1994•The Knowledge Bank (The Ohio State University)Requires access

THE MICROWAVE SPECTRUM, STRUCTURE AND TUNNELING MOTION OF THE ARGON-KETENE VAN DER WAALS COMPLEX

Ryan D. Molloy, C. W. Gillies, Jennifer Z. Gillies, Frank J. Lovas

Open publisher page 0 citations

Abstract

Rotational spectra of $Ar-CH_{2}CO$ and $Ar-CD_{2}CO$ were observed with a pulsed-beam Fourier-transform microwave spectrometer. Two states exhibiting strong {b}-type and weak {a}-type transitions were assigned and fit separately to an asymmetrical top Watson Hamiltonian for each isotopomer. Relative intensities and nuclear spin weights indicate the spectral splitting of transitions arises from an internal rotation about the C=C=O axis of ketene which exchanges the pair of hydrogen (deuterium) nuclei in the two isotopomers. The spectral constants in MHz obtained from the fit for the ground state of $Ar-CH_{2}CO$ are A = 10447.926(1) = 1918.281(40), and C = 1606.703(36). The moments of inertia for the two isotopomers give an argon-ketene center of mass separation $R_{cm}$ =3.60 {\\AA} and an Ar-cm-C angle of $83^{\\circ}$. Although the hydrogen positions are not well determined, the effective geometry is assumed to be planar.

About this research paper

What this paper is about

Rotational spectra of $Ar-CH_{2}CO$ and $Ar-CD_{2}CO$ were observed with a pulsed-beam Fourier-transform microwave spectrometer. Two states exhibiting strong {b}-type and weak {a}-type transitions were assigned and fit separately to an asymmetrical top Watson Hamiltonian for each isotopomer. Relative intensities and nuclear spin weights indicate the spectral splitting of transitions arises from an internal rotation about the C=C=O axis of ketene which exchanges the pair of hydrogen (deuterium) nuclei in the two isotopomers. The spectral constants in MHz obtained from the fit for the ground state of $Ar-CH_{2}CO$ are A = 10447.926(1) = 1918.281(40), and C = 1606.703(36). The moments of inertia for the two isotopomers give an argon-ketene center of mass separation $R_{cm}$ =3.60 {\\AA} and an Ar-cm-C angle of $83^{\\circ}$. Although the hydrogen positions are not well determined, the effective geometry is assumed to be planar.

Why it matters

A significance statement is not available in the OpenAlex record.

Key contribution

A contribution statement is not available in the OpenAlex record.

Method / approach

Method details are not available in the OpenAlex metadata.

Main findings

Findings are not separately available in the OpenAlex metadata.

Limitations

Limitations are not available in the OpenAlex metadata.

Applications

Application details are not available in the OpenAlex metadata.

Available abstract

Rotational spectra of $Ar-CH_{2}CO$ and $Ar-CD_{2}CO$ were observed with a pulsed-beam Fourier-transform microwave spectrometer. Two states exhibiting strong {b}-type and weak {a}-type transitions were assigned and fit separately to an asymmetrical top Watson Hamiltonian for each isotopomer. Relative intensities and nuclear spin weights indicate the spectral splitting of transitions arises from an internal rotation about the C=C=O axis of ketene which exchanges the pair of hydrogen (deuterium) nuclei in the two isotopomers. The spectral constants in MHz obtained from the fit for the ground state of $Ar-CH_{2}CO$ are A = 10447.926(1) = 1918.281(40), and C = 1606.703(36). The moments of inertia for the two isotopomers give an argon-ketene center of mass separation $R_{cm}$ =3.60 {\\AA} and an Ar-cm-C angle of $83^{\\circ}$. Although the hydrogen positions are not well determined, the effective geometry is assumed to be planar.

Key concepts: van der Waals force, Argon, Microwave, Ketene, Quantum tunnelling, Van der Waals strain, Physics, Spectrum (functional analysis)

Related papers

Back to paper searchBrowse research topicsOriginal source
THE MICROWAVE SPECTRUM, STRUCTURE AND TUNNELING MOTION OF THE ARGON-KETENE VAN DER WAALS COMPLEX — Research Paper | ScholarLens