed via the excited singlet state of ZnP ( 1ZnP*) to the C60 moiety in solvents such as benzonitrile, THF, and toluene. The rate constants and quantum yields of charge separation via 1ZnP* decrease with axle length, but they are insensitive to solvent polarity. When the axle becomes long, charge separation takes place via the excited triplet state of ZnP (3ZnP*). The lifetime of the CS state increases with axle length from 180 to 650 ns at room temperature. The small activation energies of charge recombination were evaluated by temperature dependence of electron-transfer rate constants, probably reflecting through-space electron transfer in the rotaxane structures.
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U2 - 10.1021/jp045831w
DO - 10.1021/jp045831w
M3 - Article
AN - SCOPUS:14544273206
SN - 1520-6106
VL - 109
SP - 2516
EP - 2525
JO - Journal of Physical Chemistry B
JF - Journal of Physical Chemistry B
IS - 7
ER -