Porphyrin Boxes Constructed by Homochiral Self-Sorting Assembly: Optical Separation, Exciton Coupling, and Efficient Excitation Energy Migration
meso-Pyridine-appended zinc(II) porphyrins M n and their meso − meso-linked dimers D n assemble spontaneously, in noncoordinating solvents such as CHCl3, into tetrameric porphyrin squares S n and porphyrin boxes B n , respectively. Interestingly, formation of B n from D n proceeds via homochiral sel...
Saved in:
Published in | Journal of the American Chemical Society Vol. 126; no. 49; pp. 16187 - 16198 |
---|---|
Main Authors | , , , , , , , |
Format | Journal Article |
Language | English |
Published |
WASHINGTON
American Chemical Society
15.12.2004
Amer Chemical Soc |
Subjects | |
Online Access | Get full text |
Cover
Loading…
Summary: | meso-Pyridine-appended zinc(II) porphyrins M n and their meso − meso-linked dimers D n assemble spontaneously, in noncoordinating solvents such as CHCl3, into tetrameric porphyrin squares S n and porphyrin boxes B n , respectively. Interestingly, formation of B n from D n proceeds via homochiral self-sorting assembly, which has been verified by optical separations of B1 and B2. Optically pure enantiomers of B1 and B2 display strong Cotton effects in the CD spectra, which reflect the length of the pyridyl arm, thus providing evidence for the exciton coupling between the noncovalent neighboring porphyrin rings. Excitation energy migration processes within B n have been investigated by steady-state and time-resolved spectroscopic methods in conjunction with polarization anisotropy measurements. Both the pump-power dependence on the femtosecond transient absorption and the transient absorption anisotropy decay profiles are directly associated with the excitation energy migration process within the B n boxes, where the exciton−exciton annihilation time and the polarization anisotropy rise time are well described in terms of the Förster-type incoherent energy hopping model by assuming a number of hopping sites of N = 4 and an exciton coherence length of L = 2. Consequently, the excitation energy hopping rates between the zinc(II) diporphyrin units have been estimated for B1 (48 ps)-1, B2 (98 ± 3 ps)-1, and B3 (361 ± 6 ps)-1. Overall, the self-assembled porphyrin boxes B n serve as a well-defined three-dimensional model for the light-harvesting complex. |
---|---|
Bibliography: | ark:/67375/TPS-SLS9DW41-Z istex:1C0A1812D829B62FA78A1B1C7AEA74EAB03E14F0 ObjectType-Article-1 SourceType-Scholarly Journals-1 ObjectType-Feature-2 content type line 23 |
ISSN: | 0002-7863 1520-5126 |
DOI: | 10.1021/ja046241e |