qcx#h0_ory#o8.dat

Charge Exchange Cross Sections

Ion
O8+
Energy Range
10.00 keV/amu → 200 keV/amu

ADF01

Filename
qcx#h0_ory#o8.dat
Full Path
adf01/qcx#h0/qcx#h0_ory#o8.dat
Download data
O8+ + H0 → O7+ + H+total
O8+ + H0 → O7+(n=2) + H+n-resolved
O8+ + H0 → O7+(2s) + H+nl-resolved
O8+ + H0 → O7+(2p) + H+nl-resolved
O8+ + H0 → O7+(n=3) + H+n-resolved
O8+ + H0 → O7+(3s) + H+nl-resolved
O8+ + H0 → O7+(3p) + H+nl-resolved
O8+ + H0 → O7+(3d) + H+nl-resolved
O8+ + H0 → O7+(n=4) + H+n-resolved
O8+ + H0 → O7+(4s) + H+nl-resolved
O8+ + H0 → O7+(4p) + H+nl-resolved
O8+ + H0 → O7+(4d) + H+nl-resolved
O8+ + H0 → O7+(4f) + H+nl-resolved
O8+ + H0 → O7+(n=5) + H+n-resolved
O8+ + H0 → O7+(5s) + H+nl-resolved
O8+ + H0 → O7+(5p) + H+nl-resolved
O8+ + H0 → O7+(5d) + H+nl-resolved
O8+ + H0 → O7+(5f) + H+nl-resolved
O8+ + H0 → O7+(5g) + H+nl-resolved
O8+ + H0 → O7+(n=6) + H+n-resolved
O8+ + H0 → O7+(6s) + H+nl-resolved
O8+ + H0 → O7+(6p) + H+nl-resolved
O8+ + H0 → O7+(6d) + H+nl-resolved
O8+ + H0 → O7+(6f) + H+nl-resolved
O8+ + H0 → O7+(6g) + H+nl-resolved
O8+ + H0 → O7+(6h) + H+nl-resolved
O8+ + H0 → O7+(n=7) + H+n-resolved
O8+ + H0 → O7+(7s) + H+nl-resolved
O8+ + H0 → O7+(7p) + H+nl-resolved
O8+ + H0 → O7+(7d) + H+nl-resolved
O8+ + H0 → O7+(7f) + H+nl-resolved
O8+ + H0 → O7+(7g) + H+nl-resolved
O8+ + H0 → O7+(7h) + H+nl-resolved
O8+ + H0 → O7+(7i) + H+nl-resolved
O8+ + H0 → O7+(n=8) + H+n-resolved
O8+ + H0 → O7+(8s) + H+nl-resolved
O8+ + H0 → O7+(8p) + H+nl-resolved
O8+ + H0 → O7+(8d) + H+nl-resolved
O8+ + H0 → O7+(8f) + H+nl-resolved
O8+ + H0 → O7+(8g) + H+nl-resolved
O8+ + H0 → O7+(8h) + H+nl-resolved
O8+ + H0 → O7+(8i) + H+nl-resolved
O8+ + H0 → O7+(8j) + H+nl-resolved
O8+ + H0 → O7+(n=9) + H+n-resolved
O8+ + H0 → O7+(9s) + H+nl-resolved
O8+ + H0 → O7+(9p) + H+nl-resolved
O8+ + H0 → O7+(9d) + H+nl-resolved
O8+ + H0 → O7+(9f) + H+nl-resolved
O8+ + H0 → O7+(9g) + H+nl-resolved
O8+ + H0 → O7+(9h) + H+nl-resolved
O8+ + H0 → O7+(9i) + H+nl-resolved
O8+ + H0 → O7+(9j) + H+nl-resolved
O8+ + H0 → O7+(9k) + H+nl-resolved
O8+ + H0 → O7+(n=10) + H+n-resolved
O8+ + H0 → O7+(10s) + H+nl-resolved
O8+ + H0 → O7+(10p) + H+nl-resolved
O8+ + H0 → O7+(10d) + H+nl-resolved
O8+ + H0 → O7+(10f) + H+nl-resolved
O8+ + H0 → O7+(10g) + H+nl-resolved
O8+ + H0 → O7+(10h) + H+nl-resolved
O8+ + H0 → O7+(10i) + H+nl-resolved
O8+ + H0 → O7+(10j) + H+nl-resolved
O8+ + H0 → O7+(10k) + H+nl-resolved
O8+ + H0 → O7+(10l) + H+nl-resolved
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 DATA REFORMATTED TO NEW ADF01 FORMAT.

 INPUT DATA FILE : JETSHP.CHEXDATA.DATA(O8NEW1)
 SUB-BLOCK USED  : 1
 SUB-BLOCK TITLE :  UDWA    H. RYUFUKU      10.0KEV/AMU - 200.0KEV/AMU     O+8

 COMMENT RECORDS FROM INPUT DATA FILE ARE APPENDED BELOW.

-------------------------------------------------------------------------------------------
 ===================================================================== 
                        H(1S) + O(8+) --> H(+) + O(7+)                 
                        ------------------------------                 
                                                                       
      INFORMATION                              #1989 RESTRUCTURED DATA 
      -----------                                                      
      THE FOLLOWING OPTIONS ARE AVAILABLE SELECTED BY IBLOCK           
                                                                       
      IBLOCK=1                                                         
      ________                                                         
                                                                       
      ENERGY    = 10.0KEV/AMU - 200.0KEV/AMU                           
      N         =           2 - 10                                     
      APPROX    = UDWA                                                 
      REFERENCE = H. RYUFUKU                                           
                  JAERI-M-82-031                                       
                  1982                                                 
      REMARKS                                                          
             ONLY THE SIGMA(TOTAL) AND SIGMA(N)'S OF RYUFUKU ARE       
      USED.  THE ASYMPTOTIC PROJECTION SLOPE'S ALPHA ARE INFERRED      
      FROM THE LAST TWO SIGMA(N) VALUES.                               
      NO TAIL CORRECTION IS REQUIRED HERE SO ITAIL=0.                  
                                                                       
      LFORMA, XLCUTA, PL2A, PL3A
            THESE ARE DERIVED BY INSPECTION OF THE PRINCIPAL QUANTA    
      CLOSEST OR EQUAL TO N=10 FOR SIGMA(N,L) AT                       
      ALL ENERGIES -------- RYUFUKU (1982) ......... UDW               
                                                                       
                                         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

Data Classes

Fundamental

ADF01ADF04ADF07ADF08ADF09ADF38ADF39ADF48

Derived

ADF11ADF12ADF13ADF15ADF21ADF22