\\ Species Tag:        &   51002 & Name:&  ClO            
\\ Version:            &       3 & & Chlorine monoxide,
\\ Date:       & Jan. 1991       & & X $^2\Pi$ states, v = 0
\\ Contributor:&  E. A. Cohen    & & 
\\             &                 & & 
\\ Lines Listed:       &    2585 & Q(300.0)=&     3349.655
\\ Freq. (GHz) $<$     &    2983 & Q(225.0)=&     2307.810
\\ Max. J:             &      83 & Q(150.0)=&     1424.624
\\ LOGSTR0=            &   -10.0 & Q(75.00)=&      689.287
\\ LOGSTR1=            &   -11.5 & Q(37.50)=&      351.318
\\ Isotope Corr.:      &  -0.122 & Q(18.75)=&      183.316
\\ Egy. (cm$^{-1}$) $>$&     0.0 & Q(9.375)=&       99.701
\\ $\mu_a$ = &  1.2974           & A=& 
\\ $\mu_b$ = &                   & B=& 18601.791
\\ $\mu_c$ = &                   & C=& 
\headend

	The experimental lines are from R. K. Kakar, E. A. Cohen,
and M. Geller, 1978, J. Mol. Spect. {\bf 70}, 243,
and E. A. Cohen, H. M. Pickett, and M. Geller, 1984, J. Mol. Spect. {\bf 
106}, 430.  The millimeter and submillimeter data were combined with the FT
infrared data of J. B. Burkholder {\it et al.}, 1987, J. Mol. Spect. {\bf 124}, 139,
in a simultaneous fit to both vibrational states.  The partition function is
a sum over the ground and first vibrational state up to
F = 90 for both the $\Omega = 3/2$ and $\Omega = 1/2$ states.  The dipole moment
is from D. Yaron, K. Peterson, and W. Klemperer, 1988, J. Chem. Phys.
{\bf 88,}  4702.