slike_jmb09#ar2.dat
Resolved Specific Ion Data Collections
- Ion
- Ar2+
- Temperature Range
- 0.155 eV → 388 eV
ADF04
- Filename
- slike_jmb09#ar2.dat
- Full Path
- adf04/slike/slike_jmb09#ar2.dat
Download data
- Spontaneous Emission: Ar+2(i) → Ar+2(j) + hv
- Electron Impact Excitation: Ar+2(i) + e → Ar+2(j) + e
| 3s2 3p4 3P2.0 | 0.0 cm-1 |
| 3s2 3p4 3P1.0 | 1112.0 cm-1 |
| 3s2 3p4 3P0.0 | 1570.0 cm-1 |
| 3s2 3p4 1D2.0 | 14010.0 cm-1 |
| 3s2 3p4 1S0.0 | 33266.0 cm-1 |
| 3s1 3p5 3P2.0 | 113800.0 cm-1 |
| 3s1 3p5 3P1.0 | 114797.0 cm-1 |
| 3s1 3p5 3P0.0 | 115328.0 cm-1 |
| 3s1 3p5 1P1.0 | 144022.0 cm-1 |
| 3s2 3p3 3d1 5D0.0 | 144420.0 cm-1 |
| 3s2 3p3 3d1 5D1.0 | 144426.0 cm-1 |
| 3s2 3p3 3d1 5D2.0 | 144439.0 cm-1 |
| 3s2 3p3 3d1 5D3.0 | 144458.0 cm-1 |
| 3s2 3p3 3d1 5D4.0 | 144484.0 cm-1 |
| 3s2 3p3 3d1 3D3.0 | 159431.0 cm-1 |
| 3s2 3p3 3d1 3D2.0 | 159443.0 cm-1 |
| 3s2 3p3 3d1 3D1.0 | 159515.0 cm-1 |
| 3s2 3p3 3d1 3F2.0 | 164780.0 cm-1 |
| 3s2 3p3 3d1 3F3.0 | 165053.0 cm-1 |
| 3s2 3p3 3d1 3F4.0 | 165396.0 cm-1 |
| 3s2 3p3 3d1 1S0.0 | 167519.0 cm-1 |
| 3s2 3p3 3d1 3G3.0 | 174531.0 cm-1 |
| 3s2 3p3 3d1 3G4.0 | 174569.0 cm-1 |
| 3s2 3p3 3d1 3G5.0 | 174620.0 cm-1 |
| 3s2 3p3 4s1 5S2.0 | 176229.0 cm-1 |
| 3s2 3p3 3d1 1G4.0 | 179222.0 cm-1 |
| 3s2 3p3 3d1 1D2.0 | 179653.0 cm-1 |
| 3s2 3p3 4s1 3S1.0 | 184637.0 cm-1 |
| 3s2 3p3 3d1 3F4.0 | 186923.0 cm-1 |
| 3s2 3p3 3d1 3F3.0 | 187149.0 cm-1 |
| 3s2 3p3 3d1 3F2.0 | 187358.0 cm-1 |
| 3s2 3p3 3d1 3D1.0 | 188672.0 cm-1 |
| 3s2 3p3 3d1 3D2.0 | 189134.0 cm-1 |
| 3s2 3p3 3d1 3P0.0 | 189413.0 cm-1 |
| 3s2 3p3 3d1 3P1.0 | 189702.0 cm-1 |
| 3s2 3p3 3d1 3D3.0 | 189792.0 cm-1 |
| 3s2 3p3 3d1 3P2.0 | 190325.0 cm-1 |
| 3s2 3p3 4s1 3D1.0 | 201924.0 cm-1 |
| 3s2 3p3 4s1 3D2.0 | 201954.0 cm-1 |
| 3s2 3p3 4s1 3D3.0 | 202008.0 cm-1 |
| 3s2 3p3 3d1 1F3.0 | 203252.0 cm-1 |
| 3s2 3p3 4s1 1D2.0 | 206056.0 cm-1 |
| 3s2 3p3 3d1 3S1.0 | 210251.0 cm-1 |
| 3s2 3p3 4p1 5P1.0 | 214696.0 cm-1 |
| 3s2 3p3 4p1 5P2.0 | 214714.0 cm-1 |
| 3s2 3p3 4p1 5P3.0 | 214743.0 cm-1 |
| 3s2 3p3 4s1 3P0.0 | 216337.0 cm-1 |
| 3s2 3p3 4s1 3P2.0 | 216347.0 cm-1 |
| 3s2 3p3 4s1 3P1.0 | 216347.0 cm-1 |
| 3s2 3p3 4p1 3P0.0 | 219090.0 cm-1 |
