\\ Species Tag:        &   48011 & Name:& CH3OOH        
\\ Version:            &       1 & & Ground  
\\ Date:       & Dec. 2005       & & 0$^+$, 0$^-$, A, E States
\\ Contributor:& B. J. Drouin    & & 
\\             &                 & & 
\\ Lines Listed:       &   46191 & Q(300.0)=&  106466.2980
\\ Freq. (GHz) $<$     &    1800 & Q(225.0)=&   68323.1834
\\ Max. J:             &      50 & Q(150.0)=&   36346.9932
\\ LOGSTR0=            &   -11.0 & Q(75.00)=&   12054.7879
\\ LOGSTR1=            &    -7.0 & Q(37.50)=&    3811.4277
\\ Isotope Corr.:      &  -0.007 & Q(18.75)=&    1139.3855
\\ Egy. (cm$^{-1}$) $>$&     0.0 & Q(9.375)=&     339.0903
\\ $\mu_a$ = & 0.606 / 0.703     & A=&42828.738  
\\ $\mu_b$ = & 0.071 / 0.133     & B=&10500.288
\\ $\mu_c$ = &      0.5          & C=& 9055.050
\headend 
 
The frequencies and dipole moment were taken from: M. Typlewski, 
T. -K. Ha, R. Meyer, A. Bauder, C. E. Blom, 1992, J.
Chem. Phys. {\bf 97}, 9. The 'c' type transition dipole moment is unknown 
so a 0.5 D dipole was assumed in the calculations.  A $K_a$ = 6 $\leftarrow$ 7 $Q$ branch
between the 0$^+$ and 0$^-$ states was reassigned for splittings due to methyl torsion (A/E)
rather than asymmetry splittings.  This results in an improved global fit to the four states.

The state specific quantum numbers, v = 0-5 correspond to the following symmetries:
\begin{table}[h]
\begin{tabular*}{\hsize}{@{\extracolsep{\fill}}c|c|c|c}
     inversion   &  $ I.R.$  & v \\
\hline
$0^+$  &  A   & 0     \\
$0^+$  &  E  & 1,2     \\
$0^-$  &  A  & 3       \\
$0^-$  &  E  & 4,5     \\
\end{tabular*}
\end{table}