Conversion of standardized ReadMe file for
file /./ftp/cats/J/A_A/535/A117 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 2024-Apr-19
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/535/A117 Low-charge ions charge transfer rate coeff. (Sterling+, 2011)
*================================================================================
*Atomic data for neutron-capture elements.
*III. Charge transfer rate coefficients for low-charge ions of Ge, Se, Br, Kr,
*Rb, and Xe.
* Sterling N.C., Stancil P.C.
* <Astron. Astrophys. 535, A117 (2011)>
* =2011A&A...535A.117S
C=============================================================================
C Internal variables
integer*4 i__
c - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - -
C Declarations for 'table4.dat' ! Final-state resolved charge transfer recombination
rate coefficients (cm^3^/s) for the reactions
X^q+^+H --> X^(q-1)+^+H^+^+{delta}E
integer*4 nr__
parameter (nr__=159) ! Number of records
character*212 ar__ ! Full-size record
character*2 El (nr__) ! Projectile element (Ge Se Br Kr Rb Xe)
integer*4 ion (nr__) ! [0/5] Ionisation state
character*24 ExitC (nr__) ! Exit channel
real*4 a_0_1 (nr__) ! (cm3/s) Rate coefficient {alpha} over T=100K (1)
real*4 a_0_2 (nr__) ! (cm3/s) Rate coefficient {alpha} over T=200K (1)
real*4 a_0_4 (nr__) ! (cm3/s) Rate coefficient {alpha} over T=400K (1)
real*4 a_0_6 (nr__) ! (cm3/s) Rate coefficient {alpha} over T=600K (1)
real*4 a_0_8 (nr__) ! (cm3/s) Rate coefficient {alpha} over T=800K (1)
real*4 a_1_0 (nr__) ! (cm3/s) Rate coefficient {alpha} over T=1000K (1)
real*4 a_1_2 (nr__) ! (cm3/s) Rate coefficient {alpha} over T=2000K (1)
real*4 a_1_4 (nr__) ! (cm3/s) Rate coefficient {alpha} over T=4000K (1)
real*4 a_1_6 (nr__) ! (cm3/s) Rate coefficient {alpha} over T=6000K (1)
real*4 a_1_8 (nr__) ! (cm3/s) Rate coefficient {alpha} over T=8000K (1)
real*4 a_10_ (nr__) ! (cm3/s) Rate coefficient {alpha} over T=10kK (1)
real*4 a_20_ (nr__) ! (cm3/s) Rate coefficient {alpha} over T=20kK (1)
real*4 a_40_ (nr__) ! (cm3/s) Rate coefficient {alpha} over T=40kK (1)
real*4 a_60_ (nr__) ! (cm3/s) Rate coefficient {alpha} over T=60kK (1)
real*4 a_80_ (nr__) ! (cm3/s) Rate coefficient {alpha} over T=80kK (1)
real*4 a_100 (nr__) ! (cm3/s) Rate coefficient {alpha} over T=100kK (1)
real*4 a_200 (nr__) ! (cm3/s) Rate coefficient {alpha} over T=200kK (1)
real*4 a_400 (nr__) ! (cm3/s) Rate coefficient {alpha} over T=400kK (1)
real*4 a_600 (nr__) ! (cm3/s) Rate coefficient {alpha} over T=600kK (1)
real*4 a_800 (nr__) ! (cm3/s) Rate coefficient {alpha} over T=800kK (1)
*Note (1):
* * For table4.dat: Each listed rate coefficient is the largest of the
* radially-coupled CT rate coefficient from our MCLZ and Demkov calculations
* and the canonical radiative CT rate coefficient 10^-14^cm^3^/s (Butler et al.
* 1977, Phys. Rev. A, 16, 500; Stancil & Zygelman 1996ApJ...472..102S).
* Note that radiative CT does not occur for endoergic reactions.
* * For table5.dat: For Ge, Se, and Br, the spin-orbit coupling rate
* coefficient found for Cl^+^, 10^-12^cm^3^/s (Pradhan & Dalgarno, 1994,
* Phys. Rev. A, 49, 960), is adopted as an upper limit when the rate from
* radial coupling falls below that value. In the case of Se and Br, the SO rate
* coefficient is adopted only for the dominant exit channels for SO coupling.
* For CT reactions involving neutral Kr, Rb, and Xe, SO coupling is not
* relevant and hence we set the rate coefficient to the canonical radiative CT
* rate 10^-14^cm^3^/s (Butler et al. 1977, Phys. Rev. A, 16, 500) when the
* radial coupling rate coefficient is smaller than that value.
