qcx#h0_ool#o8.dat
Charge Exchange Cross Sections
- Ion
- O8+
- Energy Range
- 0.100 keV/amu → 100 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 : 3 SUB-BLOCK TITLE : CTMC OLSEN 50-100 KEV/AMU FULL RANGE 0.1-100KEV/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=3 ________ ENERGY = 0.1KEV/AMU - 30.0KEV/AMU N = 4 - 10 APPROX = CCAO REFERENCE = W. FRITSCH (1984), W.FRITSCH & C.D. LIN (1984) ENERGY = 50.0KEV/AMU - 100.0KEV/AMU N = 4 - 10 APPROX = CTMC REFERENCE = R.E. OLSEN (1981). REMARKS ONLY THE SIGMA(TOTAL) AND SIGMA(N)'S ARE USED. THE CCAO DATA IS THE SAME AS FOR THOERY 2 ABOVE. THE ASYMPTOTIC PROJECTION SLOPE'S ALPHA ARE INFERRED FROM THE LAST TWO SIGMA(N) VALUES. A TAIL CORRECTION IS NOT INCLUDED SO ITAIL=0. LFORMA, XLCUTA, PL2A, PL3A THESE ARE DERIVED BY INSPECTION OF THE PRINCIPAL QUANTA CLOSEST OR EQUAL TO N=10 FOR SIGMA(N,L) AT E< 50KEV/AMU -------- FRITSCH & LIN (1984) ...... CCAO E>=50KEV/AMU -------- RYUFUKU (1982) ............ UDW H.P.SUMMERS 13 DEC 1989 ======================================================================= 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 ----------------------------------------------------------------------- --------------------------------------------------------------------------------- ---------------------------------------------------------------------------------