1968•The Knowledge Bank (The Ohio State University)Requires access

MICROWAVE SPECTRUM, STRUCTURE AND $l$-TYPE DOUBLING OF DCNO: DEUTERO-FULMINIC ACID

H. K. Bodenseh, Manfred Winnewisser

Open publisher page 0 citations

Abstract

The microwave spectrum of the deuterated form of fulminic acid has been investigated in the frequency region from 10 to 45 GHz. For the ground vibrational state of DCNO the following rotational constants were obtained: $B_{o}(D^{12}C^{14}N^{16}O) = 10 292.51$ MHz, $B_{o}(D^{18}C^{14}N^{16}O) = 10 011.69$ MHz, $B_{o}(D^{12}C^{14}N^{18}O) = 9 759.87$ MHz. These constants yield a combined $r_{***}$ and $r_{o}$-structure: $r(C-D) = 1.027 \\pm 0.001 {\\AA}, r(C-N) = 1.175 \\pm 0.015 {\\AA}$, and $r(N-O) = 1.186 \\pm 0.015 {\\AA}$. The large uncertainties in two of the distances are due to the close proximity of the nitrogen atom to the center of gravity, as it has been observed before in the case of HCNO (refs. $^{1,2}$). For the two degenerate bending modes v*** and v*** the l-type doublets of the transition $J = 1 \\rightarrow 2$ and the two corresponding series of l-type doubling transitions have been observed. The doubling constants are: $q_{4} = 17.92 \\pm 0.05$ MHz, and $q_{5} = 38.09 \\pm 0.05$ MHz. A third series of l-type doubling transitions has been found, whose doubling constant can be expressed as a linear combination of $q_{4}$ and $q_{5}$. For both HCNO and DCNO, rotational transitions $(J = 0\\rightarrow 1 and J = 1\\rightarrow 2)$ of molecules in the following seven vibrational states are now assigned: $(00100), (0001^{1}0), (0002^{0}0), (00001^{1}), (00002^{0}), (000(11)^{\\circ}) \\Sigma^{+}$, and $(000(11)^{\\circ}) \\Sigma^{-}$. In HCNO, the difference between $\\nu_{4}$ and $\\nu_{5}$ was determined to be $200 \\pm 10 cm^{-1}$ from the relative intensities of the $(0001^{1}1^{1})$ and $(00002^{\\circ})$ vibrational satellites.

About this research paper

What this paper is about

The microwave spectrum of the deuterated form of fulminic acid has been investigated in the frequency region from 10 to 45 GHz. For the ground vibrational state of DCNO the following rotational constants were obtained: $B_{o}(D^{12}C^{14}N^{16}O) = 10 292.51$ MHz, $B_{o}(D^{18}C^{14}N^{16}O) = 10 011.69$ MHz, $B_{o}(D^{12}C^{14}N^{18}O) = 9 759.87$ MHz. These constants yield a combined $r_{***}$ and $r_{o}$-structure: $r(C-D) = 1.027 \\pm 0.001 {\\AA}, r(C-N) = 1.175 \\pm 0.015 {\\AA}$, and $r(N-O) = 1.186 \\pm 0.015 {\\AA}$. The large uncertainties in two of the distances are due to the close proximity of the nitrogen atom to the center of gravity, as it has been observed before in the case of HCNO (refs. $^{1,2}$). For the two degenerate bending modes v*** and v*** the l-type doublets of the transition $J = 1 \\rightarrow 2$ and the two corresponding series of l-type doubling transitions have been observed. The doubling constants are: $q_{4} = 17.92 \\pm 0.05$ MHz, and $q_{5} = 38.09 \\pm 0.05$ MHz. A third series of l-type doubling transitions has been found, whose doubling constant can be expressed as a linear combination of $q_{4}$ and $q_{5}$. For both HCNO and DCNO, rotational transitions $(J = 0\\rightarrow 1 and J = 1\\rightarrow 2)$ of molecules in the following seven vibrational states are now assigned: $(00100), (0001^{1}0), (0002^{0}0), (00001^{1}), (00002^{0}), (000(11)^{\\circ}) \\Sigma^{+}$, and $(000(11)^{\\circ}) \\Sigma^{-}$. In HCNO, the difference between $\\nu_{4}$ and $\\nu_{5}$ was determined to be $200 \\pm 10 cm^{-1}$ from the relative intensities of the $(0001^{1}1^{1})$ and $(00002^{\\circ})$ vibrational satellites.

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

The microwave spectrum of the deuterated form of fulminic acid has been investigated in the frequency region from 10 to 45 GHz. For the ground vibrational state of DCNO the following rotational constants were obtained: $B_{o}(D^{12}C^{14}N^{16}O) = 10 292.51$ MHz, $B_{o}(D^{18}C^{14}N^{16}O) = 10 011.69$ MHz, $B_{o}(D^{12}C^{14}N^{18}O) = 9 759.87$ MHz. These constants yield a combined $r_{***}$ and $r_{o}$-structure: $r(C-D) = 1.027 \\pm 0.001 {\\AA}, r(C-N) = 1.175 \\pm 0.015 {\\AA}$, and $r(N-O) = 1.186 \\pm 0.015 {\\AA}$. The large uncertainties in two of the distances are due to the close proximity of the nitrogen atom to the center of gravity, as it has been observed before in the case of HCNO (refs. $^{1,2}$). For the two degenerate bending modes v*** and v*** the l-type doublets of the transition $J = 1 \\rightarrow 2$ and the two corresponding series of l-type doubling transitions have been observed. The doubling constants are: $q_{4} = 17.92 \\pm 0.05$ MHz, and $q_{5} = 38.09 \\pm 0.05$ MHz. A third series of l-type doubling transitions has been found, whose doubling constant can be expressed as a linear combination of $q_{4}$ and $q_{5}$. For both HCNO and DCNO, rotational transitions $(J = 0\\rightarrow 1 and J = 1\\rightarrow 2)$ of molecules in the following seven vibrational states are now assigned: $(00100), (0001^{1}0), (0002^{0}0), (00001^{1}), (00002^{0}), (000(11)^{\\circ}) \\Sigma^{+}$, and $(000(11)^{\\circ}) \\Sigma^{-}$. In HCNO, the difference between $\\nu_{4}$ and $\\nu_{5}$ was determined to be $200 \\pm 10 cm^{-1}$ from the relative intensities of the $(0001^{1}1^{1})$ and $(00002^{\\circ})$ vibrational satellites.

Key concepts: Molecular spectroscopy, Spectroscopy, Physics, Chemistry, Crystallography, Stereochemistry, Quantum mechanics

Related papers

Back to paper searchBrowse research topicsOriginal source
MICROWAVE SPECTRUM, STRUCTURE AND $l$-TYPE DOUBLING OF DCNO: DEUTERO-FULMINIC ACID — Research Paper | ScholarLens