Comparative study of the photophysical properties of nonplanar tetraphenylporphyrin and octaethylporphyrin diacids

被引:126
作者
Chirvony, VS
van Hoek, A
Galievsky, VA
Sazanovich, IV
Schaafsma, TJ
Holten, D
机构
[1] Natl Acad Sci Belarus, Inst Mol & Atom Phys, Minsk 220072, BELARUS
[2] Agr Univ Wageningen, Dept Biomol Sci, Phys Mol Lab, NL-6703 HA Wageningen, Netherlands
[3] Washington Univ, Dept Chem, St Louis, MO 63130 USA
关键词
D O I
10.1021/jp001631i
中图分类号
O64 [物理化学(理论化学)、化学物理学];
学科分类号
070304 ; 081704 ;
摘要
The photophysical properties of the lowest excited singlet states, S-1(pi,pi*), of two porphyrin diacids have been investigated. The diacids are H4TPP2+ and H4OEP2+, the diprotonated forms of free base tetraphenylporphyrin (H2TPP) and octaethylporphyrin (H2OEP), respectively. Both diacids exhibit perturbed static and dynamic characteristics relative to the parent neutral complexes in solution at room temperature. These properties include enhanced yields of S-1 - S-0 radiationless deactivation (internal conversion), which increase from similar to0.1 for H2TPP and H2OEP to 0.4 for H4OEP2+ and 0.6 for H4TPP2+. The fluorescence lifetimes of both diacids are strongly temperature dependent, with an activation enthalpy of similar to 1400 cm(-1) for S-1-state deactivation. The enhanced nonradiative decays and many other photophysical consequences of diacid formation are attributed primarily to nonplanar macrocycle distortions. Both H4TPP2+ and H4OEP2+ have been shown previously by X-ray crystallography to adopt saddle-shaped conformations, and the magnitudes of the perturbed properties for the two diacids in solution correlate with the extent of the deviations from planarity in the crystals. A model is proposed to explain the nonradiative decay behavior of the porphyrin diacids that is relevant to nonplanar porphyrins in general. The model includes the existence of decay funnels on the S-1-(pi,pi*)- state energy surface that are separated from the equilibrium conformation and other minima by activation barriers. It is suggested that these funnels involve configurations at which the potential-energy surfaces of the ground and excited states approach more closely than at the equilibrium excited-state structure(s) from which steady-state fluorescence occurs. Possible contributions to the relevant nuclear coordinates are discussed.
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页码:9909 / 9917
页数:9
相关论文
共 72 条
[51]  
RAVIKANTH M, 1995, STRUCT BOND
[52]   Photoinduced evolution on the conformational landscape of nonplanar dodecaphenylporphyrin:: Picosecond relaxation dynamics in the 1(π,π*) excited state [J].
Retsek, JL ;
Gentemann, S ;
Medforth, CJ ;
Smith, KM ;
Chirvony, VS ;
Fajer, J ;
Holten, D .
JOURNAL OF PHYSICAL CHEMISTRY B, 2000, 104 (29) :6690-6693
[53]  
RETSEK JL, UNPUB
[54]  
SAGUN EI, 1990, KHIM FIZ, V9, P764
[55]   Matrix photochemistry of cycloheptatriene: Site effects [J].
Samuni, U ;
Kahana, S ;
Haas, E .
JOURNAL OF PHYSICAL CHEMISTRY A, 1998, 102 (25) :4758-4768
[56]  
Senge MO, 1999, J PORPHYR PHTHALOCYA, V3, P216
[57]  
Senge MO, 1999, Z NATURFORSCH B, V54, P821
[58]   Synthesis and structural characterization of nonplanar tetraphenylporphyrins and their metal complexes with graded degrees of β-ethyl substitution [J].
Senge, MO ;
Kalisch, WW .
INORGANIC CHEMISTRY, 1997, 36 (26) :6103-6116
[59]  
SENGE MO, 1994, ANGEW CHEM INT EDIT, V33, P2485
[60]   PORPHYRINS .13. FLUORESCENCE SPECTRA AND QUANTUM YIELDS [J].
SEYBOLD, PG ;
GOUTERMA.M .
JOURNAL OF MOLECULAR SPECTROSCOPY, 1969, 31 (01) :1-&