𝔖 Bobbio Scriptorium
✦   LIBER   ✦

Strong non-adiabatic effects in C2D4+

✍ Scribed by H. Köppel; L.S. Cederbaum; W. Domcke


Publisher
Elsevier Science
Year
1984
Tongue
English
Weight
449 KB
Volume
110
Category
Article
ISSN
0009-2614

No coin nor oath required. For personal study only.

✦ Synopsis


It is demonstrated that the second band in the photoelectron spectrum of CaD, is subject to strong non-adiabatic effects, as was previously found for CzH4. The calculation yields a dense and irrcr&ar vibronic line structure, the line density exceeding that expected front the Fran&-Condon principle by two orders of ma:gitude. The feasibility of extracting vibrational frequencies from peak spacings of the envelope of such complex bands is critically examined. The profound impact which conical intersections of molecular potential-ener,~ surfaces [l-3] exert on the nuclear motion has been well estabhshed in recent years [4-91. For realistic values of the electron-vibrational coupling constants [9] these leads to a highly non-adiabatic nuclear motion which manifests itself, e.g., in a complex and erratic vibronic line structure of the corresponding electronic band [S-l?] or in an ultrafast non-radiative decay [7,13,14].


📜 SIMILAR VOLUMES


Non-adiabatic effects in HD+
✍ R.E. Moss; I.A. Sadler 📂 Article 📅 1986 🏛 Elsevier Science 🌐 English ⚖ 291 KB

Non-adiabatic corrections for HD+ are estimated by transforming the Hamiltonian to give an effective electrostatic potential that may be interpreted in terms of effective nuclear charges. The results compare well with previous work, particularly at large bond lengths.

Non-adiabatic effects on resonance-enhan
✍ Sima Banerjee; S. S. Bhattacharyya; Samir Saha 📂 Article 📅 1993 🏛 John Wiley and Sons 🌐 English ⚖ 948 KB

## Abstract Resonance‐enhanced Raman scattering (RERS) from the ground __X__^1^Σ~__g__~^+^(ν~__g__~ = 0, __J__~g~) state of H~2~ via the excited intermediate __C__^1^Π~__u__~(ν = 0/1/2/3, __J__~i~) state coupled non‐adiabatically with the __B__^1^Σ~__u__~^+^(ν~__iB__~ = 8/10/12/14, __J__~i~) state