| 3s2 3p3 4p1 3P1.0 | 219097.0 cm-1 |
| 3s2 3p3 4p1 3P2.0 | 219148.0 cm-1 |
| 3s2 3p3 3d1 3D3.0 | 219353.0 cm-1 |
| 3s2 3p3 3d1 3D2.0 | 219921.0 cm-1 |
| 3s2 3p3 4s1 1P1.0 | 220293.0 cm-1 |
| 3s2 3p3 3d1 3D1.0 | 220334.0 cm-1 |
| 3s2 3p3 3d1 3P2.0 | 223731.0 cm-1 |
| 3s2 3p3 3d1 3P1.0 | 224248.0 cm-1 |
| 3s2 3p3 3d1 3P0.0 | 224530.0 cm-1 |
| 3s2 3p3 3d1 1D2.0 | 228519.0 cm-1 |
| 3s2 3p3 3d1 1P1.0 | 230259.0 cm-1 |
| 3s2 3p3 3d1 1F3.0 | 236262.0 cm-1 |
| 3s2 3p3 4p1 1P1.0 | 237145.0 cm-1 |
| 3s2 3p3 4p1 3D2.0 | 237675.0 cm-1 |
| 3s2 3p3 4p1 3D1.0 | 237697.0 cm-1 |
| 3s2 3p3 4p1 3D3.0 | 237789.0 cm-1 |
| 3s2 3p3 4p1 3F2.0 | 238426.0 cm-1 |
| 3s2 3p3 4p1 3F3.0 | 238467.0 cm-1 |
| 3s2 3p3 4p1 3F4.0 | 238510.0 cm-1 |
| 3s2 3p3 4p1 1F3.0 | 239239.0 cm-1 |
| 3s2 3p3 4p1 3P2.0 | 243911.0 cm-1 |
| 3s2 3p3 4p1 3P1.0 | 243919.0 cm-1 |
| 3s2 3p3 4p1 3P0.0 | 243924.0 cm-1 |
| 3s2 3p3 3d1 1P1.0 | 244577.0 cm-1 |
| 3s2 3p3 4p1 1D2.0 | 247478.0 cm-1 |
| 3s2 3p3 4d1 5D0.0 | 248827.0 cm-1 |
| 3s2 3p3 4d1 5D1.0 | 248829.0 cm-1 |
| 3s2 3p3 4d1 5D2.0 | 248834.0 cm-1 |
| 3s2 3p3 4d1 5D3.0 | 248842.0 cm-1 |
| 3s2 3p3 4d1 5D4.0 | 248853.0 cm-1 |
| 3s2 3p3 4p1 3S1.0 | 253228.0 cm-1 |
| 3s2 3p3 4p1 3D3.0 | 253869.0 cm-1 |
| 3s2 3p3 4p1 3D1.0 | 253888.0 cm-1 |
| 3s2 3p3 4p1 3D2.0 | 253892.0 cm-1 |
| 3s2 3p3 5s1 5S2.0 | 254292.0 cm-1 |
| 3s2 3p3 4p1 1P1.0 | 255169.0 cm-1 |
| 3s2 3p3 5s1 3S1.0 | 255823.0 cm-1 |
| 3s2 3p3 4p1 3P0.0 | 256958.0 cm-1 |
| 3s2 3p3 4p1 3P1.0 | 256974.0 cm-1 |
| 3s2 3p3 4p1 3P2.0 | 256976.0 cm-1 |
| 3s2 3p3 4d1 3D2.0 | 257565.0 cm-1 |
| 3s2 3p3 4d1 3D3.0 | 257573.0 cm-1 |
| 3s2 3p3 4d1 3D1.0 | 257586.0 cm-1 |
| 3s2 3p3 4p1 1D2.0 | 258117.0 cm-1 |
| 3s2 3p3 4p1 1S0.0 | 265769.0 cm-1 |
| 3s2 3p3 4f1 5F1.0 | 266717.0 cm-1 |
| 3s2 3p3 4f1 5F2.0 | 266717.0 cm-1 |
| 3s2 3p3 4f1 5F3.0 | 266718.0 cm-1 |
| 3s2 3p3 4f1 5F4.0 | 266718.0 cm-1 |
| 3s2 3p3 4f1 5F5.0 | 266719.0 cm-1 |
| 3s2 3p3 4f1 3F2.0 | 267486.0 cm-1 |
| 3s2 3p3 4f1 3F3.0 | 267489.0 cm-1 |
| 3s2 3p3 4f1 3F4.0 | 267494.0 cm-1 |
| 3s2 3p3 4d1 3F2.0 | 271649.0 cm-1 |
| 3s2 3p3 4d1 3F3.0 | 271765.0 cm-1 |
| 3s2 3p3 4d1 1S0.0 | 271896.0 cm-1 |
