qcx#li0_kvi#ne10.dat

Charge Exchange Cross Sections

Ion
Ne10+
Energy Range
1.000 keV/amu → 10.00 keV/amu

ADF01

Filename
qcx#li0_kvi#ne10.dat
Full Path
adf01/qcx#li0/qcx#li0_kvi#ne10.dat
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Ne10+ + Li0(2s) → Ne9+ + Li+total
Ne10+ + Li0(2s) → Ne9+(n=8) + Li+n-resolved
Ne10+ + Li0(2s) → Ne9+(8s) + Li+nl-resolved
Ne10+ + Li0(2s) → Ne9+(8p) + Li+nl-resolved
Ne10+ + Li0(2s) → Ne9+(8d) + Li+nl-resolved
Ne10+ + Li0(2s) → Ne9+(8f) + Li+nl-resolved
Ne10+ + Li0(2s) → Ne9+(8g) + Li+nl-resolved
Ne10+ + Li0(2s) → Ne9+(8h) + Li+nl-resolved
Ne10+ + Li0(2s) → Ne9+(8i) + Li+nl-resolved
Ne10+ + Li0(2s) → Ne9+(8j) + Li+nl-resolved
Ne10+ + Li0(2s) → Ne9+(n=9) + Li+n-resolved
Ne10+ + Li0(2s) → Ne9+(9s) + Li+nl-resolved
Ne10+ + Li0(2s) → Ne9+(9p) + Li+nl-resolved
Ne10+ + Li0(2s) → Ne9+(9d) + Li+nl-resolved
Ne10+ + Li0(2s) → Ne9+(9f) + Li+nl-resolved
Ne10+ + Li0(2s) → Ne9+(9g) + Li+nl-resolved
Ne10+ + Li0(2s) → Ne9+(9h) + Li+nl-resolved
Ne10+ + Li0(2s) → Ne9+(9i) + Li+nl-resolved
Ne10+ + Li0(2s) → Ne9+(9j) + Li+nl-resolved
Ne10+ + Li0(2s) → Ne9+(9k) + Li+nl-resolved
Ne10+ + Li0(2s) → Ne9+(n=10) + Li+n-resolved
Ne10+ + Li0(2s) → Ne9+(10s) + Li+nl-resolved
Ne10+ + Li0(2s) → Ne9+(10p) + Li+nl-resolved
Ne10+ + Li0(2s) → Ne9+(10d) + Li+nl-resolved
Ne10+ + Li0(2s) → Ne9+(10f) + Li+nl-resolved
Ne10+ + Li0(2s) → Ne9+(10g) + Li+nl-resolved
Ne10+ + Li0(2s) → Ne9+(10h) + Li+nl-resolved
Ne10+ + Li0(2s) → Ne9+(10i) + Li+nl-resolved
Ne10+ + Li0(2s) → Ne9+(10j) + Li+nl-resolved
Ne10+ + Li0(2s) → Ne9+(10k) + Li+nl-resolved
Ne10+ + Li0(2s) → Ne9+(10l) + Li+nl-resolved
Ne10+ + Li0(2s) → Ne9+(n=11) + Li+n-resolved
Ne10+ + Li0(2s) → Ne9+(11s) + Li+nl-resolved
Ne10+ + Li0(2s) → Ne9+(11p) + Li+nl-resolved
Ne10+ + Li0(2s) → Ne9+(11d) + Li+nl-resolved
Ne10+ + Li0(2s) → Ne9+(11f) + Li+nl-resolved
Ne10+ + Li0(2s) → Ne9+(11g) + Li+nl-resolved
Ne10+ + Li0(2s) → Ne9+(11h) + Li+nl-resolved
Ne10+ + Li0(2s) → Ne9+(11i) + Li+nl-resolved
Ne10+ + Li0(2s) → Ne9+(11j) + Li+nl-resolved
Ne10+ + Li0(2s) → Ne9+(11k) + Li+nl-resolved
Ne10+ + Li0(2s) → Ne9+(11l) + Li+nl-resolved
Ne10+ + Li0(2s) → Ne9+(11m) + Li+nl-resolved
Ne10+ + Li0(2s) → Ne9+(n=12) + Li+n-resolved
Ne10+ + Li0(2s) → Ne9+(12s) + Li+nl-resolved
Ne10+ + Li0(2s) → Ne9+(12p) + Li+nl-resolved
Ne10+ + Li0(2s) → Ne9+(12d) + Li+nl-resolved
Ne10+ + Li0(2s) → Ne9+(12f) + Li+nl-resolved
Ne10+ + Li0(2s) → Ne9+(12g) + Li+nl-resolved
Ne10+ + Li0(2s) → Ne9+(12h) + Li+nl-resolved
Ne10+ + Li0(2s) → Ne9+(12i) + Li+nl-resolved
Ne10+ + Li0(2s) → Ne9+(12j) + Li+nl-resolved
Ne10+ + Li0(2s) → Ne9+(12k) + Li+nl-resolved
Ne10+ + Li0(2s) → Ne9+(12l) + Li+nl-resolved
Ne10+ + Li0(2s) → Ne9+(12m) + Li+nl-resolved
Ne10+ + Li0(2s) → Ne9+(12n) + Li+nl-resolved
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  Source:  The data consists of results of CTMC calculations made at the University of Missouri over 
              the period 1995-97.
     
  Comments:  From the comparison of CTMC calculations for Be+4, B+5 and C+6 with experiments performed
             at KVI, it seems that in the 1-15 keV/amu energy range, these collisions are well 
             described by the theory.  For verification, we compared our data with the recommended
             scaled cross-sections of Schweinzer et al (1994).  Agreement is good.  It is to be noted
             that the scaled formulae of Schweinzer are to be used with the effective principal quantum
             number of the donor state.  Calculations of Fritsch and Lin
             (1984) for C+4 are in agreement with the CTMC results for Be+4.  Also total one-electron 
             capture cross-sections, which were experimentally determined by different groups 
             confirm the results for one-electron capture in He+2 collisions.  

             The data was assembled as ADAS data files of type adf01 at JET Joint Undertaking in the
             period    

  Authors:   J. W. Turkstra, G. Lubinski, R. Hoekstra*, R. E. Olson#
                  * KVI, Groningen, Netherlands
                  # University of Missouri, Rolla, USA. 

  Date:  9 June 1997.

  Updates:  23/12/97  R. Hoekstra & H.P. Summers - amended comments section following clarifications
                                                   by Schweinzer. 

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Dependents

Contributors

  • Kernfysisch Versneller Instituut
  • Hugh Summers
  • Transitions
  • Comments
  • Origins

Data Classes

Fundamental

ADF01ADF04ADF07ADF08ADF09ADF38ADF39ADF48

Derived

ADF11ADF12ADF13ADF15ADF21ADF22