qcx#h0_ex4#c6.dat

Charge Exchange Cross Sections

Ion
C6+
Energy Range
1.000 keV/amu → 700 keV/amu

ADF01

Filename
qcx#h0_ex4#c6.dat
Full Path
adf01/qcx#h0/qcx#h0_ex4#c6.dat
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C6+ + H0(n=4) → C5+ + H+total
C6+ + H0(n=4) → C5+(n=1) + H+n-resolved
C6+ + H0(n=4) → C5+(1s) + H+nl-resolved
C6+ + H0(n=4) → C5+(n=2) + H+n-resolved
C6+ + H0(n=4) → C5+(2s) + H+nl-resolved
C6+ + H0(n=4) → C5+(2p) + H+nl-resolved
C6+ + H0(n=4) → C5+(n=3) + H+n-resolved
C6+ + H0(n=4) → C5+(3s) + H+nl-resolved
C6+ + H0(n=4) → C5+(3p) + H+nl-resolved
C6+ + H0(n=4) → C5+(3d) + H+nl-resolved
C6+ + H0(n=4) → C5+(n=4) + H+n-resolved
C6+ + H0(n=4) → C5+(4s) + H+nl-resolved
C6+ + H0(n=4) → C5+(4p) + H+nl-resolved
C6+ + H0(n=4) → C5+(4d) + H+nl-resolved
C6+ + H0(n=4) → C5+(4f) + H+nl-resolved
C6+ + H0(n=4) → C5+(n=5) + H+n-resolved
C6+ + H0(n=4) → C5+(5s) + H+nl-resolved
C6+ + H0(n=4) → C5+(5p) + H+nl-resolved
C6+ + H0(n=4) → C5+(5d) + H+nl-resolved
C6+ + H0(n=4) → C5+(5f) + H+nl-resolved
C6+ + H0(n=4) → C5+(5g) + H+nl-resolved
C6+ + H0(n=4) → C5+(n=6) + H+n-resolved
C6+ + H0(n=4) → C5+(6s) + H+nl-resolved
C6+ + H0(n=4) → C5+(6p) + H+nl-resolved
C6+ + H0(n=4) → C5+(6d) + H+nl-resolved
C6+ + H0(n=4) → C5+(6f) + H+nl-resolved
C6+ + H0(n=4) → C5+(6g) + H+nl-resolved
C6+ + H0(n=4) → C5+(6h) + H+nl-resolved
 + 6     H + 0 (1)  / receiver, donor (donor state index)    / LPARMS /
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 DATA REFORMATTED TO NEW ADF01 FORMAT.

 INPUT DATA FILE : JETSHP.CHEXDATA.DATA(C6#HEXC1)
 SUB-BLOCK USED  : 3
 SUB-BLOCK TITLE :  COMPOSITE FOR CAPTURE FROM N=4  N'**2*E =1.0KEV/AMU - 700 KEV/AMU  C+6

 COMMENT RECORDS FROM INPUT DATA FILE ARE APPENDED BELOW.

-------------------------------------------------------------------------------------------
 ======================================================================
                  H(N>1) + C(6+) --> H(+) + C(5+)
                  -------------------------------

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

      IBLOCK=3
      --------

      ENERGY    =
      N         =
      APPROX    =
      REFERENCE =

      REMARKS

                                            H.P.SUMMERS    13 DEC 1989
=======================================================================
   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

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