\\ Species Tag:        &   64001 & Name:&  S2            
\\ Version:            &       2 & &Diatomic sulfur
\\ Date:       &  Oct. 1989      & & 
\\ Contributor:&  H. M. Pickett & &
\\             &                 & &
\\ Lines Listed:       &     174 & Q(300.0)=&      989.464
\\ Freq. (GHz) $<$     &    2823 & Q(225.0)=&      725.604
\\ Max. J:             &      71 & Q(150.0)=&      462.488
\\ LOGSTR0=            &    -8.4 & Q(75.00)=&      203.751
\\ LOGSTR1=            &    -9.3 & Q(37.50)=&       82.130
\\ Isotope Corr.:      &  -0.044 & Q(18.75)=&       30.733
\\ Egy. (cm$^{-1}$) $>$&     0.0 & Q(9.375)=&       12.437
\\ $\mu_a$ = &                   & A=& 
\\ $\mu_b$ = &                   & B=& 8831.2
\\ $\mu_c$ = &                   & C=& 
\headend 

	The experimentally measured lines are given in H. M. Pickett and T. L.
Boyd, 1979, J. Mol. Spect. {\bf 75}, 53.  Additional combination differences 
were taken from E.~H. Fink, H. Kruse, and D. A. Ramsay, 1986, J. Mol.~Spect.~
{\bf 119}, 377.  The intensities of the magnetic dipole allowed transitions were
calculated using the g values given in Pickett and Boyd.  Hund's case (b)
nomenclature is used even though the states are closer to Hund's case (a) for
low J.  The J = N + 1 states correlate with $\Sigma = 0$, and the J = N $-$ 1 and
J = N states correlate with $\Sigma =  \pm 1$ states of p = $\pm$ ($-$1)$^J$
inversion parity, respectively.  The value of Q is determined from a sum over states to J = 80.