Photoelectron spectroscopy of ammonia: Mode-dependent vibrational autoionization

Vibrational autoionization of state-selective jet-cooled methanethiol (CH3SH) investigated with infrared + vacuum-ultraviolet photoionization

Vibrational autoionization of Rydberg states provides key information about nonadiabatic processes above an ionization threshold. We employed time-of-flight mass detection of CH₃SH⁺ to record vibrational-state selective photo-ionization efficiency (PIE) spectra of jet-cooled methanethiol (CH₃SH) on exciting CH₃SH to a specific vibrationally excited state with an infrared (IR) laser, followed by excitation with a tunable laser in the vacuum-ultraviolet (VUV) region for ionization. Autoionizing Rydberg states assigned to the ns, np, nd and nf series are identified. When IR light at 2601 (ν₃, SH stretching mode) and 2948 cm^-1 (ν₂, CH₃ symmetric stretching mode) was employed, the Rydberg series converged to the respective vibrationally excited (ν₃ and ν₂) states of CH₃SH⁺. When IR light at 3014 cm^-1 (overlapped ν₁/ν₉, CH₃ antisymmetric stretching and CH₂ antisymmetric stretching modes) was employed, Rydberg series converging to two vibrationally excited states (ν₁ and ν₉) of CH₃SH⁺ were observed. When IR light at 2867 cm^-1 (2ν₁₀, overtone of CH₃ deformation mode) and 2892 cm^-1 (2ν₄, overtone of CH₂ scissoring mode) was employed, both Δν = -1 and Δν = -2 ionization transitions were observed; there is evidence for direct ionization from the initial state into the CH₃SH⁺ (ν₄⁺ = 1) continuum. In all observed IR-VUV-PIE spectra, the ns and nd series show intensity greater than the other Rydberg series, which is consistent with the fact that the highest-occupied molecular orbital of CH₃SH is a p-like lone pair orbital on the S atom. The quantum yields for autoionization of various vibrational excited states are discussed. Values of ν₁ = 3035, ν₂ = 2884, ν₃ = 2514, and ν₉ = 2936 cm^-1 for CH₃SH⁺ derived from the converged limits agree satisfactorily with values observed for Ar-tagged CH₃SH⁺ at 3026, 2879, 2502, and 2933 cm^-1.

Molecular collisions coming into focus

Control over molecules in a Stark decelerator enables the measurement of diffraction oscillations in NO-atom scattering.

VIBRATIONAL AUTOIONIZATION IN POLYATOMIC MOLECULES

▪ Abstract  The vibrationally autoionizing Rydberg states of small polyatomic molecules provide a fascinating laboratory in which to study fundamental nonadiabatic processes. In this review, recent results on the vibrational mode dependence of vibrational autoionization are discussed. In general, autoionization rates depend strongly on the character of the normal mode driving the process and on the electronic character of the Rydberg electron. Although quantitative calculations based on multichannel quantum defect theory are available for some polyatomic molecules, including H3, only qualitative information exists for most molecules. This review shows how qualitative information, such as Walsh diagrams along different normal coordinates of the molecule, can provide insight into the vibrational autoionization rates.

Ion rotational distributions following vibrational autoionization of the Rydberg states of water

Double-resonance laser excitation and high-resolution energy dispersive photoelectron spectroscopy were used to determine the ionic rotational-state distributions following vibrational autoionization of Rydberg states of water having principal quantum number n=8-10 and converging to the X (2)B(1) (1,0,0) state of H(2)O(+). Where possible, these states were identified by comparison with results of a calculation based on multichannel quantum defect theory. Symmetry and angular momentum constraints link the observed ionic rotational states to particular values of the orbital angular momentum of the Rydberg electron, l, and to the partial-wave composition of the ejected electron. In particular, this connection allows an unambiguous determination of the even or odd character of the partial waves and provides a test of the predicted character of the autoionizing resonances. The effects of l mixing induced by the nonspherical nature of the ionic field are plainly evident in the ion distributions. The present results also allow a tentative assignment of some resonances to the previously unidentified np Rydberg states.

Mode dependent vibrational autoionization of Rydberg states of NO2. II. Comparing the symmetric stretching and bending vibrations

Triple-resonance excitation and high-resolution photoelectron spectroscopy are combined to characterize the mode selectivity of vibrational autoionization of the high Rydberg states of NO2. Photoelectron spectra and vibrational branching fractions are reported for autoionizing Rydberg states converging to the NO2+ X 1Sigmag +(110) state, that is, with one quantum in the symmetric stretch, nu1, and one quantum in the bending vibration, nu2. These results indicate that autoionization proceeds most efficiently through the loss of one quantum from the symmetric stretch rather than from the bending vibration. The implications of this result are discussed in terms of the autoionization mechanism.