The anomalous behavior of the Zeeman anticrossing spectra of à 1Au acetylene: Theoretical considerations

P. Dupre, R. Jost, M. Lombardi, P. G. Green, E. Abramson, and R. W. Field have observed anomalous behavior of the anticrossing density in the Zeeman anticrossing (ZAC) spectra of gas phase A 1Au acetylene in the 42 200 to 45 300 cm−1 energy range. To best explain this result, they hypothesize a large singlet–triplet coupling due to the existence of a linear isomerization barrier connecting a triplet‐excited cis‐ and trans‐acetylene in the vicinity of the studied energy range (∼45 500 cm−1). Theoretically such a linear stationary point, however, must have two different degenerate bending vibrational frequencies which are either imaginary or exactly zero. Neither case has yet been experimentally detected. Here, we have studied the two lowest‐lying linear triplet‐excited‐state stationary points of acetylene, 3Σ+u and 3Δu, to see if they fit Dupre et al.’s hypothesis. We have completed geometry optimization and harmonic vibrational frequency analysis using complete‐active‐space self‐consistent field (CASSCF)...

[1]  P. Dupré Study of Zeeman anticrossing spectra of the Ã1Au state of the acetylene molecule (C2H2) by Fourier transform: product ϱvibV〉 and isomerization barrier , 1995 .

[2]  R. Field,et al.  Quantum beat spectroscopic studies of Zeeman anticrossings in the Ã1Au state of the acetylene molecule (C2H2) , 1995 .

[3]  J. Gauss,et al.  Some predictions relevant to future spectroscopic observation of S1 vinylidene , 1994 .

[4]  J. Stanton,et al.  Stationary points on the S1 potential energy surface of C2H2 , 1994 .

[5]  M. Drabbels,et al.  A study of the singlet–triplet perturbations in the à 1Au state of acetylene by high resolution ultraviolet spectroscopy , 1994 .

[6]  P. G. Green,et al.  Characterization of a large single-triplet coupling in the à state of the acetylene molecule , 1993 .

[7]  George Vacek,et al.  Low-lying triplet electronic states of acetylene:cis3B2 and3A2,trans3Bu and3Au , 1993 .

[8]  T. Crawford,et al.  The balance between theoretical method and basis set quality: A systematic study of equilibrium geometries, dipole moments, harmonic vibrational frequencies, and infrared intensities , 1993 .

[9]  H. Abe,et al.  Nonradiative process induced by external magnetic fields in the C2H2 Ã 1Au state near predissociation limit , 1993 .

[10]  Henry F. Schaefer,et al.  Isomerization reactions on the lowest potential energy hypersurface of triplet vinylidene and triplet acetylene , 1993 .

[11]  H. Schaefer,et al.  A systematic theoretical study of the harmonic vibrational frequencies for polyatomic molecules: The single, double, and perturbative triple excitation coupled‐cluster [CCSD(T)] method , 1993 .

[12]  Christopher S. Johnson,et al.  Characterization of the X̃ 1A’ state of isocyanic acid , 1993 .

[13]  N. Ochi,et al.  Rovibronic level structure of electronically excited acetylene (A1Au) in a supersonic jet as studied by laser-induced fluorescence and Zeeman quantum beat spectroscopy , 1991 .

[14]  R. Field,et al.  Anomalous behavior of the anticrossing density as a function of excitation energy in the C2H2 molecule , 1991 .

[15]  Klaus Ruedenberg,et al.  Bifurcations and transition states , 1986 .

[16]  Henry F. Schaefer,et al.  The shape‐driven graphical unitary group approach to the electron correlation problem. Application to the ethylene molecule , 1982 .

[17]  Lawrence B. Harding,et al.  AB INITIO STUDIES OF (1,2)-HYDROGEN MIGRATIONS IN OPEN-SHELL HYDROCARBONS: VINYL RADICAL, ETHYL RADICAL, AND TRIPLET METHYLCARBENE , 1981 .

[18]  S. Hurlock,et al.  Infrared bands of 12C2HD , 1976 .

[19]  D. Demoulin The shapes of some excited states of acetylene , 1975 .

[20]  T. H. Dunning Gaussian Basis Functions for Use in Molecular Calculations. III. Contraction of (10s6p) Atomic Basis Sets for the First‐Row Atoms , 1970 .

[21]  George S. Hammond,et al.  A Correlation of Reaction Rates , 1955 .