qcx#h0_ory#c6.dat
Charge Exchange Cross Sections
- Ion
- C6+
- Energy Range
- 10.00 keV/amu → 200 keV/amu
ADF01
- Filename
- qcx#h0_ory#c6.dat
- Full Path
- adf01/qcx#h0/qcx#h0_ory#c6.dat
Download data
| C6+ + H0 → C5+ + H+ | total |
| C6+ + H0 → C5+(n=1) + H+ | n-resolved |
| C6+ + H0 → C5+(1s) + H+ | nl-resolved |
| C6+ + H0 → C5+(n=2) + H+ | n-resolved |
| C6+ + H0 → C5+(2s) + H+ | nl-resolved |
| C6+ + H0 → C5+(2p) + H+ | nl-resolved |
| C6+ + H0 → C5+(n=3) + H+ | n-resolved |
| C6+ + H0 → C5+(3s) + H+ | nl-resolved |
| C6+ + H0 → C5+(3p) + H+ | nl-resolved |
| C6+ + H0 → C5+(3d) + H+ | nl-resolved |
| 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 : 1 SUB-BLOCK TITLE : UDWA H. RYUFUKU 10.0KEV/AMU - 200.0KEV/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=1 ________ ENERGY = 10.0KEV/AMU - 200.0KEV/AMU N = 1 - 8 APPROX = UDWA REFERENCE = H. RYUFUKU JAERI-M-82-031 1982 REMARKS ONLY THE SIGMA(TOTAL) AND SIGMA(N)'S OF RYUFUKU ARE USED. THE ASYMPTOTIC PROJECTION SLOPE'S ALPHA ARE INFERRED FROM THE LAST TWO SIGMA(N) VALUES. NO TAIL CORRECTION IS REQUIRED HERE 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 ALL ENERGIES -------- 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 ----------------------------------------------------------------------- --------------------------------------------------------------------------------- ---------------------------------------------------------------------------------