The singlet excited states of fulvene and of its 6,6-dimethyl derivative: A combined study of their energy levels by absorption spectroscopy, configuration interaction, and density functional calculations

M Michael H. Palmer (School of Chemistry, University of Edinburgh 1 , Joseph Black Building, David Brewster Road, Edinburgh EH9 3FJ, Scotland,) S Søren Vrønning Hoffmann (ISA, Department of Physics and Astronomy, Aarhus University 2 , Ny Munkegade 120, DK-8000 Aarhus C,) N Nykola C. Jones (ISA, Department of Physics and Astronomy, Aarhus University 2 , Ny Munkegade 120, DK-8000 Aarhus C,) M Marcello Coreno (CNR–Istituto di Struttura della Materia (ISM), Basovizza, Trieste 34149, Italy) M Monica de Simone (IOM-CNR, Istituto Officina dei Materiali 4 , Basovizza SS-14, Km 163.5, 34149 Trieste,) C Cesare Grazioli (CNR–Istituto Officina dei Materiali (IOM), Basovizza, Trieste 34149, Italy) R R. Alan Aitken (School of Chemistry, University of St Andrews 5 , North Haugh, St Andrews, Fife KY16 9ST, Scotland,) I Iain L. J. Patterson (School of Chemistry, University of St Andrews 5 , North Haugh, St Andrews, Fife KY16 9ST, Scotland,)

Abstract

The ultraviolet and vacuum ultraviolet (VUV) photo absorption spectra of fulvene were reconsidered by a combination of configuration interaction and density functional methods and extended to the newly acquired VUV photo absorption spectrum of the 6,6-dimethylfulvene derivative, where several Rydberg states have been identified. Singlet states of fulvene were studied using multi-root multi-reference configuration interaction with the H2C unit either coplanar with, or perpendicular to the ring. In contrast to ethylene, the lowest states are coplanar. The vibrational structure of the lowest (1B2) excited states of fulvene is well reproduced by calculated values. The second singlet state of fulvene, previously assigned as 1A1 on the basis of intensity, is incompatible with the calculated planar 1A1 state, which itself is a saddle point. This state shows significant quartic character on bending, and the best interpretation of the observed UV band of fulvene is of a bent form. The UV spectral state with low onset intensity is probably a 1B1 state of CS symmetry. Theoretical Rydberg states were determined for fulvene; the closest fit to the two known Rydberg states is to the 3p and 4p states (1B1). Comparison of the separation of the 2A2 and 2B1 states in the photoelectron spectra of the two compounds, with the threshold photoelectron spectrum of fulvene, shows that the 2B1 state vibrational structure is largely lost for both molecules. A reconsideration of the interaction between the X2A2 and A2B1 ionic states has led to the identification of the 4A2 quartic state of fulvene.

Article Details

Volume / Issue Vol. 163, Issue 2
Published July 14, 2025
ISSN 0021-9606
Publisher American Institute of Physics

Journal Info

The Journal of Chemical Physics

American Institute of Physics

ISSN: 0021-9606 Physical Sciences

Authors (8)

M

Michael H. Palmer

School of Chemistry, University of Edinburgh 1 , Joseph Black Building, David Brewster Road, Edinburgh EH9 3FJ, Scotland,

S

Søren Vrønning Hoffmann

ISA, Department of Physics and Astronomy, Aarhus University 2 , Ny Munkegade 120, DK-8000 Aarhus C,

N

Nykola C. Jones

ISA, Department of Physics and Astronomy, Aarhus University 2 , Ny Munkegade 120, DK-8000 Aarhus C,

M

Marcello Coreno

CNR–Istituto di Struttura della Materia (ISM), Basovizza, Trieste 34149, Italy

M

Monica de Simone

IOM-CNR, Istituto Officina dei Materiali 4 , Basovizza SS-14, Km 163.5, 34149 Trieste,

C

Cesare Grazioli

CNR–Istituto Officina dei Materiali (IOM), Basovizza, Trieste 34149, Italy

R

R. Alan Aitken

School of Chemistry, University of St Andrews 5 , North Haugh, St Andrews, Fife KY16 9ST, Scotland,

I

Iain L. J. Patterson

School of Chemistry, University of St Andrews 5 , North Haugh, St Andrews, Fife KY16 9ST, Scotland,