README FILE=============================================== 
Updated ULB/IASB/Reims H2O lines file converted in HITRAN format

Linelist available from http://www.ulb.ac.be/cpm/
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Reference:
These data should be referred to as:
- Coheur P.-F., Fally S., Carleer M., Clerbaux C., Colin R., Jenouvrier A., Mérienne M.-F., Hermans C., Vandaele A. C., JQSRT, 74, 2002, 493-510
for frequencies, intensities, self-broadened halfwidths, N2-broadened halfwidths and N2-induced pressure shifts. 

- Fally S., Coheur P.-F., Carleer M., Clerbaux C., Colin R., Jenouvrier A., Mérienne M.-F., Hermans C., Vandaele A. C., JQSRT, 82, 2003, 119-132 
for air-broadened halfwidths and air-induced pressure shifts.

- Zobov N. F. et al., to be published
for line assignments

Reading (HITRAN) Format
(I2,I1,F12.6,1P2E10.3,0P2F5.4,F10.4,F4.2,0PF8.6,2I3,2(4I2,2A1),3I1,6I1))

Molecule number (I2) 
set to 1 for H20 

Isotopomer number (I1) 

Vacuum wavenumber in cm-1 (F12.6)

Intensity in cm-1/(molecule.cm-2) @296K (E10.3)
Calculated from intensities recorded at 291.3 K, using equation of Giver et al., JQSRT, 2000
For unassigned lines, the temperature correction is not applied.

Weighted transition moment-squared in Debye2 (E10.3)
Not provided

Air-broadened halfwidth (HWHM) in cm-1/atm @296K (F5.4)
Calculated from air-broadened halfwidth recorded at 289.0 K
In several cases, values are obtained from nitrogen-broadened halfwidths recorded at 291.3 K using an  empirical multiplicative factor of 0.98 (=Median of the air-to-N2 ratio) in order to reproduce air-broadened halfwidths (See reference indices to identify the buffer gas)
Values are converted to 296 K using equation [1] of Toth et al., JQSRT, 1998
For unassigned lines, the temperature correction is not applied.
Set to 0.090 (averaged value) when experimental value were unattainable 

Self-broadening halfwidth (HWHM)  in cm-1/atm @296K (F5.4)
Calculated from self-broadened halfwidth recorded at 291.3 K, using equation [1] of Toth et al., JQSRT, 1998, 
For unassigned lines, the temperature correction is not applied.
Set to 0.441 (averaged value) when experimental value were unattainable
!!!May exceed 1.0 >> written in F5.3 format, reading in F5.4 OK

Lower state energy in cm-1 (F10.4)
Set to -1.0 for unassigned lines

Temperature dependent coefficient of air-broadened halfwidth (F4.2)
Not measured >> Set to 0.68

Air-pressure shift of line transition in cm-1/atm @296K (F8.6)
Calculated from air-induced pressure shift recorded at 289.0 K 
In several cases, values are obtained from nitrogen-induced pressure shifts recorded at 291.3 K using an  empirical multiplicative factor of 1.40 (=Median of the air-to-N2 ratio); See reference indices to identify the buffer gas.
Values are converted to 296 K using equation [1] of Toth et al., JQSRT, 1998
For unassigned lines, the temperature correction is not applied.
!!!Use with caution because large uncertainties and scatter are observed

Upper state global quota index (I3) 
from BD_VIBS file 
Lower state global quota index (I3)
from BD_VIBS file 
For transition unavailable in the  BD_VIBS file:
033=82; 034=83; 043=84; 053=85; 061=86; 063=87; 071=88;115=89;132=90; 133=91; 142=92; 160=93; 170=94;223=95; 240=96; 241=97; 322=98; 340=99; 341=100; 430=101;431=102; 510=103; 511=104; 521=105; 600=106; 601=107; 610=108; 611=109; 620=110; 700=111; 701=112; 800=113 

Upper state local quota index (J' Ka' Kc' F' Sym') (3I2,A2,A1)           
Lower state local quota index (J'' Ka'' Kc'' F'' Sym'') (3I2,A2,A1)
F Sym not provided

Accuracy indices (3I1)
1)
Accuracy index for frequencies (see HITRAN tables for codes)
=root sum squared of 3sigma error fit and 0.00002%*wnum (systematic error)
2)
Accuracy index for intensities (see HITRAN tables for codes) 
Set to '0 (=undefined)' for saturated lines
else: root sum squared of 3sigma error fit and and 2.5%*intensity (systematic error)
3)
Accuracy index for half widths (see HITRAN tables for codes)
Set to '0 (=undefined)' for averaged values 
else: root sum squared of 3sigma error fit and 1%*halfwidth (systematic error)

