Conversion of standardized ReadMe file for
file /./ftp/cats/J/A_A/589/A127 into FORTRAN code for loading all data files into arrays.
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-May-17
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/589/A127 Dimethyl sulfide laboratory um, mm & FIR spectra (Jabri+, 2016)
*================================================================================
*Laboratory microwave, millimeter wave and far-infrared spectra of dimethyl
*sulfide
* Jabri A., Nguyen H.V.L., Mouhib H., Tchana F.K., Manceron L., Stahl W.,
* Kleiner I.
* <Astron. Astrophys. 589, A127 (2016)>
* =2016A&A...589A.127J (SIMBAD/NED BibCode)
C=============================================================================
C Internal variables
integer*4 i__
c - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - -
C Declarations for 'appenb.dat' ! *Microwave and millimeter-wave range
integer*4 nr__
parameter (nr__=602) ! Number of records
character*92 ar__ ! Full-size record
integer*4 v111 (nr__) ! [0/1] Observed v11 upper state (G1)
integer*4 v151 (nr__) ! [0/1] Observed v15 upper state (G1)
integer*4 J1 (nr__) ! Observed J upper state
integer*4 Ka1 (nr__) ! Observed Ka upper state
integer*4 Kc1 (nr__) ! Observed Kc upper state
integer*4 v110 (nr__) ! [0/1] Observed v11 lower state (G1)
integer*4 v150 (nr__) ! [0/1] Observed v15 lower state (G1)
integer*4 J0 (nr__) ! Observed J lower state
integer*4 Ka0 (nr__) ! Observed Ka lower state
integer*4 Kc0 (nr__) ! Observed Kc lower state
real*8 Freq_Obs (nr__) ! (MHz) Observed line frequency
integer*4 e_Freq_Obs (nr__) ! (kHz) rms uncertainty on Freq.Obs (G2)
real*8 Freq_Cal (nr__) ! (MHz) Calculated line frequency
real*4 e_Freq_Cal (nr__) ! (MHz) ? rms uncertainty on Freq.Cal
real*4 O_C (nr__) ! (MHz) Difference between the experimental and
* calculated frequencies
real*8 S_mu__2 (nr__) ! (D+2) Calculated line strength (3)
real*8 E0 (nr__) ! (cm-1) Upper state energy including the
* zero-point torsional energy
real*8 E1 (nr__) ! (cm-1) Lower state energy including the
* zero-point torsional energy
character*2 Sym (nr__) ! Symmetry species in the
* C^-^_3v_ X c^+^_3v_ direct product (4)
*Note (3): Note that the line strengths are given as S*mu**2. To obtain
* intensities the line strengths need to be multiplied by appropriate
* statistical weights, Boltzmann factor and divided by the total partition
* function (see appendix C).
*Note (4): The spin-weight statistics for the transitions AA: EE: AE: EA depend
* on the parity of KaKc, i.e. 6:16:4:2 for KaKc: ee-oo and
* 10:16:4:6 for KaKc: eo-oe (Vacherand et al. 1987).
c - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - -
C Declarations for 'appenc.dat' ! *Far-infrared range
integer*4 nr__1
parameter (nr__1=578) ! Number of records
character*72 ar__1 ! Full-size record
integer*4 v111_1 (nr__1) ! [0] Observed v11 upper state
integer*4 v151_1 (nr__1) ! [1] Observed v15 upper state
integer*4 J1_1 (nr__1) ! J upper state
integer*4 Ka1_1 (nr__1) ! Ka upper state
integer*4 Kc1_1 (nr__1) ! Kc upper state
integer*4 v110_1 (nr__1) ! [0] v11 lower state
integer*4 v150_1 (nr__1) ! [0] v15 lower state
integer*4 J0_1 (nr__1) ! J lower state
integer*4 Ka0_1 (nr__1) ! Ka lower state
integer*4 Kc0_1 (nr__1) ! Kc lower state
real*8 Freq_Obs_1 (nr__1) ! (MHz) Observed line frequency
integer*4 e_Freq_Obs_1(nr__1) ! (kHz) rms uncertainty on Freq.Obs
real*8 Freq_Cal_1 (nr__1) ! (MHz) Calculated line frequency
real*8 O_C_1 (nr__1) ! (MHz) Difference between the experimental and
* calculated frequencies
real*8 E0_1 (nr__1) ! (cm-1) Upper state energy including the zero-point
* torsional energy calculated at 187.6294cm^-1^
real*8 E1_1 (nr__1) ! (cm-1) Lower state energy including the zero-point
* torsional energy calculated at 187.6294cm^-1^
character*2 Sym_1 (nr__1) ! Symmetry species in the
* C^-^_3v_ X c^+^_3v_ direct product
c - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - -
C Declarations for 'appene.dat' ! A line-list of all rotational transitions
reliably predicted between 0 and 300GHz with
the set of spectroscopic parameters
determined in Appendix A
integer*4 nr__2
parameter (nr__2=7158) ! Number of records
character*94 ar__2 ! Full-size record
integer*4 v111_2 (nr__2) ! [0] Observed v11 upper state (G1)
integer*4 v151_2 (nr__2) ! [0] Observed v15 upper state (G1)
integer*4 J1_2 (nr__2) ! Observed J upper state
integer*4 Ka1_2 (nr__2) ! Observed Ka upper state
integer*4 Kc1_2 (nr__2) ! Observed Kc upper state
integer*4 v110_2 (nr__2) ! [0] Observed v11 lower state (G1)
integer*4 v150_2 (nr__2) ! [0] Observed v15 lower state (G1)
integer*4 J0_2 (nr__2) ! Observed J lower state
integer*4 Ka0_2 (nr__2) ! Observed Ka lower state
integer*4 Kc0_2 (nr__2) ! Observed Kc lower state
real*8 Freq_Obs_2 (nr__2) ! (MHz) ? Observed line frequency
integer*4 e_Freq_Obs_2(nr__2) ! (kHz) ? rms uncertainty on Freq.Obs (G2)
real*8 Freq_Cal_2 (nr__2) ! (MHz) Calculated line frequency
real*4 e_Freq_Cal_1(nr__2) ! (MHz) rms uncertainty on Freq.Cal
real*4 O_C_2 (nr__2) ! (MHz) ? Difference between the experimental and
* calculated frequencies
real*8 Smu_2 (nr__2) ! (D+2) Calculated line strength
real*8 E0_2 (nr__2) ! (cm-1) Upper state energy including the
* zero-point torsional energy
real*8 E1_2 (nr__2) ! (cm-1) Lower state energy including the
* zero-point torsional energy
character*2 Sym_2 (nr__2) ! Symmetry species in the
* C^-^_3v_ X c^+^_3v_ direct product
C=============================================================================
C Loading file 'appenb.dat' ! *Microwave and millimeter-wave range
C Format for file interpretation
1 format(
+ I1,I1,1X,I2,1X,I2,1X,I2,1X,I1,I1,1X,I2,1X,I2,1X,I2,1X,F10.3,
+ 1X,I3,1X,F10.3,1X,F5.3,1X,F6.3,1X,F8.5,1X,F8.4,1X,F8.4,1X,A2)
C Effective file loading
open(unit=1,status='old',file=
+'appenb.dat')
write(6,*) '....Loading file: appenb.dat'
do i__=1,602
read(1,'(A92)')ar__
read(ar__,1)
+ v111(i__),v151(i__),J1(i__),Ka1(i__),Kc1(i__),v110(i__),
+ v150(i__),J0(i__),Ka0(i__),Kc0(i__),Freq_Obs(i__),
+ e_Freq_Obs(i__),Freq_Cal(i__),e_Freq_Cal(i__),O_C(i__),
+ S_mu__2(i__),E0(i__),E1(i__),Sym(i__)
if(ar__(51:55) .EQ. '') e_Freq_Cal(i__) = rNULL__
c ..............Just test output...........
