qcx#h0_ofr#o8.dat
Charge Exchange Cross Sections
- Ion
- O8+
- Energy Range
- 1.000 keV/amu → 700 keV/amu
| O8+ + H0 → O7+ + H+ | total |
| 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 |
Contributors
- Hugh Summers
------------------------------------------------------------------------------------------- DATA REFORMATTED TO NEW ADF01 FORMAT. INPUT DATA FILE : JETSHP.CHEXDATA.DATA(O8NEW1) SUB-BLOCK USED : 2 SUB-BLOCK TITLE : CCAO FRITSCH 1.0-42 KEV/AMU FULL RANGE 1.0-700 KEV/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=2 ________ ENERGY = 1.0KEV/AMU - 700.0KEV/AMU N = 4 - 10 APPROX = CCAO + UDWA COMBINED PREFERRED CURVES REFERENCE = W. FRITSCH (1984), W. FRITSCH & C.D. LIN (1984) W. FRITSCH (1989), H. RYUFUKU (1982) REMARKS THE DATASET IS OBTAINED BY MANUALLY FITTING CURVES THROUGH N - SHELL FRACTIONAL CROSS-SECTION DATA INFLUENCED BY THE ABOVE AUTHORS. ONLY THE SIGMA(TOTAL) AND SIGMA(N) ARE USED. THE ASYMPTOTIC PROJECTION SLOPE'S ALPHA ARE INFERRED AS A PREFERRED CURVE FROM THE BEHAVIOUR AND SPREAD OF VALUES FROM SUBDOMINANT PAIRS OF SIGMA(N) VALUES. A TAIL CORRECTION IS NOT INCLUDED SO ITAIL=0 THE PREFERRED TOTAL IS AS IN IONATOM.DATA(H). 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=8. A PREFERRED CURVE IS DEVELOPED FROM AN ASSESSMENT BY KONIG (JUNE 1990) INCLUDING OTHER HYDROGENIC IONS. FRITSCH MAY ALTER THE LOW ENERGY DATA IN THE LIGHT OF DETAILED WORK ON THE EFFECT OF EXCITED HYDROGEN STATES. THE PRESENT DATA OF FRITSCH EXCLUDES(?) PASSAGE THROUGH EXCITED HYDROGEN STATES IN THE COLLISION. H.P.SUMMERS 20 JUN 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 ----------------------------------------------------------------------- --------------------------------------------------------------------------------- ---------------------------------------------------------------------------------