\\ Species Tag:        &   75003 & Name:& H2NCH2COOH II
\\ Version:            &       1 & & Glycine, Conformer II
\\ Date:       &  Jan. 1996      & & ground and first
\\ Contributor:&  H. S. P.  M\"uller & & excited torsional states
\\             &                 & & 
\\ Lines Listed:       &   26544 & Q(300.0)=&   124879.8881
\\ Freq. (GHz) $<$     &    1000 & Q(225.0)=&   100530.4504
\\ Max. J:             &      40 & Q(150.0)=&    68673.2239
\\ LOGSTR0=            &   -11.0 & Q(75.00)=&    29376.5224
\\ LOGSTR1=            &    -8.0 & Q(37.50)=&    10752.5529
\\ Isotope Corr.:      &         & Q(18.75)=&     3810.1565
\\ Egy. (cm$^{-1}$) $>$& 700.0   & Q(9.375)=&     1350.3826
\\ $\mu_a$ = & 5.372             & A=& 10130.152 
\\ $\mu_b$ = & 0.930             & B=&  4071.5075 
\\ $\mu_c$ = &                   & C=&  3007.4892 
\headend 
This conformer of glycine is $\approx$700 cm$^{-1}$ higher in energy
than conformer I (2, 3). 
The data were taken from (1) R. D. Suenram and F. J. Lovas, 1978, 
J. Mol. Spectrosc. {\bf 72}, 372 (millimeterwave region), and
(2) F. J. Lovas, Y. Kawashima, J.-U. Grabow, R. D. Suenram, G. T. Fraser, 
and E. Hirota, 1995, Astrophys. J. Lett. {\bf 455}, 201; (microwave region, 
dipole moment, and $^{14}$N quadrupole coupling).

The ground and first excited states have been fit simultaneously, 
using only changes in the vibrational constants and $D_{JK}$ for the 
excited state. The estimated torsional energy of 87 cm$^{-1}$ has been taken 
from an $ab \ initio$ calculation (SCF/DZP, scaled by 0.9; (3) C. H. Hu, 
M. Shen, and H. F. Schaefer, III, 1993, J. Am. Chem. Soc. {\bf 115}, 2923).

For low $J$ ($<$ 10) hyperfine splittings are included in the catalog. 

For the relative intensities between ground and first excited torsional states 
the approximate position of the torsional state was taken into account. 
Because there are several low lying vibrational modes that have not been 
investgated, the partition function was calculated for the ground state
of the lower energy conformation including the nitrogen spin degeneracy.  
The partition function was calculated up to $J$ = 150 because of the 
small rotational constants.