\\ Species Tag:        &   34004 & Name:&  H2O2          
\\ Version:            &       4 & & Hydrogen peroxide, 
\\ Date:       &  Sept. 1995     & & H$_2$O$_2$,
\\ Contributor:&  J. C. Pearson  & & first 5 torsional states
\\             &                 & &
\\ Lines Listed:       &   38357 & Q(300.0)=&     9785.505
\\ Freq. (GHz) $<$     &    9999 & Q(225.0)=&     5760.578
\\ Max. J:             &      60 & Q(150.0)=&     2814.265
\\ LOGSTR0=            &   -10.0 & Q(75.00)=&      895.518
\\ LOGSTR1=            &   -10.0 & Q(37.50)=&      288.930
\\ Isotope Corr.:      &     0.0 & Q(18.75)=&       88.856
\\ Egy. (cm$^{-1}$) $>$&     0.0 & Q(9.375)=&       26.680
\\ $\mu_a$ = &                   & A=& 301878.
\\ $\mu_b$ = &                   & B=&  26211.9
\\ $\mu_c$ = &  1.5724           & C=&  25099.14
\headend

The spectral lines and method of calculation are from D. T. Petkie, T.
M. Goyette, J. J. Holton, F. C. De Lucia and P. Helminger, 1995, J.
Mol. Spect. {\bf 171}, 145-159. This paper included the previous lines
of P. Helminger, W. C. Bowman and F. C. De Lucia, 1981, J. Mol. Spect.
{\bf 85}, 120. E. A. Cohen and H. M. Pickett, 1981, J. Mol. Spect. {\bf
87}, 582.  Also used in the analysis were energy levels from C.
Cammy-Peyret, J.-M. Flaud, J. W. C. Johns and M. Noel, 1992, J. Mol.
Spect. {\bf 155}, 84-104. Dipoles are from A. Perrin, J.-M. Flaud, C.
Camy-Peyret, R. Schermaul, M. Winnewisser, \mbox{J.-Y.} Mandin, V.
Danna, M. Badaoui, and J. Koput, Line Intensities in the Far-Infrared
Spectrum of  H$_2$O$_2$, in preparation.

The dipole moment is c-type in all cases. The value given is for the
ground state transitions only.  The vibrational quantum number
designation is as follows:

\begin{center}\begin{tabular}{cccc}
v(catalog)  & n  & $\tau_{even}$ & $\tau_{odd}$ \\
0           & 0  &    1 &             2 \\
1           & 1  &    1 &             2 \\
2           & 2  &    1 &             2 \\
3           & 0  &    4 &             3 \\
4           & 1  &    4 &             3 \\
\end{tabular}\end{center}

$\tau_{even}$ is the value of $\tau$ when K$_a$ is even, and $\tau_{odd}$ 
is the value of $\tau$ when K$_a$ is odd.  The analysis must be separated into
$\tau$ = odd and $\tau$ = even parts due to torsional staggering.