Abstract
The vibronic structure superimposed on the benzene Rydberg transition corresponding to 3e1u(r) → 3s(a1g) excitation at 11 eV has been studied spectroscopically. The revealed structure is interpreted in terms of two Rydberg systems deriving from 3e2g(σ) → 6p(e1u) and 3e2g(σ) → 6f(b1u, b2u, e1u, e2u) which fit respectively the δ = 0.47 and δ = 0.3 Rydberg series converging to the second ionization limit. In n = 6; δ = 0.3 the pure electronic band as well as the 0-1 band corresponding to ν2(a1g) split upon reducing the vibrational symmetry to D2h by suitable deuterations whereas no such splitting was detected on the 0-1 band corresponding to the Jahn-Teller active mode ν18(e2g). The same pattern is revealed in n = 4 of the same Rydberg series. This pattern is accounted for theoretically.
Original language | English |
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Pages (from-to) | 92-97 |
Number of pages | 6 |
Journal | Chemical Physics Letters |
Volume | 52 |
Issue number | 1 |
DOIs | |
State | Published - 15 Nov 1977 |
ASJC Scopus subject areas
- General Physics and Astronomy
- Physical and Theoretical Chemistry