Technetium energy level diagram
Energy levels and transitions of neutral technetium (Tc I): the 70 strongest classified lines below 2 µm from the NIST Atomic Spectra Database and the 37 levels they connect, each line with its vacuum wavelength, frequency and, for 70 of them, the reduced dipole matrix element derived from the NIST transition rate. Measured lifetimes, transition rates, hyperfine constants and isotope shifts from the literature are included, each with its citation.
Hover a line or a level to isolate it, click to keep it selected. Scroll to zoom, drag to move.

Download: diagram (PDF) diagram (SVG) transitions (CSV) levels (CSV) source code
Key transitions of technetium
| Transition | λ vac (nm) | λ air (nm) | ν (THz) | |⟨J‖er‖J′⟩| (ea₀) | A (s⁻¹) | Γ/2π up. (MHz) | branch (%) | Use |
|---|---|---|---|---|---|---|---|---|
| 4d55s2 6S5/2 – 4d55s5p 6P°3/2 | 423.9372 | 423.8178 | 707.1624 | 2.391 | 3.800e+07 | 5.682 | 100 | first step of the three-step Ti:sapphire resonance-ioniza… |
| 4d55s2 6S5/2 – 4d55s5p 6P°5/2 | 426.3445 | 426.2245 | 703.1695 | 3.030 | 4.000e+07 | 5.889 | 100 | first step of the three-step Ti:sapphire resonance-ioniza… |
| 4d55s2 6S5/2 – 4d55s5p 6P°7/2 | 429.8243 | 429.7034 | 697.4768 | 3.629 | 4.200e+07 | 6.239 | 100 | first step of the three-step Ti:sapphire resonance-ioniza… |
λ, ν from NIST level energies unless a measured frequency for this isotope is available. A: measured value or NIST. Γ/2π: natural linewidth of the upper level, 1/(2πτ).
99Tc hyperfine structure (I = 9/2)
| Level | A (MHz) | B (MHz) | Shift of each F level from the centre of gravity (MHz) |
|---|---|---|---|
| 4d55s2 6S5/2 | -107.34(8) | 0.3(20) | F=2: +1476.06 F=3: +1153.95 F=4: +724.51 F=5: +187.76 F=6: -456.26 F=7: -1207.50 |
| 4d55s5p 6P°7/2 | 799.99(26) | -44(4) | F=1: -15419.93 F=2: -13813.68 F=3: -11405.61 F=4: -8197.28 F=5: -4190.80 F=6: +611.23 F=7: +6205.67 F=8: +12588.87 |
| 4d55s5p 6P°5/2 | 894.08(28) | 57(4) | F=2: -12267.29 F=3: -9602.27 F=4: -6042.22 F=5: -1581.38 F=6: +3787.40 F=7: +10072.75 |
| 4d55s5p 6P°3/2 | 1183.27(27) | -13(3) | F=3: -9767.75 F=4: -5026.27 F=5: +892.70 F=6: +7983.92 |
Measured A, B constants; sources in the data file.
Isotope shifts
| Transition | λ vac (nm) | Isotopes | Shift (MHz) |
|---|---|---|---|
| 4d55s2 6S5/2 – 4d55s5p 6P°3/2 | 423.937 | 97-99 | 308(14) |
| 4d55s2 6S5/2 – 4d55s5p 6P°3/2 | 423.937 | 98-99 | 324(14) |
| 4d55s2 6S5/2 – 4d55s5p 6P°5/2 | 426.344 | 97-99 | 313(14) |
| 4d55s2 6S5/2 – 4d55s5p 6P°5/2 | 426.344 | 98-99 | 327(14) |
| 4d55s2 6S5/2 – 4d55s5p 6P°7/2 | 429.824 | 97-99 | 347(14) |
| 4d55s2 6S5/2 – 4d55s5p 6P°7/2 | 429.824 | 98-99 | 369(14) |
Shift = ν(first isotope) − ν(second isotope).
