1994
DOI: 10.1021/ja00102a086
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Low-Energy Electronic Absorptions in 17-Electron Organometallic Piano Stool Radicals

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Cited by 51 publications
(33 citation statements)
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“…4000 cm À1 with a very low intensity (100 L mol À1 cm À1 ) (Fig. 6) [81,82]. The predictions of intramolecular interactions in 7 discussed within the electrochemical part (vide supra) are validated with these results.…”
Section: Spectroelectrochemistrysupporting
confidence: 64%
“…4000 cm À1 with a very low intensity (100 L mol À1 cm À1 ) (Fig. 6) [81,82]. The predictions of intramolecular interactions in 7 discussed within the electrochemical part (vide supra) are validated with these results.…”
Section: Spectroelectrochemistrysupporting
confidence: 64%
“…Additionally, a very weak excitation ( ϵ <100 L mol –1 cm –1 ) at λ = 2500 nm was detected, which can be assigned to the forbidden metal‐centered ligand‐field electronic transition (Figure 2). This excitation is a typical indication of the formation of a 17‐valence electron ferrocenium species 50,51. The absence of an intervalence charge‐transfer absorption is attributed to the structural properties of 2 excluding π conjugation and validates that mainly electrostatic interactions are responsible for the observed redox splitting between the equally charged redox centers in 2 n + ( n = 2, 3, 4).…”
Section: Resultsmentioning
confidence: 53%
“…With this in mind, 3,4‐diferrocenyl‐ N ‐phenylpyrrole ( 3a ) and 3,4‐diferrocenyl‐ N ‐tosylpyrrole ( 3b ) could be classified as weak coupled class II systems according to Robin and Day 29. Hence spectroelectrochemical investigations show the influence of the position of ferrocenyl groups on the intervalence charge transfer through the N ‐phenylpyrrole, thus demonstrating that the 2,5‐position is more suitable to facilitate electron transfer 25,28,30…”
Section: Resultsmentioning
confidence: 82%
“…The forbidden metal‐centered ligand‐field (LF) electronic transition usually occurs at approximately 4000 cm –1 with a very low intensity (generally close to 100 L mol –1 cm –1 ) (Figure 5). 27,28 The LMCT and LF transition can be described very well by Gaussian‐shaped functions by using the method of deconvolution (Figure 5). Considering that the experimental graph is described by two Gauss functions (Table 3), the extinction should tend to zero in the region between 5000 and 7000 cm –1 .…”
Section: Resultsmentioning
confidence: 99%