| 3s2 3p3 4d1 3F4.0 | 271910.0 cm-1 |
| 3s2 3p3 4d1 3G3.0 | 272760.0 cm-1 |
| 3s2 3p3 4d1 3G4.0 | 272791.0 cm-1 |
| 3s2 3p3 4d1 3G5.0 | 272822.0 cm-1 |
| 3s2 3p3 4d1 1G4.0 | 273432.0 cm-1 |
| 3s2 3p3 4d1 3D1.0 | 275539.0 cm-1 |
| 3s2 3p3 4d1 3D2.0 | 275605.0 cm-1 |
| 3s2 3p3 4d1 3D3.0 | 275660.0 cm-1 |
| 3s2 3p3 5s1 3D1.0 | 277684.0 cm-1 |
| 3s2 3p3 5s1 3D2.0 | 277704.0 cm-1 |
| 3s2 3p3 5s1 3D3.0 | 277738.0 cm-1 |
| 3s2 3p3 4d1 3S1.0 | 277817.0 cm-1 |
| 3s2 3p3 4d1 1P1.0 | 277871.0 cm-1 |
| 3s2 3p3 5s1 1D2.0 | 278115.0 cm-1 |
| 3s2 3p3 4d1 3P2.0 | 278551.0 cm-1 |
| 3s2 3p3 4d1 3P1.0 | 278720.0 cm-1 |
| 3s2 3p3 4d1 3P0.0 | 278752.0 cm-1 |
| 3s2 3p3 4d1 1D2.0 | 279297.0 cm-1 |
| 3s2 3p3 4d1 1F3.0 | 284003.0 cm-1 |
| 3s2 3p3 4d1 3F4.0 | 287709.0 cm-1 |
| 3s2 3p3 4d1 3F3.0 | 287795.0 cm-1 |
| 3s2 3p3 4d1 3F2.0 | 287831.0 cm-1 |
| 3s2 3p3 4d1 3P0.0 | 288416.0 cm-1 |
| 3s2 3p3 4d1 3P1.0 | 288490.0 cm-1 |
| 3s2 3p3 4d1 3P2.0 | 288623.0 cm-1 |
| 3s2 3p3 4f1 3G3.0 | 289581.0 cm-1 |
| 3s2 3p3 4f1 3G4.0 | 289642.0 cm-1 |
| 3s2 3p3 4f1 3G5.0 | 289742.0 cm-1 |
| 3s2 3p3 4f1 3H4.0 | 289882.0 cm-1 |
| 3s2 3p3 4f1 3F3.0 | 289908.0 cm-1 |
| 3s2 3p3 4f1 3F4.0 | 289909.0 cm-1 |
| 3s2 3p3 4f1 3F2.0 | 289926.0 cm-1 |
| 3s2 3p3 4f1 3H5.0 | 289929.0 cm-1 |
| 3s2 3p3 4f1 3H6.0 | 289942.0 cm-1 |
| 3s2 3p3 4f1 1H5.0 | 290003.0 cm-1 |
| 3s2 3p3 4f1 3D3.0 | 290019.0 cm-1 |
| 3s2 3p3 4f1 1P1.0 | 290071.0 cm-1 |
| 3s2 3p3 4f1 3D2.0 | 290102.0 cm-1 |
| 3s2 3p3 4f1 3D1.0 | 290235.0 cm-1 |
| 3s2 3p3 4f1 1D2.0 | 290360.0 cm-1 |
| 3s2 3p3 4f1 3P2.0 | 290516.0 cm-1 |
| 3s2 3p3 4f1 3P1.0 | 290520.0 cm-1 |
| 3s2 3p3 4f1 3P0.0 | 290527.0 cm-1 |
| 3s2 3p3 4d1 3D2.0 | 290573.0 cm-1 |
| 3s2 3p3 4f1 1F3.0 | 290594.0 cm-1 |
| 3s2 3p3 4f1 1G4.0 | 290612.0 cm-1 |
| 3s2 3p3 4d1 3D3.0 | 290615.0 cm-1 |
| 3s2 3p3 4d1 3D1.0 | 290696.0 cm-1 |
| 3s2 3p3 4d1 1D2.0 | 291482.0 cm-1 |
| 3s2 3p3 5s1 3P0.0 | 293092.0 cm-1 |
| 3s2 3p3 5s1 3P1.0 | 293116.0 cm-1 |
| 3s2 3p3 5s1 3P2.0 | 293169.0 cm-1 |
| 3s2 3p3 5s1 1P1.0 | 293902.0 cm-1 |
| 3s2 3p3 4d1 1F3.0 | 294326.0 cm-1 |
| 3s2 3p3 4d1 1P1.0 | 302688.0 cm-1 |
| 3s2 3p3 4f1 3G5.0 | 305409.0 cm-1 |
| 3s2 3p3 4f1 3G4.0 | 305428.0 cm-1 |