Closed and nearly closed transitions of technetium
| Transition | λ vacuum (nm) | Lower level | A (s⁻¹) | Leak per scattered photon | Photons before a leak | Where the leak goes |
|---|---|---|---|---|---|---|
| 4d65s 6D9/2 → 4d65p 6F°11/2 | 363.7104 | metastable | 1.570e+08 NIST | 1.45 × 10−4 from semi-empirical calc. | 6,900 | 4d7 4F9/2 ≈ 5.68 × 10−5 (long-lived); 4d55s2 4G11/2 ≈ 5.22 × 10−5 (long-lived); 4d65s 4F9/2 ≈ 2.26 × 10−5; 17 weaker lines |
| 4d55s2 6S5/2 → 4d55s5p 8P°5/2 | 608.6905 | ground | 9.665e+04 semi-empirical | ≥ 0.286 % from semi-empirical calc. | ≤ 350 | 4d65s 6D7/2 ≈ 0.237 % (long-lived); 4d65s 6D3/2 ≈ 2.68 × 10−4 (long-lived); 4d65s 6D5/2 ≈ 1.7 × 10−4 (long-lived); 7 weaker lines; 3 more possible paths without a listed rate |
| 4d65s 6D9/2 → 4d55s5p 6F°11/2 | 272.7499 | metastable | 2.379e+08 semi-empirical | 0.488 % from semi-empirical calc. | 205 | 4d7 4F9/2 ≈ 0.191 % (long-lived); 4d65s 4H13/2 ≈ 0.128 % (long-lived); 4d65s 4G11/2 ≈ 5.79 × 10−4; 17 weaker lines |
| 4d55s2 6S5/2 → 4d55s5p 8P°7/2 | 592.6098 | ground | 1.873e+05 semi-empirical | ≥ 0.534 % from semi-empirical calc. | ≤ 187 | 4d65s 6D7/2 ≈ 0.276 % (long-lived); 4d65s 6D9/2 ≈ 0.187 % (long-lived); 4d65s 6D5/2 ≈ 7.1 × 10−4 (long-lived); 8 weaker lines; 1 more possible path without a listed rate |
| 4d55s2 6S5/2 → 4d55s5p 6P°7/2 | 429.8243 | ground | 4.200e+07 NIST | 2.29 % from semi-empirical calc. | 44 | 4d65s 6D7/2 ≈ 1.01 % (long-lived); 4d65s 6D9/2 ≈ 0.974 % (long-lived); 4d65s 6D5/2 ≈ 0.346 % (long-lived); 26 weaker lines |
| 4d55s2 6S5/2 → 4d55s5p 6P°5/2 | 426.3445 | ground | 4.000e+07 NIST | 3.36 % from semi-empirical calc. | 30 | 4d65s 6D5/2 ≈ 1.48 % (long-lived); 4d65s 6D7/2 ≈ 1.24 % (long-lived); 4d65s 6D3/2 ≈ 0.741 % (long-lived); 27 weaker lines |
| 4d55s2 6S5/2 → 4d55s5p 6P°3/2 | 423.9372 | ground | 3.800e+07 NIST | 4.61 % from semi-empirical calc. | 22 | 4d65s 6D3/2 ≈ 2.01 % (long-lived); 4d65s 6D1/2 ≈ 1.68 % (long-lived); 4d65s 6D5/2 ≈ 1.14 % (long-lived); 21 weaker lines |
| 4d65s 6D9/2 → 4d65p 6D°9/2 | 403.2762 | metastable | 1.010e+08 NIST | ≥ 7.37 % from semi-empirical calc. | ≤ 14 | 4d65s 6D7/2 ≈ 7.47 % (long-lived); 4d65s 4D7/2 ≈ 0.461 % (long-lived); 4d7 4F9/2 ≈ 1.17 × 10−4 (long-lived); 24 weaker lines; 1 more possible path without a listed rate |
A transition is closed when its upper level can decay only to the level it was excited from, so the atom keeps scattering photons. “closed”: among the levels NIST lists, no other level below the upper level has the opposite parity and |ΔJ| ≤ 1, so no other electric-dipole decay exists. Otherwise the leak is the sum of the branching ratios of the other decay lines of the upper level (or 1 − branching ratio where that of the line itself has been measured), and the number of photons is 1 / leak. “≥” and “≤”: at least one possible decay path has no listed rate, so the leak is a lower limit. These numbers are derived from the branching ratios, lifetimes and rates of this page, not measured as such; the tag names the weakest of the inputs, * marks theory and ≈ a model or semi-empirical calculation. Listed: lines that start on the ground level or on a metastable level and leak at most 10 %, unless more than three possible decay paths have no listed rate. Fine-structure levels only: hyperfine and Zeeman dark states and forbidden decays without a listed rate are not considered. Select a line in the diagram for the full list of its leak channels.