* Note that radiative CT does not occur for the endoergic reaction
* Kr^0^+H^+^ --> Kr^+^+H+{delta}E.
c - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - -
C Declarations for 'table5.dat' ! Final-state resolved charge transfer ionization
rate coefficients (cm^3^/s) for the reactions
X^0^+H^+^ --> X^+^+H+{delta}E
integer*4 nr__1
parameter (nr__1=9) ! Number of records
character*212 ar__1 ! Full-size record
character*2 El_1 (nr__1) ! Projectile element (Ge Se Br Kr Rb Xe)
integer*4 ion_1 (nr__1) ! [0/5] Ionisation state
character*24 ExitC_1 (nr__1) ! Exit channel
real*4 a_0_1_1 (nr__1) ! (cm3/s) Rate coefficient {alpha} over T=100K (1)
real*4 a_0_2_1 (nr__1) ! (cm3/s) Rate coefficient {alpha} over T=200K (1)
real*4 a_0_4_1 (nr__1) ! (cm3/s) Rate coefficient {alpha} over T=400K (1)
real*4 a_0_6_1 (nr__1) ! (cm3/s) Rate coefficient {alpha} over T=600K (1)
real*4 a_0_8_1 (nr__1) ! (cm3/s) Rate coefficient {alpha} over T=800K (1)
real*4 a_1_0_1 (nr__1) ! (cm3/s) Rate coefficient {alpha} over T=1000K (1)
real*4 a_1_2_1 (nr__1) ! (cm3/s) Rate coefficient {alpha} over T=2000K (1)
real*4 a_1_4_1 (nr__1) ! (cm3/s) Rate coefficient {alpha} over T=4000K (1)
real*4 a_1_6_1 (nr__1) ! (cm3/s) Rate coefficient {alpha} over T=6000K (1)
real*4 a_1_8_1 (nr__1) ! (cm3/s) Rate coefficient {alpha} over T=8000K (1)
real*4 a_10__1 (nr__1) ! (cm3/s) Rate coefficient {alpha} over T=10kK (1)
real*4 a_20__1 (nr__1) ! (cm3/s) Rate coefficient {alpha} over T=20kK (1)
real*4 a_40__1 (nr__1) ! (cm3/s) Rate coefficient {alpha} over T=40kK (1)
real*4 a_60__1 (nr__1) ! (cm3/s) Rate coefficient {alpha} over T=60kK (1)
real*4 a_80__1 (nr__1) ! (cm3/s) Rate coefficient {alpha} over T=80kK (1)
real*4 a_100_1 (nr__1) ! (cm3/s) Rate coefficient {alpha} over T=100kK (1)
real*4 a_200_1 (nr__1) ! (cm3/s) Rate coefficient {alpha} over T=200kK (1)
real*4 a_400_1 (nr__1) ! (cm3/s) Rate coefficient {alpha} over T=400kK (1)
real*4 a_600_1 (nr__1) ! (cm3/s) Rate coefficient {alpha} over T=600kK (1)
real*4 a_800_1 (nr__1) ! (cm3/s) Rate coefficient {alpha} over T=800kK (1)
*Note (1):
* * For table4.dat: Each listed rate coefficient is the largest of the
* radially-coupled CT rate coefficient from our MCLZ and Demkov calculations
* and the canonical radiative CT rate coefficient 10^-14^cm^3^/s (Butler et al.
* 1977, Phys. Rev. A, 16, 500; Stancil & Zygelman 1996ApJ...472..102S).
* Note that radiative CT does not occur for endoergic reactions.
* * For table5.dat: For Ge, Se, and Br, the spin-orbit coupling rate
* coefficient found for Cl^+^, 10^-12^cm^3^/s (Pradhan & Dalgarno, 1994,
* Phys. Rev. A, 49, 960), is adopted as an upper limit when the rate from
* radial coupling falls below that value. In the case of Se and Br, the SO rate
* coefficient is adopted only for the dominant exit channels for SO coupling.
* For CT reactions involving neutral Kr, Rb, and Xe, SO coupling is not
* relevant and hence we set the rate coefficient to the canonical radiative CT
* rate 10^-14^cm^3^/s (Butler et al. 1977, Phys. Rev. A, 16, 500) when the
* radial coupling rate coefficient is smaller than that value.
