2011
DOI: 10.1021/jp204111u
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Energy Transfer and Confined Motion of Dyes Trapped in Semiconducting Conjugated Polymer Nanoparticles

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Cited by 41 publications
(82 citation statements)
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“…The shortening of the monomolecular decay time (420 to 372 ps) is due to the increase in microviscosity and polarizability inside the polymer NPs 11. 35 The slower decay component is assigned to the H‐aggregated state of QTH molecules inside the polymer NPs 43. 46 The aggregation formation inside polymer NPs was enhanced as the relative concentration of QTH was increased.…”
Section: Resultsmentioning
confidence: 99%
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“…The shortening of the monomolecular decay time (420 to 372 ps) is due to the increase in microviscosity and polarizability inside the polymer NPs 11. 35 The slower decay component is assigned to the H‐aggregated state of QTH molecules inside the polymer NPs 43. 46 The aggregation formation inside polymer NPs was enhanced as the relative concentration of QTH was increased.…”
Section: Resultsmentioning
confidence: 99%
“…Figure 7A shows the anisotropic decay curves of QTH in THF and encapsulated in PMMA NPs in the absence of NR dye. Here, we assumed that the rotational diffusion time of PMMA polymer NPs does not affect the faster rotational motion of encapsulated oligothiophene molecules 35. For pure QTH in THF, a very fast anisotropic decay with average reorientation time of approximately 69 ps was observed.…”
Section: Resultsmentioning
confidence: 99%
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“…[30][31][32] First, 300 mL of 1 mg mL À1 P3HT in THF, 150 mL of 1 mg mL À1 hexadecylamine (HDA) in THF and 150 mL of THF were mixed under an inert atmosphere and the mixed solution was ultrasonicated to get a completely homogeneous solution. [30][31][32] First, 300 mL of 1 mg mL À1 P3HT in THF, 150 mL of 1 mg mL À1 hexadecylamine (HDA) in THF and 150 mL of THF were mixed under an inert atmosphere and the mixed solution was ultrasonicated to get a completely homogeneous solution.…”
Section: Methodsmentioning
confidence: 99%
“…Host–guest donor–acceptor systems, consisting of polymer/dye blends or of different conjugated polymers, might exploit nonradiative energy transfer processes to reduce self‐absorption and other sources of optical losses. For instance, Coumarin 153 (C153, Figure b) in poly( N ‐vinylcarbazole) (PVK) nanoparticles show higher yield upon increasing the particle size, quenching of the luminescence spectrum and shortening of the PVK host decay time, suggesting an energy transfer from PVK to C153 . In another study, F8BT is found to show a significantly reduced ASE threshold depending on the blending ratio with other copolymers, such as the Dow Red F .…”
Section: Methodsmentioning
confidence: 98%