1976
DOI: 10.1016/0009-2614(76)85254-2
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The mixed crystal absorption spectra of 1,1′-diethyl-2,2′-cyanine iodide

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Cited by 3 publications
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“…This matrix shift has been taken into account phenomenologically in the theory of molecular excitons. , The energy down shift results largely from the dispersive stabilization of the S 1 state relative to the ground state owing to the higher polarizability of the former. In neat PIC the solvent shift must be close to that in aza-PIC, since the resonance interaction leads to a nearly symmetric level splitting by 1270 ± 10 cm -1 relative to the monomer peak at 18223 cm -1 in the aza-PIC crystal .…”
Section: Resultsmentioning
confidence: 99%
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“…This matrix shift has been taken into account phenomenologically in the theory of molecular excitons. , The energy down shift results largely from the dispersive stabilization of the S 1 state relative to the ground state owing to the higher polarizability of the former. In neat PIC the solvent shift must be close to that in aza-PIC, since the resonance interaction leads to a nearly symmetric level splitting by 1270 ± 10 cm -1 relative to the monomer peak at 18223 cm -1 in the aza-PIC crystal .…”
Section: Resultsmentioning
confidence: 99%
“…Fairly large Stokes' shift between the fluorescence and absorption band maxima of monomeric PIC in 50% glycerol/water glass (570 cm -1 , Figure ) reveals strong coupling to low-frequency vibrations. A weak ZPL of PIC monomer in the aza-PIC matrix is accompanied by a huge asymmetric wing spreading between 40 and 340 cm -1 (at half-intensity) and peaking at 100 ± 10 cm -1 (data taken from Figure in ref ). These vibrations seem to be characteristic mainly to the chromophore itself rather than to the matrix, because the Stokes' shift in a glass is twice as large as the width of the wing in the crystal (300 cm -1 ).…”
Section: Resultsmentioning
confidence: 99%
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