Resolved Specific Ion Data Collections

Temperature Range
0.844 eV → 8444 eV


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  • Spontaneous Emission: Na+6(i) → Na+6(j) + hv
  • Electron Impact Excitation: Na+6(i) + e → Na+6(j) + e
2s2 2p1 2P0.5 0.0 cm-1
2s2 2p1 2P1.5 2134.6 cm-1
2s1 2p2 4P0.5 114995.0 cm-1
2s1 2p2 4P1.5 115728.0 cm-1
2s1 2p2 4P2.5 116798.0 cm-1
2s1 2p2 2D1.5 205412.0 cm-1
2s1 2p2 2D2.5 205448.0 cm-1
2s1 2p2 2S0.5 264400.0 cm-1
2s1 2p2 2P0.5 283868.0 cm-1
2s1 2p2 2P1.5 285189.0 cm-1
2p3 4S1.5 367308.0 cm-1
2p3 2D1.5 412310.0 cm-1
2p3 2D2.5 412395.0 cm-1
2p3 2P0.5 465017.0 cm-1
2p3 2P1.5 465111.0 cm-1
2s2 3s1 2S0.5 948957.0 cm-1
2s2 3p1 2P0.5 1005910.0 cm-1
2s2 3p1 2P1.5 1006470.0 cm-1
2s2 3d1 2D1.5 1060060.0 cm-1
2s2 3d1 2D2.5 1060210.0 cm-1
2s1 2p1 3s1 4P0.5 1075910.0 cm-1
2s1 2p1 3s1 4P1.5 1076640.0 cm-1
2s1 2p1 3s1 4P2.5 1077890.0 cm-1
2s1 2p1 3s1 2P0.5 1104940.0 cm-1
2s1 2p1 3s1 2P1.5 1106350.0 cm-1
2s1 2p1 3p1 2P0.5 1125660.0 cm-1
2s1 2p1 3p1 2P1.5 1126310.0 cm-1
2s1 2p1 3p1 4D0.5 1128130.0 cm-1
2s1 2p1 3p1 4D1.5 1128500.0 cm-1
2s1 2p1 3p1 4D2.5 1129180.0 cm-1
2s1 2p1 3p1 4D3.5 1130270.0 cm-1
2s1 2p1 3p1 4S1.5 1139460.0 cm-1
2s1 2p1 3p1 4P0.5 1146120.0 cm-1
2s1 2p1 3p1 4P1.5 1146670.0 cm-1
2s1 2p1 3p1 4P2.5 1147410.0 cm-1
2s1 2p1 3p1 2D1.5 1155530.0 cm-1
2s1 2p1 3p1 2D2.5 1156810.0 cm-1
2s1 2p1 3p1 2S0.5 1174040.0 cm-1
2s1 2p1 3d1 4F1.5 1175760.0 cm-1
2s1 2p1 3d1 4F2.5 1176180.0 cm-1
2s1 2p1 3d1 4F3.5 1176780.0 cm-1
2s1 2p1 3d1 4F4.5 1177580.0 cm-1
2s1 2p1 3d1 4D0.5 1188740.0 cm-1
2s1 2p1 3d1 4D1.5 1188850.0 cm-1
2s1 2p1 3d1 4D2.5 1189070.0 cm-1
2s1 2p1 3d1 4D3.5 1189520.0 cm-1
2s1 2p1 3d1 2D1.5 1191590.0 cm-1
2s1 2p1 3d1 2D2.5 1191770.0 cm-1
2s1 2p1 3d1 4P2.5 1194150.0 cm-1
2s1 2p1 3d1 4P1.5 1194530.0 cm-1
2s1 2p1 3d1 4P0.5 1194780.0 cm-1
2s1 2p1 3s1 2P0.5 1205000.0 cm-1
2s1 2p1 3s1 2P1.5 1205030.0 cm-1
2s1 2p1 3d1 2F2.5 1217480.0 cm-1
2s1 2p1 3d1 2F3.5 1218730.0 cm-1
2s1 2p1 3d1 2P1.5 1223730.0 cm-1
2s1 2p1 3d1 2P0.5 1224430.0 cm-1
2s1 2p1 3p1 2P0.5 1260870.0 cm-1
2s1 2p1 3p1 2P1.5 1261210.0 cm-1
2s1 2p1 3p1 2D1.5 1261680.0 cm-1
2s1 2p1 3p1 2D2.5 1261770.0 cm-1
2s1 2p1 3p1 2S0.5 1269010.0 cm-1
2p2 3s1 4P0.5 1292580.0 cm-1
