qcx#h0_ool#c6.dat
Charge Exchange Cross Sections
- Ion
- C6+
- Energy Range
- 0.100 keV/amu → 100 keV/amu
ADF01
- Filename
- qcx#h0_ool#c6.dat
- Full Path
- adf01/qcx#h0/qcx#h0_ool#c6.dat
Download data
| C6+ + H0 → C5+ + H+ | total |
| C6+ + H0 → C5+(n=4) + H+ | n-resolved |
| C6+ + H0 → C5+(4s) + H+ | nl-resolved |
| C6+ + H0 → C5+(4p) + H+ | nl-resolved |
| C6+ + H0 → C5+(4d) + H+ | nl-resolved |
| C6+ + H0 → C5+(4f) + H+ | nl-resolved |
| C6+ + H0 → C5+(n=5) + H+ | n-resolved |
| C6+ + H0 → C5+(5s) + H+ | nl-resolved |
| C6+ + H0 → C5+(5p) + H+ | nl-resolved |
| C6+ + H0 → C5+(5d) + H+ | nl-resolved |
| C6+ + H0 → C5+(5f) + H+ | nl-resolved |
| C6+ + H0 → C5+(5g) + H+ | nl-resolved |
| C6+ + H0 → C5+(n=6) + H+ | n-resolved |
| C6+ + H0 → C5+(6s) + H+ | nl-resolved |
| C6+ + H0 → C5+(6p) + H+ | nl-resolved |
| C6+ + H0 → C5+(6d) + H+ | nl-resolved |
| C6+ + H0 → C5+(6f) + H+ | nl-resolved |
| C6+ + H0 → C5+(6g) + H+ | nl-resolved |
| C6+ + H0 → C5+(6h) + H+ | nl-resolved |
| C6+ + H0 → C5+(n=7) + H+ | n-resolved |
| C6+ + H0 → C5+(7s) + H+ | nl-resolved |
| C6+ + H0 → C5+(7p) + H+ | nl-resolved |
| C6+ + H0 → C5+(7d) + H+ | nl-resolved |
| C6+ + H0 → C5+(7f) + H+ | nl-resolved |
| C6+ + H0 → C5+(7g) + H+ | nl-resolved |
| C6+ + H0 → C5+(7h) + H+ | nl-resolved |
| C6+ + H0 → C5+(7i) + H+ | nl-resolved |
| C6+ + H0 → C5+(n=8) + H+ | n-resolved |
| C6+ + H0 → C5+(8s) + H+ | nl-resolved |
| C6+ + H0 → C5+(8p) + H+ | nl-resolved |
| C6+ + H0 → C5+(8d) + H+ | nl-resolved |
| C6+ + H0 → C5+(8f) + H+ | nl-resolved |
| C6+ + H0 → C5+(8g) + H+ | nl-resolved |
| C6+ + H0 → C5+(8h) + H+ | nl-resolved |
| C6+ + H0 → C5+(8i) + H+ | nl-resolved |
| C6+ + H0 → C5+(8j) + H+ | nl-resolved |
+ 6 H + 0 (1) / receiver, donor (donor state index) / LPARMS / ------------------------------------------------------------------------------------------- DATA REFORMATTED TO NEW ADF01 FORMAT. INPUT DATA FILE : JETSHP.CHEXDATA.DATA(C6NEW1) SUB-BLOCK USED : 3 SUB-BLOCK TITLE : CTMC OLSEN 25-100 KEV/AMU FULL RANGE 0.1-100 KEV/AMU C+6 COMMENT RECORDS FROM INPUT DATA FILE ARE APPENDED BELOW. ------------------------------------------------------------------------------------------- ===================================================================== H(1S) + C(6+) --> H(+) + C(5+) ------------------------------ INFORMATION #1989 RESTRUCTURED DATA ----------- THE FOLLOWING OPTIONS ARE AVAILABLE SELECTED BY ITHEOR IBLOCK=3 ________ ENERGY = 0.1KEV/AMU - 30.0KEV/AMU N = 4 - 8 APPROX = CCAO REFERENCE = W. FRITSCH (1984), W.FRITSCH & C.D. LIN (1984) ENERGY = 50.0KEV/AMU - 100.0KEV/AMU N = 4 - 8 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=8 FOR SIGMA(N,L) AT E< 50KEV/AMU -------- FRITSCH & LIN (1984,84) ... CCAO (N=4,5,8) E>=50KEV/AMU -------- RYUFUKU (1982) ............ UDW (N=7,8) J. SPENCE 22 MAY 1986 H.P. SUMMERS & S. TURNER 10 JULY 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 ----------------------------------------------------------------------- --------------------------------------------------------------------------------- ---------------------------------------------------------------------------------