qcx#h0_old#si14.dat

Charge Exchange Cross Sections

Ion
Si14+
Energy Range
25.00 keV/amu → 1000 keV/amu

ADF01

Filename
qcx#h0_old#si14.dat
Full Path
adf01/qcx#h0/qcx#h0_old#si14.dat
Download data
Si14+ + H0 → Si13+ + H+total
Si14+ + H0 → Si13+(n=2) + H+n-resolved
Si14+ + H0 → Si13+(2s) + H+nl-resolved
Si14+ + H0 → Si13+(2p) + H+nl-resolved
Si14+ + H0 → Si13+(n=3) + H+n-resolved
Si14+ + H0 → Si13+(3s) + H+nl-resolved
Si14+ + H0 → Si13+(3p) + H+nl-resolved
Si14+ + H0 → Si13+(3d) + H+nl-resolved
Si14+ + H0 → Si13+(n=4) + H+n-resolved
Si14+ + H0 → Si13+(4s) + H+nl-resolved
Si14+ + H0 → Si13+(4p) + H+nl-resolved
Si14+ + H0 → Si13+(4d) + H+nl-resolved
Si14+ + H0 → Si13+(4f) + H+nl-resolved
Si14+ + H0 → Si13+(n=5) + H+n-resolved
Si14+ + H0 → Si13+(5s) + H+nl-resolved
Si14+ + H0 → Si13+(5p) + H+nl-resolved
Si14+ + H0 → Si13+(5d) + H+nl-resolved
Si14+ + H0 → Si13+(5f) + H+nl-resolved
Si14+ + H0 → Si13+(5g) + H+nl-resolved
Si14+ + H0 → Si13+(n=6) + H+n-resolved
Si14+ + H0 → Si13+(6s) + H+nl-resolved
Si14+ + H0 → Si13+(6p) + H+nl-resolved
Si14+ + H0 → Si13+(6d) + H+nl-resolved
Si14+ + H0 → Si13+(6f) + H+nl-resolved
Si14+ + H0 → Si13+(6g) + H+nl-resolved
Si14+ + H0 → Si13+(6h) + H+nl-resolved
Si14+ + H0 → Si13+(n=7) + H+n-resolved
Si14+ + H0 → Si13+(7s) + H+nl-resolved
Si14+ + H0 → Si13+(7p) + H+nl-resolved
Si14+ + H0 → Si13+(7d) + H+nl-resolved
Si14+ + H0 → Si13+(7f) + H+nl-resolved
Si14+ + H0 → Si13+(7g) + H+nl-resolved
Si14+ + H0 → Si13+(7h) + H+nl-resolved
Si14+ + H0 → Si13+(7i) + H+nl-resolved
Si14+ + H0 → Si13+(n=8) + H+n-resolved
Si14+ + H0 → Si13+(8s) + H+nl-resolved
Si14+ + H0 → Si13+(8p) + H+nl-resolved
Si14+ + H0 → Si13+(8d) + H+nl-resolved
Si14+ + H0 → Si13+(8f) + H+nl-resolved
Si14+ + H0 → Si13+(8g) + H+nl-resolved
Si14+ + H0 → Si13+(8h) + H+nl-resolved
Si14+ + H0 → Si13+(8i) + H+nl-resolved
Si14+ + H0 → Si13+(8j) + H+nl-resolved
Si14+ + H0 → Si13+(n=9) + H+n-resolved
Si14+ + H0 → Si13+(9s) + H+nl-resolved
Si14+ + H0 → Si13+(9p) + H+nl-resolved
Si14+ + H0 → Si13+(9d) + H+nl-resolved
Si14+ + H0 → Si13+(9f) + H+nl-resolved
Si14+ + H0 → Si13+(9g) + H+nl-resolved
Si14+ + H0 → Si13+(9h) + H+nl-resolved
Si14+ + H0 → Si13+(9i) + H+nl-resolved
Si14+ + H0 → Si13+(9j) + H+nl-resolved
Si14+ + H0 → Si13+(9k) + H+nl-resolved
Si14+ + H0 → Si13+(n=10) + H+n-resolved
Si14+ + H0 → Si13+(10s) + H+nl-resolved
Si14+ + H0 → Si13+(10p) + H+nl-resolved
Si14+ + H0 → Si13+(10d) + H+nl-resolved
Si14+ + H0 → Si13+(10f) + H+nl-resolved
Si14+ + H0 → Si13+(10g) + H+nl-resolved
Si14+ + H0 → Si13+(10h) + H+nl-resolved
Si14+ + H0 → Si13+(10i) + H+nl-resolved
Si14+ + H0 → Si13+(10j) + H+nl-resolved
Si14+ + H0 → Si13+(10k) + H+nl-resolved
Si14+ + H0 → Si13+(10l) + H+nl-resolved
Si14+ + H0 → Si13+(n=11) + H+n-resolved
Si14+ + H0 → Si13+(11s) + H+nl-resolved
Si14+ + H0 → Si13+(11p) + H+nl-resolved
Si14+ + H0 → Si13+(11d) + H+nl-resolved
Si14+ + H0 → Si13+(11f) + H+nl-resolved
Si14+ + H0 → Si13+(11g) + H+nl-resolved
Si14+ + H0 → Si13+(11h) + H+nl-resolved
Si14+ + H0 → Si13+(11i) + H+nl-resolved
Si14+ + H0 → Si13+(11j) + H+nl-resolved
Si14+ + H0 → Si13+(11k) + H+nl-resolved
Si14+ + H0 → Si13+(11l) + H+nl-resolved
Si14+ + H0 → Si13+(11m) + H+nl-resolved
Si14+ + H0 → Si13+(n=12) + H+n-resolved
Si14+ + H0 → Si13+(12s) + H+nl-resolved
Si14+ + H0 → Si13+(12p) + H+nl-resolved
Si14+ + H0 → Si13+(12d) + H+nl-resolved
Si14+ + H0 → Si13+(12f) + H+nl-resolved
Si14+ + H0 → Si13+(12g) + H+nl-resolved
Si14+ + H0 → Si13+(12h) + H+nl-resolved
Si14+ + H0 → Si13+(12i) + H+nl-resolved
Si14+ + H0 → Si13+(12j) + H+nl-resolved
Si14+ + H0 → Si13+(12k) + H+nl-resolved
Si14+ + H0 → Si13+(12l) + H+nl-resolved
Si14+ + H0 → Si13+(12m) + H+nl-resolved
Si14+ + H0 → Si13+(12n) + H+nl-resolved
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 DATA REFORMATTED TO NEW ADF01 FORMAT.