2p2 3s1 4P1.5 1293330.0 cm-1
2p2 3s1 4P2.5 1294550.0 cm-1
2s2 4s1 2S0.5 1304360.0 cm-1
2s1 2p1 3d1 2F3.5 1305490.0 cm-1
2s1 2p1 3d1 2F2.5 1305500.0 cm-1
2s2 4p1 2P0.5 1315060.0 cm-1
2s2 4p1 2P1.5 1315290.0 cm-1
2s1 2p1 3d1 2D1.5 1316980.0 cm-1
2s1 2p1 3d1 2D2.5 1317200.0 cm-1
2p2 3s1 2P0.5 1322980.0 cm-1
2p2 3s1 2P1.5 1324360.0 cm-1
2p2 3p1 2S0.5 1330060.0 cm-1
2s1 2p1 3d1 2P0.5 1333750.0 cm-1
2s1 2p1 3d1 2P1.5 1333980.0 cm-1
2s2 4d1 2D1.5 1338890.0 cm-1
2s2 4d1 2D2.5 1338950.0 cm-1
2p2 3p1 4D0.5 1339530.0 cm-1
2p2 3p1 4D1.5 1339990.0 cm-1
2p2 3p1 4D2.5 1340750.0 cm-1
2p2 3s1 2D1.5 1340790.0 cm-1
2p2 3s1 2D2.5 1340820.0 cm-1
2p2 3p1 4D3.5 1341820.0 cm-1
2p2 3p1 4P0.5 1346630.0 cm-1
2p2 3p1 4P1.5 1347040.0 cm-1
2p2 3p1 4P2.5 1347760.0 cm-1
2s2 4f1 2F2.5 1352500.0 cm-1
2s2 4f1 2F3.5 1352540.0 cm-1
2p2 3p1 2D1.5 1355550.0 cm-1
2p2 3p1 2D2.5 1356880.0 cm-1
2p2 3p1 2P1.5 1368670.0 cm-1
2p2 3p1 2P0.5 1368770.0 cm-1
2p2 3p1 4S1.5 1374230.0 cm-1
2p2 3d1 4F1.5 1381200.0 cm-1
2p2 3d1 4F2.5 1381610.0 cm-1
2p2 3d1 4F3.5 1382200.0 cm-1
2p2 3d1 4F4.5 1382980.0 cm-1
2p2 3p1 2F2.5 1389930.0 cm-1
2p2 3p1 2F3.5 1390370.0 cm-1
2p2 3d1 4D0.5 1391410.0 cm-1
2p2 3d1 4D1.5 1391540.0 cm-1
2p2 3d1 4D2.5 1391880.0 cm-1
2p2 3d1 4D3.5 1392180.0 cm-1
2p2 3d1 2P1.5 1393290.0 cm-1
2p2 3d1 2P0.5 1394490.0 cm-1
2p2 3d1 2F2.5 1396890.0 cm-1
2p2 3d1 2F3.5 1398290.0 cm-1
2p2 3d1 4P2.5 1405970.0 cm-1
2p2 3d1 4P1.5 1406460.0 cm-1
2p2 3d1 4P0.5 1406740.0 cm-1
2p2 3p1 2D2.5 1410150.0 cm-1
2p2 3p1 2D1.5 1410220.0 cm-1
2p2 3p1 2P0.5 1418020.0 cm-1
2p2 3p1 2P1.5 1418920.0 cm-1
2p2 3s1 2S0.5 1422300.0 cm-1
2s1 2p1 4s1 4P0.5 1426370.0 cm-1
2s1 2p1 4s1 4P1.5 1427070.0 cm-1
2p2 3d1 2D1.5 1427140.0 cm-1
2p2 3d1 2D2.5 1427310.0 cm-1
2s1 2p1 4s1 4P2.5 1428250.0 cm-1
2p2 3d1 2G3.5 1429910.0 cm-1
2p2 3d1 2G4.5 1430060.0 cm-1
2s1 2p1 4s1 2P0.5 1441530.0 cm-1
2p2 3d1 2F3.5 1442190.0 cm-1
2p2 3d1 2F2.5 1442250.0 cm-1
2s1 2p1 4s1 2P1.5 1442790.0 cm-1
2p2 3d1 2D1.5 1442920.0 cm-1
2p2 3d1 2D2.5 1443540.0 cm-1
2s1 2p1 4p1 4D0.5 1446380.0 cm-1
2s1 2p1 4p1 4D1.5 1446790.0 cm-1
2s1 2p1 4p1 4D2.5 1447470.0 cm-1
2s1 2p1 4p1 4D3.5 1448430.0 cm-1
2s1 2p1 4p1 2P0.5 1450060.0 cm-1
2s1 2p1 4p1 4S1.5 1450100.0 cm-1
2s1 2p1 4p1 2P1.5 1451010.0 cm-1
