2013
DOI: 10.1021/la402191p
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Excited-State Dynamics of Charged Dyes at Alkane/Water Interfaces in the Presence of Salts and Ionic Surfactants

Abstract: The excited-state dynamics of the cationic dye malachite green (MG) and of the dianionic dye eosin B at the dodecane/water interface has been investigated using femtosecond time-resolved surface second harmonic generation (TR-SSHG). By using different probe wavelengths, the contributions of monomeric and aggregated MG to the signal could be spectroscopically distinguished. The effect of the addition of a small amount of surfactants was found to strongly depend on the relative charges of surfactant and dye. For… Show more

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Cited by 13 publications
(27 citation statements)
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“…Compared to DPPG, DPPC has a zwitterionic head with an ammonium end group that should lead to substantial Coulombic repulsion of the cationic dye from the interface. A qualitatively similar effect of the charge of the surfactant head on the SSHG signal from ionic dyes has recently been observed …”
Section: Resultssupporting
confidence: 73%
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“…Compared to DPPG, DPPC has a zwitterionic head with an ammonium end group that should lead to substantial Coulombic repulsion of the cationic dye from the interface. A qualitatively similar effect of the charge of the surfactant head on the SSHG signal from ionic dyes has recently been observed …”
Section: Resultssupporting
confidence: 73%
“…This is due to the excess concentration of these anions in the interfacial region relative to the bulk and thus to the Coulombic attraction of the oppositely charged dye. A similar effect was reported with anionic surfactant sodium dodecyl sulfate (SDS) but only at concentrations lower than that required to form a monolayer . Indeed, at higher SDS concentrations, this enhancement effect totally vanished and the population of absorbed dye was apparently similar to that without any surfactant.…”
Section: Introductionsupporting
confidence: 70%
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“…[18][19] The probe pulses (~100 fs, ~2 µJ at the interface) were generated with a collinear optical parametric amplifier (TOPAS-C, Light Conversion), whereas the pump pulses (~80 fs, ~1 µJ at the interface) used for the TR-SSHG measurements were produced by a non-collinear optical parametric amplifier and were circularly polarized (TOPAS White, Light Conversion). The SSHG spectra were recorded by scanning the TOPAS-C with 2 nm steps.…”
Section: Methodsmentioning
confidence: 99%