Conversion of standardized ReadMe file for
file /./ftp/cats/J/A_A/657/A99 into FORTRAN code for reading data files line by line.
Note that special values are assigned to unknown or unspecified
numbers (also called NULL numbers);
when necessary, the coordinate components making up the right ascension
and declination are converted into floating-point numbers
representing these angles in degrees.
program load_ReadMe
C=============================================================================
C F77-compliant program generated by readme2f_1.81 (2015-09-23), on 2026-Sep-08
C=============================================================================
* This code was generated from the ReadMe file documenting a catalogue
* according to the "Standard for Documentation of Astronomical Catalogues"
* currently in use by the Astronomical Data Centers (CDS, ADC, A&A)
* (see full documentation at URL http://vizier.u-strasbg.fr/doc/catstd.htx)
* Please report problems or questions to
C=============================================================================
implicit none
* Unspecified or NULL values, generally corresponding to blank columns,
* are assigned one of the following special values:
* rNULL__ for unknown or NULL floating-point values
* iNULL__ for unknown or NULL integer values
real*4 rNULL__
integer*4 iNULL__
parameter (rNULL__=--2147483648.) ! NULL real number
parameter (iNULL__=(-2147483647-1)) ! NULL int number
integer idig ! testing NULL number
C=============================================================================
Cat. J/A+A/657/A99 The rotational spectrum of glycinamide (Kisiel+, 2022)
*================================================================================
*Millimetre-wave laboratory study of glycinamide and search for it
*with ALMA toward Sagittarius B2(N).
* Kisiel Z., Kolesnikova L., Belloche A., Guillemin J.-C., Pszczolkowski L.,
* Alonso E.R., Garrod R.T., Bialkowska-Jaworska E., Leon I., Mueller H.S.P.,
* Menten K.M., Alonso J.L.
* <Astron. Astrophys. 657, A99 (2022)>
* =2022A&A...657A..99K (SIMBAD/NED BibCode)
C=============================================================================
C Internal variables
integer*4 i__
c - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - -
C Declarations for 'table5.dat' ! Fitted rotational transitions of glycinamide
in the ground state (0+ 0- doublet)
integer*4 nr__
parameter (nr__=1400) ! Number of records
character*119 ar__ ! Full-size record
integer*4 J_ ! Upper state J quantum number
integer*4 Ka_ ! Upper state Ka quantum number
integer*4 Kc_ ! Upper state Kc quantum number
integer*4 v_ ! Upper state v quantum number (1)
integer*4 J__1 ! Lower state J quantum number
integer*4 Ka__1 ! Lower state Ka quantum number
integer*4 Kc__1 ! Lower state Kc quantum number
integer*4 v__1 ! Lower state v quantum number (1)
real*8 FreqObs ! (MHz) Observed transition frequency
real*8 O_C ! (MHz) Observed minus calculated frequency
real*4 FreqExp ! (MHz) Experimental uncertainty
real*8 v_O_C_b ! (MHz) ? Observed minus calculated frequency for blends
real*4 wb ! ? Weight of the components of the blends
character*35 Source ! Source of the data
*Note (1): The vibrational quantum number v=0 corresponds to 0+ state and
* v=1 to 0- state of the ground state tunneling doublet.
c - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - -
C Declarations for 'table6.dat' ! Fitted rotational transitions of glycinamide
in v27=1 state (1+ 1- doublet)
integer*4 nr__1
parameter (nr__1=990) ! Number of records
character*80 ar__1 ! Full-size record
integer*4 J__2 ! Upper state J quantum number
integer*4 Ka__2 ! Upper state Ka quantum number
integer*4 Kc__2 ! Upper state Kc quantum number
integer*4 v__2 ! Upper state v quantum number (1)
integer*4 J__3 ! Lower state J quantum number
integer*4 Ka__3 ! Lower state Ka quantum number
integer*4 Kc__3 ! Lower state Kc quantum number
integer*4 v__3 ! Lower state v quantum number (1)
real*8 FreqObs_1 ! (MHz) Observed transition frequency
real*8 O_C_1 ! (MHz) Observed minus calculated frequency
real*4 FreqExp_1 ! (MHz) Experimental uncertainty
real*8 v_O_C_b_1 ! (MHz) ? Observed minus calculated frequency for blends
real*4 wb_1 ! ? Weight of the components of the blends
*Note (1): The vibrational quantum number v=0 corresponds to 1+ state and
* v=1 to 1- state of the v27=1 tunneling doublet.
c - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - -
C Declarations for 'table7.dat' ! Fitted rotational transitions of glycinamide
in v26=1 state (0+ 0- doublet)
integer*4 nr__2
parameter (nr__2=781) ! Number of records
character*80 ar__2 ! Full-size record
integer*4 J__4 ! Upper state J quantum number
integer*4 Ka__4 ! Upper state Ka quantum number
integer*4 Kc__4 ! Upper state Kc quantum number
integer*4 v__4 ! Upper state v quantum number (1)
integer*4 J__5 ! Lower state J quantum number
integer*4 Ka__5 ! Lower state Ka quantum number
integer*4 Kc__5 ! Lower state Kc quantum number
integer*4 v__5 ! Lower state v quantum number (1)
real*8 FreqObs_2 ! (MHz) Observed transition frequency
real*8 O_C_2 ! (MHz) Observed minus calculated frequency
real*4 FreqExp_2 ! (MHz) Experimental uncertainty
real*8 v_O_C_b_2 ! (MHz) ? Observed minus calculated frequency for blends
real*4 wb_2 ! ? Weight of the components of the blends
*Note (1): The vibrational quantum number v=0 corresponds to 0+ state and
* v=1 to 0- state of the v26=1 tunneling doublet.
C=============================================================================
C Loading file 'table5.dat' ! Fitted rotational transitions of glycinamide
* in the ground state (0+ 0- doublet)
C Format for file interpretation
1 format(
+ I3,I3,I3,I3,2X,I3,I3,I3,I3,13X,F11.4,2X,F7.4,2X,F5.3,2X,F7.4,
+ 1X,F4.2,4X,A35)
C Effective file loading
open(unit=1,status='old',file=
+'table5.dat')
write(6,*) '....Loading file: table5.dat'
do i__=1,1400
read(1,'(A119)')ar__
read(ar__,1)
+ J_,Ka_,Kc_,v_,J__1,Ka__1,Kc__1,v__1,FreqObs,O_C,FreqExp,
+ v_O_C_b,wb,Source
if(ar__(69:75) .EQ. '') v_O_C_b = rNULL__
if(ar__(77:80) .EQ. '') wb = rNULL__
c ..............Just test output...........
write(6,1)
+ J_,Ka_,Kc_,v_,J__1,Ka__1,Kc__1,v__1,FreqObs,O_C,FreqExp,
+ v_O_C_b,wb,Source
c .......End.of.Just test output...........
end do
close(1)
C=============================================================================
C Loading file 'table6.dat' ! Fitted rotational transitions of glycinamide
* in v27=1 state (1+ 1- doublet)
C Format for file interpretation
2 format(
+ I3,I3,I3,I3,2X,I3,I3,I3,I3,13X,F11.4,2X,F7.4,2X,F5.3,2X,F7.4,
+ 1X,F4.2)
C Effective file loading
open(unit=1,status='old',file=
+'table6.dat')
write(6,*) '....Loading file: table6.dat'
do i__=1,990
read(1,'(A80)')ar__1
read(ar__1,2)
+ J__2,Ka__2,Kc__2,v__2,J__3,Ka__3,Kc__3,v__3,FreqObs_1,O_C_1,
+ FreqExp_1,v_O_C_b_1,wb_1
if(ar__1(69:75) .EQ. '') v_O_C_b_1 = rNULL__
if(ar__1(77:80) .EQ. '') wb_1 = rNULL__
c ..............Just test output...........
write(6,2)
+ J__2,Ka__2,Kc__2,v__2,J__3,Ka__3,Kc__3,v__3,FreqObs_1,O_C_1,
+ FreqExp_1,v_O_C_b_1,wb_1
c .......End.of.Just test output...........
end do
close(1)
C=============================================================================
C Loading file 'table7.dat' ! Fitted rotational transitions of glycinamide
* in v26=1 state (0+ 0- doublet)
C Format for file interpretation
3 format(
+ I3,I3,I3,I3,2X,I3,I3,I3,I3,13X,F11.4,2X,F7.4,2X,F5.3,2X,F7.4,
+ 1X,F4.2)
C Effective file loading
open(unit=1,status='old',file=
+'table7.dat')
write(6,*) '....Loading file: table7.dat'
do i__=1,781
read(1,'(A80)')ar__2
read(ar__2,3)
+ J__4,Ka__4,Kc__4,v__4,J__5,Ka__5,Kc__5,v__5,FreqObs_2,O_C_2,
+ FreqExp_2,v_O_C_b_2,wb_2
if(ar__2(69:75) .EQ. '') v_O_C_b_2 = rNULL__
if(ar__2(77:80) .EQ. '') wb_2 = rNULL__
c ..............Just test output...........
write(6,3)
+ J__4,Ka__4,Kc__4,v__4,J__5,Ka__5,Kc__5,v__5,FreqObs_2,O_C_2,
+ FreqExp_2,v_O_C_b_2,wb_2
c .......End.of.Just test output...........
end do
close(1)
C=============================================================================
stop
end