qcx#h0_old#h1.dat

Charge Exchange Cross Sections

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

ADF01

Filename
qcx#h0_old#h1.dat
Full Path
adf01/qcx#h0/qcx#h0_old#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
-------------------------------------------------------------------------------------------

 DATA REFORMATTED TO NEW ADF01 FORMAT.

 INPUT DATA FILE : JETSHP.CHEXDATA.DATA(H1NEW1)
 SUB-BLOCK USED  : 4
 SUB-BLOCK TITLE :  PREFERRED DATA H(+)  ; ENERGY:1_1000 KEV/AMU

 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 = 4
      ----------
      ENERGY    = 1 _ 1000 KEV/AMU
      N         = 1 _ 4
      APPROX    = BEST CHOICE FROM SEVERAL SOURCES (THEORY/EXPERIMENT)
      REFERENCE = LUDDE & DREIZLER, KIMURA & THORSON, WINTER & LIN,
                  SHAKESHAFT, FRITSCH, RYUFUKU.

      REMARKS:
      THE DATASET IS OBTAINED BY MANUALLY FITTING CURVES THROUGH
      N - SHELL FRACTIONAL CROSS-SECTION DATA.

      ALL DATA SOURCES WERE
      ANALYSED USING NEUTBEAM.FORT(CXERROR) CODE.  PLOTS OF ALPHA
      AND ITS APPARENT UNCERTAINTIES WERE PREPARED AND A PREFERRED
      ALPHA CURVE DRAWN MANUALLY. THIS ANALYSIS WAS ALSO USED TO
      DEDUCE A PREFERRED N=3,4 X-SECTS.  PREFERRED N-SHELL FRACTIONS
      WERE RENORMALISED USING ALPHA ONWARD FROM THE N=3 SHELL AND
      CONVERTED TO ABSOLUTE CROSS-SECTIONS USING THE PREFERRED TOTAL.


      LFORMA ,XLCUTA, PL2A AND PL3A ARE DERIVED BY FITTING SIGMA(N,L)
      USING THE A-D-A-S ENTRY PROGRAMME FOR CHARGE EXCHANGE DATA
      FOR PRINCIPAL QUANTUM SHELL N=3 AT ALL TABULATED ENERGIES

                                      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
-----------------------------------------------------------------------
---------------------------------------------------------------------------------
---------------------------------------------------------------------------------

Contributors

  • Hugh Summers
  • Transitions
  • Comments
  • Origins

Data Classes