Reference indices (2x,4I1)
1)
Index for frequencies, intensities and self-broadened halfwidths
Flag (1) for Coheur, Fally, Carleer, Clerbaux, Colin, Jenouvrier, Merienne, Hermans, Vandaele, JQSRT, 74, 2002, 493-510
Flag (2) for [Reference 9000-13000] NOT IMPLEMENTED YET
2)
Index for line assignments 
Flag (0) Not assigned
Flag (1) N.F. Zobov et al., to be published
3)
Index for air-broadened halfwidths (I1)
Flag (0) Halfwidth not provided
Flag (1) Coheur, Fally, Carleer, Clerbaux, Colin, Jenouvrier, Merienne, Hermans, Vandaele, JQSRT, 74, 2002, 493-510; Buffer gas is nitrogen.
Flag (2) Fally, Coheur, Carleer, Clerbaux, Colin, Jenouvrier, Merienne, Hermans, Vandaele, JQSRT, 82, 2003, 119-132; Buffer gas is air.
4)
Index for air-induced pressure shifts (I1)
Flag (0) Pressure shift not provided
Flag (1) Coheur, Fally, Carleer, Clerbaux, Colin, Jenouvrier, Merienne, Hermans, Vandaele, JQSRT, 74, 2002, 493-510; Buffer gas is nitrogen.
Flag (2) Fally, Coheur, Carleer, Clerbaux, Colin, Jenouvrier, Merienne, Hermans, Vandaele, JQSRT, 82, 2003, 119-132; Buffer gas is air.

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***23 lines have been fitted to a single line but were assigned to a doublet. The assignment corresponding to the line with the highest calculated intensity is given in the linelist, and the duplicate is listed below. Also given below is the ratio of the calculated intensities between the two duplicates.

 1113708.0719   1.60E+00  0.00E+00 0.0000.000    0.000 0.000.000    35  1 4 1 3    3 2 2   000  0000
 1113732.0309   1.20E+00  0.00E+00 0.0000.000    0.000 0.000.000    36  1 9 5 5    9 5 4   000  0000
 1113873.1390   1.90E+00  0.00E+00 0.0000.000    0.000 0.000.000    96  1 9 5 4    8 4 5   000  0000
 1113998.8921   3.00E+00  0.00E+00 0.0000.000    0.000 0.000.000    42  111 011   12 012   000  0000
 1114001.2038   3.60E+00  0.00E+00 0.0000.000    0.000 0.000.000    39  1 5 1 5    4 0 4   000  0000
 1114053.0395   1.00E+00  0.00E+00 0.0000.000    0.000 0.000.000    36  1 7 4 4    6 2 5   000  0000
 1114131.4278   3.10E+00  0.00E+00 0.0000.000    0.000 0.000.000    42  1 3 0 3    4 2 2   000  0000
 1114442.1898   3.00E+00  0.00E+00 0.0000.000    0.000 0.000.000    42  111 011   10 010   000  0000
 1114446.5852   3.00E+00  0.00E+00 0.0000.000    0.000 0.000.000    42  113 013   12 012   000  0000
 1115201.7083   2.90E+00  0.00E+00 0.0000.000    0.000 0.000.000    48  1 5 5 0    6 5 1   000  0000
 1115641.5204   3.10E+00  0.00E+00 0.0000.000    0.000 0.000.000    82  1 5 5 0    5 5 1   000  0000
 1115655.4008   6.20E+00  0.00E+00 0.0000.000    0.000 0.000.000    50  1 5 4 1    6 4 2   000  0000
 1115690.4203   2.90E+00  0.00E+00 0.0000.000    0.000 0.000.000    50  1 5 0 5    6 0 6   000  0000
 1115696.7480   1.10E+00  0.00E+00 0.0000.000    0.000 0.000.000    48  1 8 2 6    7 0 7   000  0000
 1116572.7521   1.13E+01  0.00E+00 0.0000.000    0.000 0.000.000    92  1 4 1 4    5 2 3   000  0000
 1117186.8547   2.90E+00  0.00E+00 0.0000.000    0.000 0.000.000    58  110 010   11 011   000  0000
 1117470.9184   1.30E+00  0.00E+00 0.0000.000    0.000 0.000.000    52  1 5 4 1    5 1 4   000  0000
 1117485.0566   1.70E+00  0.00E+00 0.0000.000    0.000 0.000.000    56  1 4 2 2    3 0 3   000  0000
 1118956.2243   3.00E+00  0.00E+00 0.0000.000    0.000 0.000.000    62  1 5 5 0    5 5 1   000  0000
 1119064.1843   3.00E+00  0.00E+00 0.0000.000    0.000 0.000.000    62  1 4 3 2    3 3 1   000  0000
 1120605.0978   1.70E+00  0.00E+00 0.0000.000    0.000 0.000.000    65  1 4 2 3    3 2 2   000  0000
 1122434.3660   1.55E+01  0.00E+00 0.0000.000    0.000 0.000.000   111  1 4 3 1    5 2 4   000  0000
 1125022.2393   3.10E+00  0.00E+00 0.0000.000    0.000 0.000.000   112  1 4 4 1    4 4 0   000  0000