“…The time-resolved fluorescence measurements were made with an up-conversion method [12,13] using a Ti:sapphire laser (Spectra Physics, Tsunami, 840 nm, 80 MHz) which was pumped with a diode-pumped solid state laser (Spectra Physics, Millennia X). The fundamental pulses are separated into two beams; the one is frequency-doubled by a BBO crystal (420 nm) and is used to excite the sample, and the other beam serves as a gate pulse.…”
Ultrafast excited-state relaxation process has been studied with zinc porphyrin dimers and circular trimer. Following 80 fs excitation at Soret band (420 nm) or Q band (580 nm) of zinc porphyrin, the fluorescence decay curves exhibit ultrafast decays with lifetimes of 80 fs in o-dimer, 450 fs in trimer and 540 fs in m-dimer. The time-resolved fluorescence spectra show that the fast decay process correspónd to disappearance of monomer-like emission followed by red-shifted and broaden spectra. These ultrafast processes are assigned as due to excitation transfer among monomers and delocalization of excitation yielding excitonic states.
“…The time-resolved fluorescence measurements were made with an up-conversion method [12,13] using a Ti:sapphire laser (Spectra Physics, Tsunami, 840 nm, 80 MHz) which was pumped with a diode-pumped solid state laser (Spectra Physics, Millennia X). The fundamental pulses are separated into two beams; the one is frequency-doubled by a BBO crystal (420 nm) and is used to excite the sample, and the other beam serves as a gate pulse.…”
Ultrafast excited-state relaxation process has been studied with zinc porphyrin dimers and circular trimer. Following 80 fs excitation at Soret band (420 nm) or Q band (580 nm) of zinc porphyrin, the fluorescence decay curves exhibit ultrafast decays with lifetimes of 80 fs in o-dimer, 450 fs in trimer and 540 fs in m-dimer. The time-resolved fluorescence spectra show that the fast decay process correspónd to disappearance of monomer-like emission followed by red-shifted and broaden spectra. These ultrafast processes are assigned as due to excitation transfer among monomers and delocalization of excitation yielding excitonic states.
“…Optical spectroscopy studies of both native and reconstituted PCP complexes have been carried out on the ensemble (Akimoto, 1996;Kleima, 2000;Krueger, 2001) and singlemolecule levels Wormke, 2007a;Wormke, 2008). Using transient absorption in femtosecond timescale main energy transfer pathways have been described, it has also been demonstrated that the two Chl a molecules interact relatively weakly with characteristic transfer time between them to be of the order to 12 ps (Kleima, 2000).…”
“…In other antenna systems the balance between how much energy comes from S 2 and how much from S 1 will vary depending on which light-harvesting complex is being studied. Akimoto et al (1996) monitored the rate of energy transfer from the carotenoid (peridinin) to chlorophyll a in the water soluble peridinin-Chl a antenna complex from a dinoflagellate, Alexandrium cohorticula. This energy transfer process is ~100% efficient.…”
Section: Singlet-singlet Energy Transfermentioning
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