FIR LASER STARK SPECTROSCOPY OF $CH_{3}OH$ AT $190 \mu m$ and $195 \mu m$.
G. R. Sudhakaran, Indranath Mukhopadhyay, J. C. Sarker, R. L. Bhattacharjee, Lawrence H. Johnston
Abstract
G. R. Sudhakaran, Indranath Mukhopadhyay, J. C. Sarker, R. L. Bhattacharjee, Lawrence H. Johnston
Abstract
The FIR laser Stark spectrum of methanol has been investigated at $\\lambda = 190 \\mu m$ and $195 \\mu m$ of the DCN laser. The spectrum has been taken up to 60,000 volts/cm both parallel and perpendicular polarizations. The low field structure observed with the $190 \\mu m$ line is assigned as the $J_{k} = 173 \\leftarrow 162 E_{2}. v_{t} = 0$ torsional state. A relatively strong transition observed with the $195 \\mu m$ and also the $195 \\mu m$ line is tentatively identified as the $J_{k} = 114 \\leftarrow 103 E_{1}, v_{t} = 0$ torsional state.
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The FIR laser Stark spectrum of methanol has been investigated at $\\lambda = 190 \\mu m$ and $195 \\mu m$ of the DCN laser. The spectrum has been taken up to 60,000 volts/cm both parallel and perpendicular polarizations. The low field structure observed with the $190 \\mu m$ line is assigned as the $J_{k} = 173 \\leftarrow 162 E_{2}. v_{t} = 0$ torsional state. A relatively strong transition observed with the $195 \\mu m$ and also the $195 \\mu m$ line is tentatively identified as the $J_{k} = 114 \\leftarrow 103 E_{1}, v_{t} = 0$ torsional state.
Key concepts: Engineering physics, Physics, Library science, Engineering, Computer science