2006
DOI: 10.1016/j.chemphys.2006.01.008
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Characterization of infrared vibrational activity in specific totally symmetric bridging modes of mixed-valence systems near the localized-to-delocalized transition

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Cited by 16 publications
(20 citation statements)
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“…Intensified IR bands have previously been reported for conjugated polymer polarons 33 , 43 47 and mixed-valence compounds, 48 , 49 and they are often described as “infra-red active vibrations” (IRAVs). They can arise from both charge localization, signifying Robin–Day class II/III borderline character, 49 and from vibronic coupling to low-energy electronic transitions, even in fully delocalized (class III) systems. 48 , 49 Charge localization reduces the symmetry of a molecule, making Raman modes become IR-active and amplifying IR bands.…”
Section: Resultsmentioning
confidence: 99%
“…Intensified IR bands have previously been reported for conjugated polymer polarons 33 , 43 47 and mixed-valence compounds, 48 , 49 and they are often described as “infra-red active vibrations” (IRAVs). They can arise from both charge localization, signifying Robin–Day class II/III borderline character, 49 and from vibronic coupling to low-energy electronic transitions, even in fully delocalized (class III) systems. 48 , 49 Charge localization reduces the symmetry of a molecule, making Raman modes become IR-active and amplifying IR bands.…”
Section: Resultsmentioning
confidence: 99%
“…The vibronic enhancement of normally forbidden IR transitions is distinctly different from the use of the 8a mode as a marker for localization of charge on the time scale longer than the period of the mode, ca. 20 fs [23,56]. IR activity of symmetric pyrazine modes exists in the full IR spectra for mixed-valence anions 4 − -6 − , but the active 8a mode (the most intense of these bands) in particular is overlapped with cluster acetate bands and is not unambiguously clear.…”
Section: If the Bridge Is Rocking The Ir Can Be Shockingmentioning
confidence: 95%
“…For this band, 3Z2600 M K1 cm K1 compared with 3Z800 M K1 cm K1 in cis-[Os(bpy) 2 (pz)Cl] C . This appears to be a non-Condon effect with coupling of the vibration to intervalence transfer across the bridge (Demadis et al 1998a(Demadis et al ,b, 1999aRocha & Shreve 2004, 2006.…”
Section: (I) Symmetrical Vibrations In the Bridgementioning
confidence: 99%
“…For harmonic oscillator vibrational wave functions, the contribution to the barrier through the vZ0/vZ0 channel is exp(KS )(S v /v!). (Demadis et al 1998a(Demadis et al ,b, 1999aRocha & Shreve 2004, 2006 (Lu et al 1995).…”
Section: (Iii) Barrier Vibrationsmentioning
confidence: 99%
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