1991•The Knowledge Bank (The Ohio State University)Requires access

STARK SPECTROSCOPY OF $^{13}CD_{3}OH$ AND $CH_{3}OD$ WITH THE HCN LASER.

G. R. Sudhakaran, R. M. Lees, R. L. Bhattacharjee, Indranath Mukhopadhyay

Open publisher page 0 citations

Abstract

Laser Stark Spectra of $^{13}CD_{3}OH$ and $CH_{3}OD$ were investigated at the $\\lambda = 311 \\mu m$ and 337 $\\mu m$ lines of the HCN laser. The spectra were taken for both parallel and perpendicular polarizations at Stark electric fields up to 60000 V/cm. For $^{13}CD_{3}OH$, the extensive series of absorption lines observed at 311 $\\mu m$ were assigned to the $J = 8$ to 12 members of the $K = 2 \\leftarrow 3 E_{1}$ Q branch in the $v_{t} = 1$ torsional state. One of the resonances observed at $337 \\mu m$ was tentatively identified as the $J_{k} - 18_{2} \\leftarrow 17_{1}A; v_{t} = 0$ transition. For $CH_{3}OD$, numerous families of resonances were observed at both of the laser lines. The Q branch transition observed at $311 \\mu m$ was assigned as $J_{k} = 18_{1} \\leftarrow 18_{0} E_{2}, v_{t} = 1$ torsional state. Zero field frequencies for all the assigned transitions are given with improved accuracy over those calculated from available molecular constants.

About this research paper

What this paper is about

Laser Stark Spectra of $^{13}CD_{3}OH$ and $CH_{3}OD$ were investigated at the $\\lambda = 311 \\mu m$ and 337 $\\mu m$ lines of the HCN laser. The spectra were taken for both parallel and perpendicular polarizations at Stark electric fields up to 60000 V/cm. For $^{13}CD_{3}OH$, the extensive series of absorption lines observed at 311 $\\mu m$ were assigned to the $J = 8$ to 12 members of the $K = 2 \\leftarrow 3 E_{1}$ Q branch in the $v_{t} = 1$ torsional state. One of the resonances observed at $337 \\mu m$ was tentatively identified as the $J_{k} - 18_{2} \\leftarrow 17_{1}A; v_{t} = 0$ transition. For $CH_{3}OD$, numerous families of resonances were observed at both of the laser lines. The Q branch transition observed at $311 \\mu m$ was assigned as $J_{k} = 18_{1} \\leftarrow 18_{0} E_{2}, v_{t} = 1$ torsional state. Zero field frequencies for all the assigned transitions are given with improved accuracy over those calculated from available molecular constants.

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

Laser Stark Spectra of $^{13}CD_{3}OH$ and $CH_{3}OD$ were investigated at the $\\lambda = 311 \\mu m$ and 337 $\\mu m$ lines of the HCN laser. The spectra were taken for both parallel and perpendicular polarizations at Stark electric fields up to 60000 V/cm. For $^{13}CD_{3}OH$, the extensive series of absorption lines observed at 311 $\\mu m$ were assigned to the $J = 8$ to 12 members of the $K = 2 \\leftarrow 3 E_{1}$ Q branch in the $v_{t} = 1$ torsional state. One of the resonances observed at $337 \\mu m$ was tentatively identified as the $J_{k} - 18_{2} \\leftarrow 17_{1}A; v_{t} = 0$ transition. For $CH_{3}OD$, numerous families of resonances were observed at both of the laser lines. The Q branch transition observed at $311 \\mu m$ was assigned as $J_{k} = 18_{1} \\leftarrow 18_{0} E_{2}, v_{t} = 1$ torsional state. Zero field frequencies for all the assigned transitions are given with improved accuracy over those calculated from available molecular constants.

Key concepts: Spectroscopy, Laser, Chemistry, Physics, Optics, Quantum mechanics

Related papers

Back to paper searchBrowse research topicsOriginal source
STARK SPECTROSCOPY OF $^{13}CD_{3}OH$ AND $CH_{3}OD$ WITH THE HCN LASER. — Research Paper | ScholarLens