write(6,1)
+ v111(i__),v151(i__),J1(i__),Ka1(i__),Kc1(i__),v110(i__),
+ v150(i__),J0(i__),Ka0(i__),Kc0(i__),Freq_Obs(i__),
+ e_Freq_Obs(i__),Freq_Cal(i__),e_Freq_Cal(i__),O_C(i__),
+ S_mu__2(i__),E0(i__),E1(i__),Sym(i__)
c .......End.of.Just test output...........
end do
close(1)
C=============================================================================
C Loading file 'appenc.dat' ! *Far-infrared range
C Format for file interpretation
2 format(
+ I1,I1,1X,I2,1X,I2,1X,I2,1X,I1,I1,1X,I2,1X,I2,1X,I2,1X,F8.4,1X,
+ I1,1X,F8.4,1X,F7.4,1X,F8.4,1X,F8.4,1X,A2)
C Effective file loading
open(unit=1,status='old',file=
+'appenc.dat')
write(6,*) '....Loading file: appenc.dat'
do i__=1,578
read(1,'(A72)')ar__1
read(ar__1,2)
+ v111_1(i__),v151_1(i__),J1_1(i__),Ka1_1(i__),Kc1_1(i__),
+ v110_1(i__),v150_1(i__),J0_1(i__),Ka0_1(i__),Kc0_1(i__),
+ Freq_Obs_1(i__),e_Freq_Obs_1(i__),Freq_Cal_1(i__),O_C_1(i__),
+ E0_1(i__),E1_1(i__),Sym_1(i__)
c ..............Just test output...........
write(6,2)
+ v111_1(i__),v151_1(i__),J1_1(i__),Ka1_1(i__),Kc1_1(i__),
+ v110_1(i__),v150_1(i__),J0_1(i__),Ka0_1(i__),Kc0_1(i__),
+ Freq_Obs_1(i__),e_Freq_Obs_1(i__),Freq_Cal_1(i__),O_C_1(i__),
+ E0_1(i__),E1_1(i__),Sym_1(i__)
c .......End.of.Just test output...........
end do
close(1)
C=============================================================================
C Loading file 'appene.dat' ! A line-list of all rotational transitions
* reliably predicted between 0 and 300GHz with
* the set of spectroscopic parameters
* determined in Appendix A
C Format for file interpretation
3 format(
+ I1,I1,1X,I2,1X,I3,1X,I2,1X,I1,I1,1X,I2,1X,I3,1X,I2,1X,F10.3,
+ 1X,I3,1X,F10.3,1X,F5.3,1X,F6.3,1X,F8.5,1X,F8.4,1X,F8.4,1X,A2)
C Effective file loading
open(unit=1,status='old',file=
+'appene.dat')
write(6,*) '....Loading file: appene.dat'
do i__=1,7158
read(1,'(A94)')ar__2
read(ar__2,3)
+ v111_2(i__),v151_2(i__),J1_2(i__),Ka1_2(i__),Kc1_2(i__),
+ v110_2(i__),v150_2(i__),J0_2(i__),Ka0_2(i__),Kc0_2(i__),
+ Freq_Obs_2(i__),e_Freq_Obs_2(i__),Freq_Cal_2(i__),
+ e_Freq_Cal_1(i__),O_C_2(i__),Smu_2(i__),E0_2(i__),E1_2(i__),
+ Sym_2(i__)
if(ar__2(27:36) .EQ. '') Freq_Obs_2(i__) = rNULL__
if(ar__2(38:40) .EQ. '') e_Freq_Obs_2(i__) = iNULL__
if(ar__2(59:64) .EQ. '') O_C_2(i__) = rNULL__
c ..............Just test output...........
write(6,3)
+ v111_2(i__),v151_2(i__),J1_2(i__),Ka1_2(i__),Kc1_2(i__),
+ v110_2(i__),v150_2(i__),J0_2(i__),Ka0_2(i__),Kc0_2(i__),
+ Freq_Obs_2(i__),e_Freq_Obs_2(i__),Freq_Cal_2(i__),
+ e_Freq_Cal_1(i__),O_C_2(i__),Smu_2(i__),E0_2(i__),E1_2(i__),
+ Sym_2(i__)
c .......End.of.Just test output...........
end do
close(1)
C=============================================================================
stop
end