| 3s2 3p3 4f1 3G3.0 | 305438.0 cm-1 |
| 3s2 3p3 4f1 3D1.0 | 305504.0 cm-1 |
| 3s2 3p3 4f1 1F3.0 | 305548.0 cm-1 |
| 3s2 3p3 4f1 3D2.0 | 305549.0 cm-1 |
| 3s2 3p3 4f1 3F2.0 | 305623.0 cm-1 |
| 3s2 3p3 4f1 3F4.0 | 305708.0 cm-1 |
| 3s2 3p3 4f1 3D3.0 | 305711.0 cm-1 |
| 3s2 3p3 4f1 3F3.0 | 305752.0 cm-1 |
| 3s2 3p3 4f1 1G4.0 | 305958.0 cm-1 |
| 3s2 3p3 4f1 1D2.0 | 306457.0 cm-1 |
| 3p6 1S0.0 | 336439.0 cm-1 |
| 3p5 3d1 3P0.0 | 491876.0 cm-1 |
| 3p5 3d1 3P1.0 | 492086.0 cm-1 |
| 3p5 3d1 3P2.0 | 492510.0 cm-1 |
| 3p5 3d1 3F4.0 | 497442.0 cm-1 |
| 3p5 3d1 3F3.0 | 497932.0 cm-1 |
| 3p5 3d1 3F2.0 | 498335.0 cm-1 |
| 3p5 3d1 3D3.0 | 508432.0 cm-1 |
| 3p5 3d1 1D2.0 | 508485.0 cm-1 |
| 3p5 3d1 3D1.0 | 508890.0 cm-1 |
| 3p5 3d1 3D2.0 | 508901.0 cm-1 |
| 3p5 3d1 1F3.0 | 509338.0 cm-1 |
| 3p5 3d1 1P1.0 | 567294.0 cm-1 |
------------------------------------------------------------------------------- Effective collision strengths were generated from a Breit-Pauli R-matrix calculation. The calculation involved 186 levels, arising from the 3s2 3p4, 3s 3p5, 3p6 and 3s2 3p3 nl, (3d<=nl<=5s) configurations. The atomic structure was generated from AUTOSTRUCTURE and optimized based on NIST energy levels and line strengths. In stage 3 of our R-matrix calculation the first 9 level energies were shifted to NIST values. The exchange calculation went from J=0.5 to 11.5, the non-exchange calculation went from J=12.5 to 37.5. The contributions from the higher partial waves were calculated for dipole transitions using the method described by Burgess (1970) and for non-dipole transitions using a a geometric series in L. Infinite energy points were calculated using AUTOSTRUCTURE and used in the effective collision strength calculation. The radiative rates for the dipole-allowed transitions were determined from our R-matrix calculation. The non-dipole radiative rates were calculated using AUTOSTRUCTURE. The calculation is reported in more detail in J M Munoz Burgos et al., Astron. & Astro., v500, p1253 (2009) DOI: 10.1051/0004-6361/200911743 Jorge Munoz February 27, 2009 -------------------------------------------------------------------------------