qcx#h0_ex3#h1.dat

Charge Exchange Cross Sections

Ion
H1+
Energy Range
1.000 keV/amu → 700 keV/amu

ADF01

Filename
qcx#h0_ex3#h1.dat
Full Path
adf01/qcx#h0/qcx#h0_ex3#h1.dat
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H+ + H0(n=3) → H0 + H+total
H+ + H0(n=3) → H0(n=1) + H+n-resolved
H+ + H0(n=3) → H0(1s) + H+nl-resolved
H+ + H0(n=3) → H0(n=2) + H+n-resolved
H+ + H0(n=3) → H0(2s) + H+nl-resolved
H+ + H0(n=3) → H0(2p) + H+nl-resolved
H+ + H0(n=3) → H0(n=3) + H+n-resolved
H+ + H0(n=3) → H0(3s) + H+nl-resolved
H+ + H0(n=3) → H0(3p) + H+nl-resolved
H+ + H0(n=3) → H0(3d) + H+nl-resolved
H+ + H0(n=3) → H0(n=4) + H+n-resolved
H+ + H0(n=3) → H0(4s) + H+nl-resolved
H+ + H0(n=3) → H0(4p) + H+nl-resolved
H+ + H0(n=3) → H0(4d) + H+nl-resolved
H+ + H0(n=3) → H0(4f) + H+nl-resolved
H+ + H0(n=3) → H0(n=5) + H+n-resolved
H+ + H0(n=3) → H0(5s) + H+nl-resolved
H+ + H0(n=3) → H0(5p) + H+nl-resolved
H+ + H0(n=3) → H0(5d) + H+nl-resolved
H+ + H0(n=3) → H0(5f) + H+nl-resolved
H+ + H0(n=3) → H0(5g) + H+nl-resolved
H+ + H0(n=3) → H0(n=6) + H+n-resolved
H+ + H0(n=3) → H0(6s) + H+nl-resolved
H+ + H0(n=3) → H0(6p) + H+nl-resolved
H+ + H0(n=3) → H0(6d) + H+nl-resolved
H+ + H0(n=3) → H0(6f) + H+nl-resolved
H+ + H0(n=3) → H0(6g) + H+nl-resolved
H+ + H0(n=3) → H0(6h) + H+nl-resolved
-------------------------------------------------------------------------------------------

 DATA REFORMATTED TO NEW ADF01 FORMAT.

 INPUT DATA FILE : JETSHP.CHEXDATA.DATA(H1#HEXC1)
 SUB-BLOCK USED  : 3
 SUB-BLOCK TITLE :  COMPOSITE FOR CAPTURE FROM N=3  N'**2*E =1.0KEV/AMU - 700 KEV/AMU  H+1

 COMMENT RECORDS FROM INPUT DATA FILE ARE APPENDED BELOW.

-------------------------------------------------------------------------------------------
 ======================================================================
                  H(N>1) + H(1) --> H(+) + H
                  --------------------------

      INFORMATION                               #1989 RESTRUCTURED DATA
      -----------
      THE FOLLOWING OPTIONS ARE AVAILABLE SELECTED BY IBLOCK

      IBLOCK=3
      --------

      ENERGY    = 1.0D3 EV/AMU - 7.0D5 EV/AMU   (N'**2*E UNITS)
      N         = 1 - 6
      APPROX    = COMPOSITE
      REFERENCE = SIMPLY ARRANGED TO GIVE MODEST PEAKING
                         (USED BELOW N'**2 *E=1.0D5)
                  EICHLER             (1981) PHYS. REV. A. 23, 498.
                         (USED ABOVE N'**2 *E=1.0D5)
                  IT IS ASSUMED THAT FRACTIONS ARE THE SAME FROM 3S,3P,
                  AND 3D.

      REMARKS
             CAPTURE FORM H(N=3) ONLY.  COMPOSITE DATA BASED ON ABOVE
             REFERENCES.  NO DATA AVAILABLE ON HIGH N EXTRAPOLATION OR
             L-SUBSHELL SPLITTING.  A CHOICE OF ALPHA IS THE SAME AS
             THAT OF BE{+4} CAPTURE FROM H(1S).
             THE SUMMED XSECT. FROM 6 TO INFINITY HAS BEEN USED TO
             COMPUTE THE N=6 XSECT BASED ON EXTRAPOLATION FROM N=6
             WITH THE PREFERRED ALPHA.

             LFORMA, XLCUTA, PL2A AND PL3A
                   THESE ARE THE SAME AS THE VALUES FOR HE{+2}+H(1S)
                   BUT WITH XLCUTA INCREASED TO 2.0

                                             H.P. SUMMERS  20 FEB 1990
=======================================================================
   L-SPLITTING IS RECONSTITUTED FROM THE JET N-SHELL RESOLUTION DATA 
   BLOCK USING  ITS L-SHELL FORM PARAMETERS.  THE DATA SET THUS EXACTLY
   MATCHES THE JET DATA SET IN APPLICATION.  NOTE THE L-SHELL FORM
   PARAMETERS ARE OPTIMIMISED AROUND THE N-SHELLS RESPONSIBLE FOR 
   VISIBLE LINE CHARGE EXCHANGE SPECTROSCOPY EMISSION.

                                             H.P. SUMMERS  28 JULY 1995
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Contributors

  • Hugh Summers
  • Transitions
  • Comments
  • Origins

Data Classes

Fundamental

ADF01ADF04ADF07ADF08ADF09ADF38ADF39ADF48

Derived

ADF11ADF12ADF13ADF15ADF21ADF22