\\ Species Tag:        &    4001 & Name:&  H2D+          
\\ Version:            &       2 & &
\\ Date:       &  Jan. 2010      & &
\\ Contributor:&  B. J. Drouin & &
\\             &                 & &
\\ Lines Listed:       &      32 & Q(300.0)=&       76.4529
\\ Freq. (GHz) $<$     &    7550 & Q(225.0)=&       49.9615
\\ Max. J:             &       5 & Q(150.0)=&       27.5467
\\ LOGSTR0=            &    -7.2 & Q(75.00)=&        9.7322
\\ LOGSTR1=            &    -3.4 & Q(37.50)=&        3.1037
\\ Isotope Corr.:      &  -3.347 & Q(18.75)=&        1.2151
\\ Egy. (cm$^{-1}$) $>$&     0.0 & Q(9.375)=&        1.0037
\\ $\mu_a$ = & 0.6               & A=&1302323.7
\\ $\mu_b$ = &                   & B=& 873563.25
\\ $\mu_c$ = &                   & C=& 497767.19
\headend

The frequency fit included rotational lines measured by Saito 
{\it et al.}, 1985, J. Chem.~Phys.~{\bf 82}, 45; Amano and Hirao J. Molec. Spectrosc. 233, 7-15 (2005); Asvany et al. Phys. Rev. Lett. 100, 233004 (2008); and Yonezu et al. J. Molec. Spectrosc. 256, 238-241 (2009 Infrared combination differences from Polyansky \& Tennyson, J. Chem. Phys. 110, 5056-5064 (1999).  This entry follows the analysis of Yonezu et al. closely.  The partition function was calculated by predicting up to J = 25, increasing the prediction beyond J = 25 did not alter the value at 300 K.