1989
DOI: 10.1016/0584-8539(89)80039-x
|View full text |Cite
|
Sign up to set email alerts
|

Electron molecular vibration coupling in vibrational spectra of BEDT-TTF based radical cation salts

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
1
1
1

Citation Types

9
91
0

Year Published

1992
1992
2020
2020

Publication Types

Select...
8

Relationship

0
8

Authors

Journals

citations
Cited by 154 publications
(100 citation statements)
references
References 17 publications
9
91
0
Order By: Relevance
“…2 with a 16% isotope ratio, and the frequency temperature dependence shown in fig. 3 is clearly an internal mode, and is assigned to an out-of-plane bSu mode, since there are no in-plane modes with this frequency and isotope shift in the results of the normal-coordinate calculations of Kozlov et al [22]. We did not obtain an isotope shift for the feature labelled # 6 and so are unable to assign it.…”
Section: Resultsmentioning
confidence: 61%
“…2 with a 16% isotope ratio, and the frequency temperature dependence shown in fig. 3 is clearly an internal mode, and is assigned to an out-of-plane bSu mode, since there are no in-plane modes with this frequency and isotope shift in the results of the normal-coordinate calculations of Kozlov et al [22]. We did not obtain an isotope shift for the feature labelled # 6 and so are unable to assign it.…”
Section: Resultsmentioning
confidence: 61%
“…50 fs indicates that the electron oscillation begins to interact coherently with the intramolecular  3 mode at the finite time delay. Considering the strong electron molecular vibration (EMV) coupling of the  3 mode [49][50][51], it is reasonable to consider that the electron oscillation selectively induces the intermolecular anti-phase  3 vibration, as shown in Figure 15f,g [49][50][51]. After 100 fs, the hollow at approximately 1450 cm -1 disappears; a broad band appears at 1450 cm -1 , reflecting the electronic dephasing [ Figure 15d and (iii) in Figure 14b].…”
Section: Ultrafast Snapshot Of Correlated Electron Dynamics 10 Fs Spementioning
confidence: 99%
“…These electron oscillations are efficiently induced between the charge-rich sites (A and B sites) and between the charge-rich site and charge-poor site (B and A' sites) [38,41,42], as shown by the arrows in Figure 16 and Figure 15f. Considering that C=C stretching modes ν 3 (presented in Figure 15g) appear between 1352 and 1476 cm -1 [49][50][51], the spectral hollow that appears at ca. 1450 cm -1 [arrow in Figure 15c and (ii) in Figure 14a,b] is attributable to the destructive interference that prevails between the electron oscillation and the intramolecular  3 mode.…”
Section: Ultrafast Snapshot Of Correlated Electron Dynamics 10 Fs Spementioning
confidence: 99%
“…A normal mode analysis of BEDT-TTF 0 and BEDT-TTF 1+ was reported by Kozlov et al [42,43]. The normal modes most sensitive to the charge (valence) of the BEDT-TTF molecule are the in-phase (ν 2 , Raman active) and out-of-phase (ν 27 infrared active) stretching modes of the ring C=C bonds, and the stretching mode of the C=C bond bridging two five member rings (ν 3 , Raman active).…”
Section: Charge-sensitive Mode Of Bedt-ttfmentioning
confidence: 99%
“…The coupling constant in BEDT-TTF is estimated in refs. [43,53]. The coupling constants of ν 2 and ν 3 were respectively estimated to be g 2 = 0.043 and g 3 = 0.071 eV from an analysis of the infrared spectrum of the isolated dimer (BEDT-TTF) 2 2+ [53].…”
Section: Electron-molecular Vibration (Emv) Coupling In Bedt-ttfmentioning
confidence: 99%