bms97#h_li3.dat
BMS: Effective Beam Stopping Coefficients
- Ion
- Li3+
- Temperature Range
- 100 eV → 5.000 x 104 eV
- Density Range
- 1.000 x 1012 cm-3 → 1.000 x 1015 cm-3
- Energy Range
- 5000 eV/amu → 1.250 x 105 eV/amu
Reference Parameters
Reference Temperature: 2000 eVReference Density: 6.000 x 1013 cm-3
Reference Energy: 6.500 x 104 eV
(Data are provided as scans from the above reference values.)
Processes
- Li3+ + H0 → Li3+ + H+ + e
- Li3+ + H0 → Li2+ + H+
(Note that included processes are more complex in that full density dependent GCR calculations are used, the above processes are simply an indication of the effective data the ADF21 file provides.)
Contributors
- K P Dere
- Harvey Anderson
WORKING ACCURACY OF THE EFFECTIVE BEAM STOPPING COEFFICIENT AT THE REFERENCE REFERENCE REFERENCE REFERENCE ENERGY, DENSITY AND TEMPERATURE ENERGY DENSITY TEMPERATURE --------------------------------------- --------- --------- ----------- +/-10.20% 6.50D+04 keV/amu 6.00D+13 cm-3 2.00D+03 eV WORKING ACCURACY OF THE EFFECTIVE BEAM STOPPING ELECTRON REFERENCE COEFFICIENT AT THE REFERENCE TEMPERATURE DENSITY TEMPERATURE ------------------------------------------------ ------------ ----------- +/- 3.73% @ 15 keV/amu +/- 9.58% @ 35 keV/amu +/- 8.45% @ 70 keV/amu 1.00D+12 cm-3 2.00D+03 eV +/- 3.64% @ 15 keV/amu +/- 9.86% @ 35 keV/amu +/- 9.09% @ 70 keV/amu 2.00D+12 cm-3 2.00D+03 eV +/- 3.62% @ 15 keV/amu +/-10.02% @ 35 keV/amu +/- 9.41% @ 70 keV/amu 3.00D+12 cm-3 2.00D+03 eV +/- 3.53% @ 15 keV/amu +/-10.15% @ 35 keV/amu +/- 9.75% @ 70 keV/amu 5.00D+12 cm-3 2.00D+03 eV +/- 3.52% @ 15 keV/amu +/-10.12% @ 35 keV/amu +/- 9.83% @ 70 keV/amu 6.00D+12 cm-3 2.00D+03 eV +/- 3.51% @ 15 keV/amu +/-10.16% @ 35 keV/amu +/- 9.85% @ 70 keV/amu 7.00D+12 cm-3 2.00D+03 eV +/- 3.51% @ 15 keV/amu +/-10.13% @ 35 keV/amu +/- 9.87% @ 70 keV/amu 8.00D+12 cm-3 2.00D+03 eV +/- 3.43% @ 15 keV/amu +/-10.10% @ 35 keV/amu +/- 9.84% @ 70 keV/amu 9.00D+12 cm-3 2.00D+03 eV +/- 3.50% @ 15 keV/amu +/-10.15% @ 35 keV/amu +/- 9.86% @ 70 keV/amu 1.00D+13 cm-3 2.00D+03 eV +/- 3.38% @ 15 keV/amu +/- 9.97% @ 35 keV/amu +/- 9.72% @ 70 keV/amu 2.00D+13 cm-3 2.00D+03 eV +/- 3.35% @ 15 keV/amu +/- 9.72% @ 35 keV/amu +/- 9.54% @ 70 keV/amu 3.00D+13 cm-3 2.00D+03 eV +/- 3.31% @ 15 keV/amu +/- 9.48% @ 35 keV/amu +/- 9.29% @ 70 keV/amu 5.00D+13 cm-3 2.00D+03 eV +/- 3.22% @ 15 keV/amu +/- 9.35% @ 35 keV/amu +/- 9.13% @ 70 keV/amu 6.00D+13 cm-3 2.00D+03 eV +/- 3.21% @ 15 keV/amu +/- 9.29% @ 35 keV/amu +/- 8.98% @ 70 keV/amu 7.00D+13 cm-3 2.00D+03 eV +/- 3.19% @ 15 keV/amu +/- 9.17% @ 35 keV/amu +/- 8.90% @ 70 keV/amu 8.00D+13 cm-3 2.00D+03 eV +/- 3.18% @ 15 keV/amu +/- 9.06% @ 35 keV/amu +/- 8.83% @ 70 keV/amu 9.00D+13 cm-3 2.00D+03 eV +/- 3.17% @ 15 keV/amu +/- 9.02% @ 35 keV/amu +/- 8.77% @ 70 keV/amu 1.00D+14 cm-3 2.00D+03 eV +/- 3.09% @ 15 keV/amu +/- 8.47% @ 35 keV/amu +/- 8.19% @ 70 keV/amu 2.00D+14 cm-3 2.00D+03 eV +/- 2.98% @ 15 keV/amu +/- 8.13% @ 35 keV/amu +/- 7.85% @ 70 keV/amu 3.00D+14 cm-3 2.00D+03 eV +/- 2.87% @ 15 keV/amu +/- 7.83% @ 35 keV/amu +/- 7.51% @ 70 keV/amu 5.00D+14 cm-3 2.00D+03 eV +/- 2.92% @ 15 keV/amu +/- 7.72% @ 35 keV/amu +/- 7.44% @ 70 keV/amu 6.00D+14 cm-3 2.00D+03 eV +/- 2.91% @ 15 keV/amu +/- 7.62% @ 35 keV/amu +/- 7.33% @ 70 keV/amu 7.00D+14 cm-3 2.00D+03 eV +/- 2.84% @ 15 keV/amu +/- 7.53% @ 35 keV/amu +/- 7.29% @ 70 keV/amu 8.00D+14 cm-3 2.00D+03 eV +/- 2.83% @ 15 keV/amu +/- 7.50% @ 35 keV/amu +/- 7.20% @ 70 keV/amu 9.00D+14 cm-3 2.00D+03 eV +/- 2.82% @ 15 keV/amu +/- 7.48% @ 35 keV/amu +/- 7.12% @ 70 keV/amu 1.00D+15 cm-3 2.00D+03 eV WORKING ACCURACY OF THE EFFECTIVE BEAM STOPPING COEFFICIENT AT THE REFERENCE REFERENCE REFERENCE ENERGY AND DENSITY ENERGY DENSITY TEMPERATURE --------------------------------------- --------- --------- ----------- +/- 9.10% 6.50D+04 keV/amu 6.00D+13 cm-3 1.00D+02 eV +/- 9.08% 6.50D+04 keV/amu 6.00D+13 cm-3 2.00D+02 eV +/- 9.26% 6.50D+04 keV/amu 6.00D+13 cm-3 3.00D+02 eV +/- 9.43% 6.50D+04 keV/amu 6.00D+13 cm-3 5.00D+02 eV +/- 9.59% 6.50D+04 keV/amu 6.00D+13 cm-3 6.00D+02 eV +/- 9.61% 6.50D+04 keV/amu 6.00D+13 cm-3 7.00D+02 eV +/- 9.75% 6.50D+04 keV/amu 6.00D+13 cm-3 8.00D+02 eV +/- 9.81% 6.50D+04 keV/amu 6.00D+13 cm-3 8.97D+02 eV +/- 9.87% 6.50D+04 keV/amu 6.00D+13 cm-3 1.00D+03 eV +/-10.20% 6.50D+04 keV/amu 6.00D+13 cm-3 2.00D+03 eV +/-10.27% 6.50D+04 keV/amu 6.00D+13 cm-3 3.00D+03 eV +/-10.10% 6.50D+04 keV/amu 6.00D+13 cm-3 5.00D+03 eV +/- 9.91% 6.50D+04 keV/amu 6.00D+13 cm-3 6.00D+03 eV +/- 9.63% 6.50D+04 keV/amu 6.00D+13 cm-3 7.00D+03 eV +/- 9.40% 6.50D+04 keV/amu 6.00D+13 cm-3 8.00D+03 eV +/- 9.24% 6.50D+04 keV/amu 6.00D+13 cm-3 8.97D+03 eV +/- 8.94% 6.50D+04 keV/amu 6.00D+13 cm-3 1.00D+04 eV +/- 6.75% 6.50D+04 keV/amu 6.00D+13 cm-3 2.00D+04 eV +/- 4.70% 6.50D+04 keV/amu 6.00D+13 cm-3 3.00D+04 eV +/- 3.57% 6.50D+04 keV/amu 6.00D+13 cm-3 5.00D+04 eV NOTE : Working accuracy The working accuracy was obtained by calculating the effective beam stopping coefficient via ADAS310 using three different ion/atom collision cross-section databases, i.e. ADF02 type files. An ADF02 type file contains indexed entries of key ion/atom reaction cross- sections with H and other species. The first detailed assessment of ion/atom cross section data for beam stopping was completed at JET in 1989 ( small corrections and extensions were made to the file up to 1993 ) . This file was originally saved /adas/adf02/ionatom/h.dat but was later reformatted and saved as /adf02/sia#h/sia#h_rfm#h.dat. Guided by experimental observations at JET and the lack of high quality CCAO calculations when the JET 1989 data set was compiled, the cross-sections of the JET 1989 data set was considered to be some what under-estimated. A new review of all ion/atom collision data was carried out. The only substantial contribution found was that of the close coupled atomic orbital (CCAO) calculations of Toshima & Tawara [1]. This data together with the data of Janev & Smith [2] was used to create yet another ADF02 type file, sia#h_tosh#h.dat.However,the CCAO calculations of Toshima & Tawara[1] only include states up to n=4 and so some over-estimation is present, particularly for ion impact ionisation from n=3 and n=4 shell. The cross-sections contained in this data set are considered to be over- estimated. A comparative data set was constructed which was a compromise between both data sets,this is what is called the JET 1997 review data set, sia#h_j97#h.dat. The JET 1997 review data is the preferred data set. The working accuracy was obtained by running ADAS310 using each data set. The results from using the JET 1997 review data is taken as the most accurate value.The results from using the JET 1989 data set are used to obtain a lower limit.The results from the Toshima & Tawara data set are used to obtain an upper limit. Using the values of the lower and upper limit a percentage difference is used to describe the MAXIMUM deviation from the results obtained using the JET 1997 review data. REFERENCES [1] Toshima,N. & Tawara,H.,NIFS-DATA-26,July 1995. [2] Janev,R.K.& Smith,J.J.,J.Nucl.Fusion(Supplement),Vol.4,1993. CONTACT : HARVEY ANDERSON UNIVERSITY OF STRATHCLYDE ANDERSON@CHAMBA.PHYS.STRATH.AC.UK DATE : 08/07/97 ------------------------------------------------------------------------------- --------------------------------------------------------------------------------- ---------------------------------------------------------------------------------