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\title{HIGH-RESOLUTION STUDY OF THE ROTATIONAL SPECTRUM OF 2-AMINOPROP-2-ENENITRILE}


\author{\underline{\FirstName K. \LastName LUKOV\'{A}}}
\address{Institute of Physics, University of Kassel, Heinrich-Plett-Strasse 40 D-34132 Kassel, Germany;  and Department of Analytical Chemistry, University of Chemistry and Technology, Technick\'{a} 5, 166 28, Prague, Czech Republic}

\author{{\FirstName L. \LastName KOLESNIKOV\'{A}},
 {\FirstName J. \LastName KOUCK\'{Y}},  {\FirstName P. \LastName KANIA}, 
 {\FirstName \v{S}. \LastName URBAN}}
\address{Department of Analytical Chemistry, University of Chemistry and Technology, Technick\'{a} 5, 166 28, Prague, Czech Republic}

\author{{\FirstName J.C. \LastName GUILLEMIN}}
\address{Institut des Sciences Chimiques de Rennes, CNRS UMR 6226, Universit\'{e} Rennes 1, 263 Avenue G\'{e}n\'{e}ral Leclerc, 35700 Rennes, France}


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\fancyhead[C]{{\footnotesize \textit{HRMS, 28th Colloquium, Dijon, France,
  Aug. 28 - Sept. 1, 2023}}}
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The high-resolution rotational spectrum of 2-aminopropen-2-enitrile (APN) was recorded in two frequency ranges: 204--240 and 292--328 GHz employing the Prague semiconductor millimetre-wave spectrometer\footnote{
\href{https://doi.org/10.1016/j.molstruc.2006.02.025}{doi:10.1016/j.molstruc.2006.02.025},
P. Kania, L. St\v{r}\'{i}tesk\'{a}, M. \v{S}ime\v{c}kov\'{a}, \v{S}. Urban, \textit{J. Mol. Struct.},
\textbf{795}, 209-218, (2006).}. Several hundreds of \emph{a}- and \emph{b}-type transitions corresponding to the 0$^{+}$ and 0$^{-}$ inversion states arising from the inversion motion of the amino group were identified and assigned. Bauder et al.\footnote{
\href{https://doi.org/10.1016/0009-2614(83)85003-9}{doi:10.1016/0009-2614(83)85003-9},
A. Bauder, T.-K. Ha, \textit{Chem. Phys. Lett.},
\textbf{97}, 135-140, (1983).} estimated the energy difference between the energy levels to be 54 $\pm$ 22 cm$^{-1}$ based on the relative intensity measurements. Since no \emph{c}-type transitions connecting the inversion states were assigned in the present spectrum, the value of $\Delta E$ separating the levels could not be derived with a better accuracy. Hence, the rotational transitions from both vibrational states were analysed separately by means of the A-reduced Hamiltonian using the SPCAT/SPFIT program package\footnote{
\href{https://doi.org/10.1016/0022-2852(91)90393-O}{doi:10.1016/0022-2852(91)90393-O},
H. M. Pickett, \textit{J. Mol. Spectrosc.},
\textbf{148}, 371-377, (1991).}. The experimentally determined molecular parameters of APN are presented in comparison with their quantum chemical counterparts. 

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