Species Tag: \> 51002 \> Species Name:\> ClO
\\ Version: \> 2 \> \> chlorine monoxide
\\ Date: \> Oct. 1980 \> \> $2^\Pi$ states, v = 0
\\ Contributor:\> H. M. Pickett \> \>
\\ \> \> \>
\\ Lines Listed: \> 2610 \> Q(300.0)=\> 3272.653
\\ Freq. (GHz) $<$ \> 2983 \> Q(225.0)=\> 2279.292
\\ Max. J: \> 83 \> Q(150.0)=\> 1407.667
\\ LOGSTR0= \> -10.0 \> Q(75.00)=\> 673.132
\\ LOGSTR1= \> -11.8 \> Q(37.50)=\> 335.120
\\ Isotope Corr.: \> -0.122 \> Q(18.75)=\> 166.801
\\ Egy. (cm$^{-1}$) $>$\> 1.2 \> Q(9.375)=\> 82.528
\\ $\mu_a$ = \> 1.239 \> A=\>
\\ $\mu_b$ = \> \> B=\> 18602.865
\\ $\mu_c$ = \> \> C=\>
\end{tabbing}
The experimental lines below 200 GHz are from R. K. Kakar, E. A. Cohen,
and M. Geller, 1978, J. Mol. Spec. {\bf 70}, 243. Lines above 200 GHz
were measured at JPL by E. A. Cohen and H. M. Pickett. The lines were fit to
a fine structure Hamiltonian which included p$_D$ and q$_D$ terms and
centrifugal distortion on B to sixth power in J. The hyperfine terms in the
Hamiltonian included all off-diagonal matrix elements for a, b, c, d,
$\eta_1$, $\eta_2$, and $\eta_3$. The partition function was determined by a
sum over states to F=86 for both the $\Omega = 3/2$ and $\Omega = 1/2$ states.