* Note that radiative CT does not occur for the endoergic reaction
* Kr^0^+H^+^ --> Kr^+^+H+{delta}E.
C=============================================================================
C Loading file 'table4.dat' ! Final-state resolved charge transfer recombination
* rate coefficients (cm^3^/s) for the reactions
* X^q+^+H --> X^(q-1)+^+H^+^+{delta}E
C Format for file interpretation
1 format(
+ A2,1X,I1,4X,A24,1X,E8.2,1X,E8.2,1X,E8.2,1X,E8.2,1X,E8.2,1X,
+ E8.2,1X,E8.2,1X,E8.2,1X,E8.2,1X,E8.2,1X,E8.2,1X,E8.2,1X,E8.2,
+ 1X,E8.2,1X,E8.2,1X,E8.2,1X,E8.2,1X,E8.2,1X,E8.2,1X,E8.2)
C Effective file loading
open(unit=1,status='old',file=
+'table4.dat')
write(6,*) '....Loading file: table4.dat'
do i__=1,159
read(1,'(A212)')ar__
read(ar__,1)
+ El(i__),ion(i__),ExitC(i__),a_0_1(i__),a_0_2(i__),a_0_4(i__),
+ a_0_6(i__),a_0_8(i__),a_1_0(i__),a_1_2(i__),a_1_4(i__),
+ a_1_6(i__),a_1_8(i__),a_10_(i__),a_20_(i__),a_40_(i__),
+ a_60_(i__),a_80_(i__),a_100(i__),a_200(i__),a_400(i__),
+ a_600(i__),a_800(i__)
c ..............Just test output...........
write(6,1)
+ El(i__),ion(i__),ExitC(i__),a_0_1(i__),a_0_2(i__),a_0_4(i__),
+ a_0_6(i__),a_0_8(i__),a_1_0(i__),a_1_2(i__),a_1_4(i__),
+ a_1_6(i__),a_1_8(i__),a_10_(i__),a_20_(i__),a_40_(i__),
+ a_60_(i__),a_80_(i__),a_100(i__),a_200(i__),a_400(i__),
+ a_600(i__),a_800(i__)
c .......End.of.Just test output...........
end do
close(1)
C=============================================================================
C Loading file 'table5.dat' ! Final-state resolved charge transfer ionization
* rate coefficients (cm^3^/s) for the reactions
* X^0^+H^+^ --> X^+^+H+{delta}E
C Format for file interpretation
2 format(
+ A2,1X,I1,4X,A24,1X,E8.2,1X,E8.2,1X,E8.2,1X,E8.2,1X,E8.2,1X,
+ E8.2,1X,E8.2,1X,E8.2,1X,E8.2,1X,E8.2,1X,E8.2,1X,E8.2,1X,E8.2,
+ 1X,E8.2,1X,E8.2,1X,E8.2,1X,E8.2,1X,E8.2,1X,E8.2,1X,E8.2)
C Effective file loading
open(unit=1,status='old',file=
+'table5.dat')
write(6,*) '....Loading file: table5.dat'
do i__=1,9
read(1,'(A212)')ar__1
read(ar__1,2)
+ El_1(i__),ion_1(i__),ExitC_1(i__),a_0_1_1(i__),a_0_2_1(i__),
+ a_0_4_1(i__),a_0_6_1(i__),a_0_8_1(i__),a_1_0_1(i__),
+ a_1_2_1(i__),a_1_4_1(i__),a_1_6_1(i__),a_1_8_1(i__),
+ a_10__1(i__),a_20__1(i__),a_40__1(i__),a_60__1(i__),
+ a_80__1(i__),a_100_1(i__),a_200_1(i__),a_400_1(i__),
+ a_600_1(i__),a_800_1(i__)
c ..............Just test output...........
write(6,2)
+ El_1(i__),ion_1(i__),ExitC_1(i__),a_0_1_1(i__),a_0_2_1(i__),
+ a_0_4_1(i__),a_0_6_1(i__),a_0_8_1(i__),a_1_0_1(i__),
+ a_1_2_1(i__),a_1_4_1(i__),a_1_6_1(i__),a_1_8_1(i__),
+ a_10__1(i__),a_20__1(i__),a_40__1(i__),a_60__1(i__),
+ a_80__1(i__),a_100_1(i__),a_200_1(i__),a_400_1(i__),
+ a_600_1(i__),a_800_1(i__)
c .......End.of.Just test output...........
end do
close(1)
C=============================================================================
stop
end