๐”– Bobbio Scriptorium
โœฆ   LIBER   โœฆ

Symmetry of the Second Excited Singlet State of Benzene

โœ Scribed by DUNN, T. M.; INGOLD, C. K.


Book ID
109585046
Publisher
Nature Publishing Group
Year
1955
Tongue
English
Weight
510 KB
Volume
176
Category
Article
ISSN
0028-0836

No coin nor oath required. For personal study only.


๐Ÿ“œ SIMILAR VOLUMES


Direct Transformation of the Second Exci
โœ Dr. D. Bryce-Smith; Dr. A. Gilbert; Prof. D. A. Robinson ๐Ÿ“‚ Article ๐Ÿ“… 1971 ๐Ÿ› John Wiley and Sons ๐ŸŒ English โš– 239 KB ๐Ÿ‘ 2 views

However, treating 2-lithiothiophene with quinoline at 20ยฐC by Giiman's methodf6] leads only to 2-(2-thienyl)quinoline (2) (38%), indicating steric hindrance of 4-addition by the peri-hydrogen atom of the quinoline. In the following reactions of the quinoline system with 2-lithiothiophene derivatives

Second excited singlet state fluorescenc
โœ D.J. Clouthier; A.R. Knight; R.P. Steer ๐Ÿ“‚ Article ๐Ÿ“… 1978 ๐Ÿ› Elsevier Science ๐ŸŒ English โš– 297 KB

Absorption, fluorescence emission and fluorescence excitation spectra of the g 'A' +% IA' (IT\* + d band system of UFCS in the gas phase at room temperature and at -78ยฐC have been measured. Quantum yieids of fluorescence from nine shle vrbronic leveIs of the g state have been measured under isolated

Fluorescence from the second excited sin
โœ Urs P. Wild; Hans J. Griesser; Vo Dinh Tuan; Jean F.M. Oth ๐Ÿ“‚ Article ๐Ÿ“… 1976 ๐Ÿ› Elsevier Science ๐ŸŒ English โš– 538 KB

The emission spectra of the second excited singlet state of [ 181 annukne and of monofluoro [ 181 annulene (m a 3methylpentanc glass at 4 K) are reported. The large ener,7 gap between the fist and second excited singlet states inhibits fast internal cogversion and favours the appearance of S2 + So e

Fluorescence from the second excited sin
โœ S.Z. Levine; A.R. Knight; R.P. Steer ๐Ÿ“‚ Article ๐Ÿ“… 1974 ๐Ÿ› Elsevier Science ๐ŸŒ English โš– 372 KB

Fluorescence has been observed from the second excited singkt stste of tkiophosgene vapour. The emission is excited mainly by transitions originating in the out-of-plane bending mode of the ground stzte and terminating in the lowest vibrational levekof the-excited state. i '.