2011
DOI: 10.1016/j.cplett.2011.06.088
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Photo-induced intramolecular charge transfer from antenna to anchor groups in phenoxazine dyes

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Cited by 19 publications
(15 citation statements)
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“…This proves the transitions with ICT characteristic mainly happen between HOMO and LUMO. Table S2 shows that the electronic density at the helicene-imide backbone significantly increases accompanying with a decrease at the lateral donor groups from HOMO to LUMO, which provides a clear picture of the ICT characteristic 35 . The CDD (charge difference density, shown in Supplementary Table S2 ) further shows the same ICT nature as above.…”
Section: Resultsmentioning
confidence: 97%
“…This proves the transitions with ICT characteristic mainly happen between HOMO and LUMO. Table S2 shows that the electronic density at the helicene-imide backbone significantly increases accompanying with a decrease at the lateral donor groups from HOMO to LUMO, which provides a clear picture of the ICT characteristic 35 . The CDD (charge difference density, shown in Supplementary Table S2 ) further shows the same ICT nature as above.…”
Section: Resultsmentioning
confidence: 97%
“…Femtosecond transient ESA processes also have been investigated in a number of organic structures, such as β -carotene, 13 photoactive yellow protein (PYP), 14 dimethylamino-substituted diphenylmethane dyes, 23 fucoxanthin, 16 trans -4-dicyanomethylene-2-methyl-6- p -dimethylamin-ostyryl-4Hpyran, 20 etc., to reveal the nature of excited-state relaxation mechanisms, 16,19 intermediate stages in photochemical reactions, 24 and ultrafast photo-induced energy and charge transfer processes, 16,25 including the role of transient excited electronic states with efficient stimulated emission (gain) properties. 14,23,26,27 …”
Section: Introductionmentioning
confidence: 99%
“…Time resolved transient absorption spectra were recorded using a transient absorption (TA) spectrometer with femtosecond resolution. 35 The laser used for excitation was a Hurricane Ti:Sapphire laser system (Spectra Physics) capable of 800 nm laser pulses of 1 mJ pulse À1 (width of 130 fs) at a rate of 1 kHz. A fraction (5%) of the beam was used to generate a probe pulse.…”
Section: Measurementmentioning
confidence: 99%