The shape and maxima of these spectra at 830 + 10 nm were the same in all three solvents. The energy of the S, (2 '4) state was found at 13200 + 300 cm-'. The fluorescence quantum yields of all-tram-g-carotene for the above-mentioned solvents are equal to (O.SkO.2) x 10Vs, (0.8kO.2) x lo-' and (2.O
Weak fluorescence from the S2(1Lb) state of biphenylene
โ Scribed by H. Shizuka; T. Ogiwara; S. Cho; T. Morita
- Publisher
- Elsevier Science
- Year
- 1976
- Tongue
- English
- Weight
- 485 KB
- Volume
- 42
- Category
- Article
- ISSN
- 0009-2614
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โฆ Synopsis
Weak fluorescence from biphenylene has been observed in some solvents [A max: 480 IUT!, Qf" 1.0 {* 0.3) X 104} ctt 350 nm and 20"Cf. The fluorescence is assigned to Sz tL Lb) -t So ('A) by means of the fiuorescence polarizrttion method. The Sz fluorescence in cyc!ohexane was ~~ve~en~h-dependent-Rapid radiationless processes in excited biphenylene are also discussed. I. introduction The spectroscopic properties of biphenylene have been studied by several workers [l---8]. Two papers -[3,4] have described the observation of fluorescence from a higher excited electronic state in biphenylene, as well as long-lived phosphorescence from a higher triplet state.. However, Hochstrasser and McA@ine f5] showed that the previously reported dual emissions _ [3,4] are caused by an impurity that absorbs around 280 nm, and emits fluorescence at 300 nm and phosphorescence at 410 nm. Munro et al. [6] also reported
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