2012
DOI: 10.1021/jp305916x
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Conformation and Electronic Population Transfer in Membrane-Supported Self-Assembled Porphyrin Dimers by 2D Fluorescence Spectroscopy

Abstract: Two-dimensional fluorescence spectroscopy (2D FS) is applied to determine the conformation and femtosecond electronic population transfer in a dimer of magnesium meso tetraphenylporphyrin. The dimers are prepared by self-assembly of the monomer within the amphiphilic regions of 1,2-distearoyl-sn-glycero-3-phosphocholine liposomes. A theoretical framework to describe 2D FS experiments is presented, and a direct comparison is made between the observables of this measurement and those of 2D electronic spectroscop… Show more

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Cited by 77 publications
(158 citation statements)
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“…These four excitation pathways contribute to the cumulative photocurrent signal according to GSB þ SE þ ESA 1 À ESA 2 , where ESA 2 ¼ G Á ESA 1 and GZ0 represents the photocurrent quantum yield associated with excitons created on state-|2i relative to the quantum yield associated with excitons created on state-|1i. We note that in previous fluorescencedetected 2D experiments performed on condensed phase molecular systems [16][17][18][19] , we typically observed the value of Go1, indicating that the fluorescence quantum yield from high-lying excited states is small (due to radiationless deactivation processes) in comparison with the fluorescence yield from lowlying excited states. For photocurrent-detected 2D experiments, we anticipate that the value of G may be much larger than for the corresponding fluorescence case (that is, G41), since we expect the photocurrent quantum yield to be enhanced for high-lying excited states in comparison to low-lying states.…”
mentioning
confidence: 63%
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“…These four excitation pathways contribute to the cumulative photocurrent signal according to GSB þ SE þ ESA 1 À ESA 2 , where ESA 2 ¼ G Á ESA 1 and GZ0 represents the photocurrent quantum yield associated with excitons created on state-|2i relative to the quantum yield associated with excitons created on state-|1i. We note that in previous fluorescencedetected 2D experiments performed on condensed phase molecular systems [16][17][18][19] , we typically observed the value of Go1, indicating that the fluorescence quantum yield from high-lying excited states is small (due to radiationless deactivation processes) in comparison with the fluorescence yield from lowlying excited states. For photocurrent-detected 2D experiments, we anticipate that the value of G may be much larger than for the corresponding fluorescence case (that is, G41), since we expect the photocurrent quantum yield to be enhanced for high-lying excited states in comparison to low-lying states.…”
mentioning
confidence: 63%
“…We implemented phase-modulation 2DPS using a train of four collinear ultrafast laser pulses. The experimental set-up and laser pulse characteristics are very similar to those previously described for 2DFS performed at visible [15][16][17]19 and at ultraviolet wavelengths 18 . The phase-modulation method provides a means to isolate the fourth-order population contribution to the photocurrent signal, which is used to construct the 2D spectra.…”
Section: Methodsmentioning
confidence: 86%
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“…Usual implementations of 2D ES rely upon optical wavevector matching to measure a thirdorder mesoscopic polarization response [2].In this work, we focus upon the two-dimensional photoexcitation spectroscopy (2D PES), as a variant of 2D ES techniques, in which the detected nonlinear optical signals rely on the fourth-order excited-state population. According to the final population of interest, one can probe the excitation spectral signals in forms of photoluminescence (PL) [6][7][8] or photocurrent (PC) [9][10][11], for example. Indeed, this implementation of 2D coherent spectroscopy has the formidable advantage that it can exploit photocurrent detection as an extraordinarily sensitive population probe [12].…”
Section: Introductionmentioning
confidence: 99%