2s1 2p1 4p1 4P0.5 1454120.0 cm-1
2s1 2p1 4p1 4P1.5 1454650.0 cm-1
2s1 2p1 4p1 4P2.5 1455190.0 cm-1
2p2 3d1 2P0.5 1458230.0 cm-1
2p2 3d1 2P1.5 1458740.0 cm-1
2s1 2p1 4p1 2D1.5 1461990.0 cm-1
2s1 2p1 4p1 2D2.5 1463100.0 cm-1
2s1 2p1 4d1 4F1.5 1463180.0 cm-1
2s1 2p1 4d1 4F2.5 1463560.0 cm-1
2p2 3d1 2S0.5 1464020.0 cm-1
2s1 2p1 4d1 4F3.5 1464130.0 cm-1
2s1 2p1 4d1 4F4.5 1464950.0 cm-1
2s1 2p1 4d1 4D0.5 1467930.0 cm-1
2s1 2p1 4d1 4D1.5 1467950.0 cm-1
2s1 2p1 4d1 4D2.5 1468010.0 cm-1
2s1 2p1 4d1 4D3.5 1468710.0 cm-1
2s1 2p1 4d1 4P2.5 1469720.0 cm-1
2s1 2p1 4d1 2D1.5 1469970.0 cm-1
2s1 2p1 4d1 4P1.5 1470300.0 cm-1
2s1 2p1 4d1 4P0.5 1470450.0 cm-1
2s1 2p1 4d1 2D2.5 1470540.0 cm-1
2s1 2p1 4p1 2S0.5 1472320.0 cm-1
2s1 2p1 4f1 4G2.5 1476700.0 cm-1
2s1 2p1 4f1 4G3.5 1476800.0 cm-1
2s1 2p1 4f1 4F4.5 1477200.0 cm-1
2s1 2p1 4f1 4F1.5 1477220.0 cm-1
2s1 2p1 4f1 4F2.5 1477590.0 cm-1
2s1 2p1 4f1 4F3.5 1477980.0 cm-1
2s1 2p1 4f1 4G4.5 1478490.0 cm-1
2s1 2p1 4f1 4G5.5 1478670.0 cm-1
2s1 2p1 4f1 2G3.5 1478810.0 cm-1
2s1 2p1 4d1 2F2.5 1479600.0 cm-1
2p2 3p1 2P0.5 1479790.0 cm-1
2p2 3p1 2P1.5 1479930.0 cm-1
2s1 2p1 4f1 2G4.5 1479990.0 cm-1
2s1 2p1 4f1 4D3.5 1480420.0 cm-1
2s1 2p1 4d1 2F3.5 1480710.0 cm-1
2s1 2p1 4f1 4D2.5 1480940.0 cm-1
2s1 2p1 4f1 4D1.5 1481270.0 cm-1
2s1 2p1 4f1 4D0.5 1481450.0 cm-1
2s1 2p1 4f1 2F2.5 1481530.0 cm-1
2s1 2p1 4d1 2P1.5 1481720.0 cm-1
2s1 2p1 4f1 2F3.5 1482160.0 cm-1
2s1 2p1 4d1 2P0.5 1482350.0 cm-1
2s1 2p1 4f1 2D2.5 1483970.0 cm-1
2s1 2p1 4f1 2D1.5 1484400.0 cm-1
2p2 3d1 2D2.5 1520320.0 cm-1
2p2 3d1 2D1.5 1520550.0 cm-1
2s1 2p1 4s1 2P0.5 1553560.0 cm-1
2s1 2p1 4s1 2P1.5 1553610.0 cm-1
2s1 2p1 4p1 2D1.5 1574400.0 cm-1
2s1 2p1 4p1 2D2.5 1574550.0 cm-1
2s1 2p1 4p1 2P0.5 1576230.0 cm-1
2s1 2p1 4p1 2P1.5 1576440.0 cm-1
2s1 2p1 4p1 2S0.5 1580950.0 cm-1
2s1 2p1 4d1 2F3.5 1591740.0 cm-1
2s1 2p1 4d1 2F2.5 1591750.0 cm-1
2s1 2p1 4d1 2D1.5 1592810.0 cm-1
2s1 2p1 4d1 2D2.5 1592890.0 cm-1
2s1 2p1 4d1 2P0.5 1597340.0 cm-1
2s1 2p1 4d1 2P1.5 1597410.0 cm-1
2s1 2p1 4f1 2F2.5 1599810.0 cm-1
2s1 2p1 4f1 2F3.5 1599830.0 cm-1
2s1 2p1 4f1 2G3.5 1603590.0 cm-1
2s1 2p1 4f1 2G4.5 1603610.0 cm-1
2s1 2p1 4f1 2D1.5 1607870.0 cm-1
2s1 2p1 4f1 2D2.5 1607880.0 cm-1

