qcx#h0_ory#h1.dat

Charge Exchange Cross Sections

Ion
H1+
Energy Range
10.00 keV/amu → 1000 keV/amu

ADF01

Filename
qcx#h0_ory#h1.dat
Full Path
adf01/qcx#h0/qcx#h0_ory#h1.dat
Download data
H+ + H0 → H0 + H+total
H+ + H0 → H0(n=1) + H+n-resolved
H+ + H0 → H0(1s) + H+nl-resolved
H+ + H0 → H0(n=2) + H+n-resolved
H+ + H0 → H0(2s) + H+nl-resolved
H+ + H0 → H0(2p) + H+nl-resolved
H+ + H0 → H0(n=3) + H+n-resolved
H+ + H0 → H0(3s) + H+nl-resolved
H+ + H0 → H0(3p) + H+nl-resolved
H+ + H0 → H0(3d) + H+nl-resolved
H+ + H0 → H0(n=4) + H+n-resolved
H+ + H0 → H0(4s) + H+nl-resolved
H+ + H0 → H0(4p) + H+nl-resolved
H+ + H0 → H0(4d) + H+nl-resolved
H+ + H0 → H0(4f) + H+nl-resolved
H+ + H0 → H0(n=5) + H+n-resolved
H+ + H0 → H0(5s) + H+nl-resolved
H+ + H0 → H0(5p) + H+nl-resolved
H+ + H0 → H0(5d) + H+nl-resolved
H+ + H0 → H0(5f) + H+nl-resolved
H+ + H0 → H0(5g) + H+nl-resolved
H+ + H0 → H0(n=6) + H+n-resolved
H+ + H0 → H0(6s) + H+nl-resolved
H+ + H0 → H0(6p) + H+nl-resolved
H+ + H0 → H0(6d) + H+nl-resolved
H+ + H0 → H0(6f) + H+nl-resolved
H+ + H0 → H0(6g) + H+nl-resolved
H+ + H0 → H0(6h) + H+nl-resolved
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 DATA REFORMATTED TO NEW ADF01 FORMAT.

 INPUT DATA FILE : JETSHP.CHEXDATA.DATA(H1NEW1)
 SUB-BLOCK USED  : 1
 SUB-BLOCK TITLE :  UDWA    H. RYUFUKU      10.0KEV/AMU - 1000.0KEV/AMU  H + 1

 COMMENT RECORDS FROM INPUT DATA FILE ARE APPENDED BELOW.

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

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

      IBLOCK=1
      ________

      ENERGY    = 10.0KEV/AMU - 1000.0KEV/AMU
      N         =           1 - 5
      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 AND PL3A
            THESE ARE DERIVED BY INSPECTION OF THE PRINCIPAL QUANTA
      CLOSEST OR EQUAL TO N=3 FOR SIGMA(N,L) AT
      ALL ENERGIES -------- RYUFUKU (1982) ......... UDW   (N=5)

                                          H.P.SUMMERS   12 JAN 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