Tables of data used in the paper "High Temperature Measurements in the Region
of the Bending Fundamental of H^1^3C^1^5N"

by Wolfgang Quapp, V.Melnikov, Georg Ch. Mellau.

    The file contain the original data and the deviations from
the least-squares fits of the data.  
The files are in ascii so that they may be
easily read by any computer.

    The file is broken into many separate groups of data.  The first line
in the file for each group gives the designation of the vibrational transition
involved, and in many cases the name of the original spectrum.  
Spectra that are
designated by one or two letters usually correspond to the "runs" given in
table 1 of the paper by Maki, Quapp, and Klee in 
J. Mol. Spectrosc. 171, 420-434 (1995).

    Each group contains data for only one vibrational transition.  Normally the
e and f sublevels are treated as different levels that give rise to diffent
vibrational transitions.  However, the e and f sub-levels are constrained to
have the same non-rotational vibrational frequency.  If the label does not give
an e or f designation when one might be expected, then the transitions given in
the group are for unresolved e and f doublets.

    The fourth line and following lines in each data-group contain the
measurements that were fit.  Each line contains the measured wavenumber of
an absorption or emission line (in units of cm^-^1), the deviation of that
measurement from the calculated line position (O-C), the upper state rotational
quantum number (J'), the lower state rotational quantum number (J"), and the
uncertainty assigned to the measurement.

    At the end of each data-group the rms deviation of that set of measurements
is given.

    If the wavenumber is followed by an asterisk (*), then the measurement was
given a weight of zero regardless of what the uncertainty column may contain.
If there is no asterisk, then the measurement was given a weight that was
equal to the reciprocal of the square of the uncertainty of the measurement
(given in the last column).

    Near the end of the file, the microwave or mm-wave measurements used in the
fit are given.  Those measurements are given in frequency units, MHz, although
the rms deviations are given in cm^-^1 units.  To calculate the weight to be
given to these measurements in the least-squares fit, the uncertainty is first
converted to cm^-^1 units to conform with the weights given for the infrared
measurements.

    These files were all computer generated as output from the least-squares
fit of the data that was used to determine the constants given in Tables 3-6
of this paper.