        Result of ICFT R-matrix calculation

 Calculation automated by offline ADAS code ADAS8#3

     Summary Information

 *  Ionisation energy taken from ADAS adf00 files

 *  Energy levels calculated by AUTOSTRUCTURE

 *  Radiative rates calculated by AUTOSTRUCTURE

 *  Effective collision strengths calculated by ICFT
    R-matrix calculation using target structure from

     Calculation details

 The following scaling parameters on bound orbitals were used:

         1S = 1.39840
         2S = 1.24440
         2P = 1.17205
         3S = 1.62817
         3P = 1.35159
         3D = 1.45478
         4S = 1.27730
         4P = 1.54966
         4D = 1.50999
         4F = 0.58666

 An exchange calculation was performed up to J=12
 A non-exchange calculation was then performed up to J=40
 Followed by a top-up calculation to J -> infinity.

 40 continuum basis orbitals were used, giving a smallest maximum
 basis-orbital energy of 169.4227 Rydbergs (2305.165256 eV)

 A fine energy mesh of 0.000005 Z**2 Rydbergs (0.00244908 eV) was used
 between the first and last thresholds for the excitation calculation.

 A coarse energy mesh of 0.001000 Z**2 Rydbergs (0.489816 eV) was used
 from the last threshold up to 1.343157 Z**2 Rydbergs (657.9 eV) in the
 excitation calculation.

 A coarse energy mesh of 0.001000 Z**2 Rydbergs (0.489816 eV) was used
 from first threshold up to 1.343157 Z**2 Rydbergs (657.9 eV) in the
 non-exchange calculation.

 Dipole and Born limits were used from the last calculated energy points
 up to infinite energy to complete the effective collision strengths

      G Y Liang, N R Badnell and G Zhao
      A&A 547, A87 (2012)
      DOI: 10.1051/0004-6361/201220277

 Produced by: Guiyun Liang
 Date:        22/05/12


  • Guiyun Liang
  • Nigel Badnell
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