Table 1
Comparison between EBIT and HFR K-vacancy level energies.
Z | N | Levela | Energy (keV) | |||
HFRa | ASa | MCDFa | EBITb | |||
|
||||||
19 | 2 |
![]() |
3.5111 | 3.5121 | 3.5099 | 3.5106(1)c |
21 | 2 |
![]() |
4.3163 | 4.3180 | 4.3147 | 4.3156(2)c |
22 | 2 |
![]() |
4.7507 | 4.7527 | 4.7489 | 4.7498(2)c |
23 | 2 | 1s2s (2S) 3S1 | 5.1546 | 51568 | 5.1516 | 5.1539(3)d |
5.15382(14)e | ||||||
23 | 2 |
![]() |
5.1783 | 5.1820 | 5.1769 | 5.1803(2)d* |
5.18022(17)e* | ||||||
23 | 2 |
![]() |
5.1809 | 5.1835 | 5.1784 | 5.1803(2)d* |
5.18022(17)e* | ||||||
23 | 2 |
![]() |
5.1894 | 5.1917 | 5.1867 | 5.1889(2)d* |
5.18912(21)e* | ||||||
23 | 2 |
![]() |
5.2064 | 5.2088 | 5.2044 | 5.2053(2)c |
5.20510(14)e | ||||||
23 | 3 |
![]() |
5.1676 | 5.1700 | 5.1654 | 5.1676(6)d |
23 | 3 |
![]() |
5.1732 | 5.1763 | 5.1701 | 5.1725(2)d |
23 | 3 |
![]() |
5.1857 | 5.1895 | 5.1821 | 5.1851(4)d* |
23 | 3 |
![]() |
5.1877 | 5.1904 | 5.1844 | 5.1851(4)d* |
23 | 5 | 1s2s22p2 (1D) 2D3/2 | 5.1058 | 5.1041 | 5.1028 | 5.1061(4)d* |
23 | 5 | 1s2s22p2 (3P) 2P1/2 | 5.1076 | 5.1056 | 5.1038 | 5.1061(4)d* |
24 | 2 |
![]() |
5.6834 | 5.6863 | 5.6812 | 5.6824(4)c |
27 | 3 |
![]() |
7.1545 | 7.1595 | 7.1489 | 7.1518(7)f |
27 | 3 |
![]() |
7.1915 | 7.1950 | 7.1892 | 7.1906(3)f |
27 | 3 |
![]() |
7.2039 | 7.2095 | 7.1998 | 7.2032(5)f |
27 | 3 |
![]() |
7.2184 | 7.2233 | 7.2140 | 7.2172(3)f |
27 | 4 |
![]() |
7.1352 | 7.1325 | 7.1305 | 7.1347(9)f |
Notes.
This work. HFR, AS and MCDF stand respectively for HFR, AUTOSTRUCTURE and MCDF-EAL calculations.
Level energies are determined from the experimental wavelengths of resonance lines. Figures in parenthesis are errors affecting the last digits.
Beiersdorfer et al. (1989).
Beiersdorfer et al. (1991).
Chantler et al. (2000).
Smith et al. (1995).
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