 INPUT DATA FILE : JETSHP.CHEXDATA.DATA(SI14NEW1)
 SUB-BLOCK USED  : 1
 SUB-BLOCK TITLE :  UDWA    H. RYUFUKU      25.0KEV/AMU - 1000.0KEV/AMU     SI+14

 COMMENT RECORDS FROM INPUT DATA FILE ARE APPENDED BELOW.

-------------------------------------------------------------------------------------------
 ===================================================================== 
                        H(1S) + SI(14+) --> H(+) + SI(13+)             
                        ------------------------------                 
                                                                       
      INFORMATION                              #1989 RESTRUCTURED DATA 
      -----------                                                      
      THE FOLLOWING OPTIONS ARE AVAILABLE SELECTED BY IBLOCK           
                                                                       
      IBLOCK=1                                                         
      ________                                                         
                                                                       
      ENERGY    = 25.0KEV/AMU - 1000.0KEV/AMU                          
      N         =           1 - 12                                     
      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.                  
                                                                       
      LCUTA AND LFORMA                                                 
            THESE ARE DERIVED BY INSPECTION OF THE PRINCIPAL QUANTA    
      CLOSEST OR EQUAL TO N=12 FOR SIGMA(N,L) AT                       
      ALL ENERGIES -------- RYUFUKU (1982) ......... UDW   (N=7,8)     
                                                                       
                                                                       
                                            J. SPENCE   22 MAY 1986    
=======================================================================
   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
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