The pure rotational spectrum of the ground state of NH3
This data file was constructed by fitting to the line positions and
intensities in the HITRAN 2008 (http://www.hitran.com)
database. The fit was restricted to J
< 16, and is sufficient to reproduce the line positions to better
than 0.001 cm-1 and the intensities to better than 10-20
cm2 cm-1 Molecule-1. There
are two points that are slightly non-standard:
- The point group used is D3h, rather than C3v.
This is necessary to account for the inversion doubling in the ground
state, which appears in the data file as two vibrational states:
- s/0+ with A1'
symmetry
- a/0- with A2"
symmetry
- To fit the K = 3n
levels
requires three perturbation
operators:
- <0+|J+-^6|0+>
= J+6 + J-6
- <0+|J^2J+-|0+>
= J2(J+6
+ J-6)
- <0+|J+-^12|0+>
= J+12 + J-12
Two separate data files are provided:
- nh3x0.pgo This has the two
inversion doublets in separate manifolds (s and a), with a transition
moment acting between the two manifolds. This is a good starting point
for simulating electronic spectra, where the transitions will typically
be from one inversion doublet or other.
- nh3x0one.pgo This has the
two inversion doublets in the same manifold. The resulting energy
levels will be the same, but as the dipole moment now acts within the
manifold, the Stark effect in the ground state can be simulated with
this file.