Listed Tc transitions below 2 µm
| Lower level | Upper level | λ vacuum (nm) | λ air (nm) | ν (THz) | Type | |⟨J‖er‖J′⟩| (ea₀) | A (s⁻¹) | Branching (%) | Source of matrix element / A |
|---|---|---|---|---|---|---|---|---|---|
| 4d55s2 6S5/2 | 4d55s5p 6D°3/2 | 260.9631 | 260.8851 | 1148.7927 | E1 | 3.686 semi-empirical | 3.872e+08 semi-empirical | 78.1 | Kurucz, R. L., Can. J. Phys. 89, 417 (2011); semi-empirical line list gf4300.pos of 2017-… |
| 4d55s2 6S5/2 | 4d55s5p 6P°7/2 | 261.5013 | 261.4232 | 1146.4282 | E1 | 5.476 semi-empirical | 4.247e+08 semi-empirical | 86.3 | Kurucz, R. L., Can. J. Phys. 89, 417 (2011); semi-empirical line list gf4300.pos of 2017-… |
| 4d55s2 6S5/2 | 4d65p 6P°5/2 | 261.6654 | 261.5873 | 1145.7093 | E1 | 4.494 semi-empirical | 3.806e+08 semi-empirical | 80.3 | Kurucz, R. L., Can. J. Phys. 89, 417 (2011); semi-empirical line list gf4300.pos of 2017-… |
| 4d65s 6D9/2 | 4d55s5p 6F°11/2 | 272.7499 | 272.6691 | 1099.1480 | E1 | 5.347 semi-empirical | 2.379e+08 semi-empirical | 99.5 | Kurucz, R. L., Can. J. Phys. 89, 417 (2011); semi-empirical line list gf4300.pos of 2017-… |
| 4d65s 6D9/2 | 4d55s5p 6D°9/2 | 273.1336 | 273.0528 | 1097.6037 | E1 | 2.612 semi-empirical | 6.783e+07 semi-empirical | 36.1 | Kurucz, R. L., Can. J. Phys. 89, 417 (2011); semi-empirical line list gf4300.pos of 2017-… |
| 4d65s 6D7/2 | 4d55s5p 6D°9/2 | 278.2872 | 278.2051 | 1077.2772 | E1 | 3.556 semi-empirical | 1.189e+08 semi-empirical | 63.2 | Kurucz, R. L., Can. J. Phys. 89, 417 (2011); semi-empirical line list gf4300.pos of 2017-… |
| 4d65s 6D9/2 | 4d55s5p 6P°7/2 | 280.3646 | 280.2820 | 1069.2949 | E1 | 2.019 semi-empirical | 4.684e+07 semi-empirical | 9.52 | Kurucz, R. L., Can. J. Phys. 89, 417 (2011); semi-empirical line list gf4300.pos of 2017-… |
| 4d65s 6D7/2 | 4d65p 6P°5/2 | 285.9934 | 285.9094 | 1048.2495 | E1 | 1.807 semi-empirical | 4.713e+07 semi-empirical | 9.94 | Kurucz, R. L., Can. J. Phys. 89, 417 (2011); semi-empirical line list gf4300.pos of 2017-… |
| 4d65s 6D5/2 | 4d55s5p 6D°3/2 | 288.8582 | 288.7735 | 1037.8533 | E1 | 1.219 semi-empirical | 3.124e+07 semi-empirical | 6.3 | Kurucz, R. L., Can. J. Phys. 89, 417 (2011); semi-empirical line list gf4300.pos of 2017-… |
| 4d65s 6D5/2 | 4d65p 6P°5/2 | 289.7189 | 289.6341 | 1034.7699 | E1 | 1.364 semi-empirical | 2.582e+07 semi-empirical | 5.45 | Kurucz, R. L., Can. J. Phys. 89, 417 (2011); semi-empirical line list gf4300.pos of 2017-… |
| 4d55s2 6S5/2 | 4d55s5p 4P°5/2 | 289.7217 | 289.6368 | 1034.7601 | E1 (intercombination) | 0.585 semi-empirical | 4.754e+06 semi-empirical | 3.17 | Kurucz, R. L., Can. J. Phys. 89, 417 (2011); semi-empirical line list gf4300.pos of 2017-… |
| 4d65s 6D3/2 | 4d55s5p 6D°3/2 | 291.4005 | 291.3152 | 1028.7987 | E1 | 1.409 semi-empirical | 4.065e+07 semi-empirical | 8.2 | Kurucz, R. L., Can. J. Phys. 89, 417 (2011); semi-empirical line list gf4300.pos of 2017-… |
| 4d65s 6D1/2 | 4d55s5p 6D°3/2 | 292.9042 | 292.8186 | 1023.5169 | E1 | 1.277 semi-empirical | 3.286e+07 semi-empirical | 6.62 | Kurucz, R. L., Can. J. Phys. 89, 417 (2011); semi-empirical line list gf4300.pos of 2017-… |
| 4d55s2 6S5/2 | 4d65p 4P°3/2 | 310.0000 | 309.9101 | 967.0723 | E1 (intercombination) | 0.674 semi-empirical | 7.715e+06 semi-empirical | 16.5 | Kurucz, R. L., Can. J. Phys. 89, 417 (2011); semi-empirical line list gf4300.pos of 2017-… |
| 4d55s2 6S5/2 | 4d65p 4F°5/2 | 312.3554 | 312.2649 | 959.7799 | E1 (intercombination) | 0.252 semi-empirical | 7.010e+05 semi-empirical | 1.03 | Kurucz, R. L., Can. J. Phys. 89, 417 (2011); semi-empirical line list gf4300.pos of 2017-… |
| 4d55s2 6S5/2 | 4d65p 4P°5/2 | 313.2144 | 313.1237 | 957.1477 | E1 (intercombination) | 1.051 semi-empirical | 1.214e+07 semi-empirical | 13.8 | Kurucz, R. L., Can. J. Phys. 89, 417 (2011); semi-empirical line list gf4300.pos of 2017-… |
| 4d55s2 6S5/2 | 4d55s5p 6P°3/2 | 317.4207 | 317.3289 | 944.4641 | E1 | 2.330 NIST | 8.600e+07 NIST | 51.2 | NIST ASD (accuracy n/a) |
| 4d55s2 6S5/2 | 4d65p 6P°7/2 | 318.3289 | 318.2369 | 941.7695 | E1 | 2.229 NIST | 3.900e+07 NIST | 17.5 | NIST ASD (accuracy n/a) |
| 4d55s2 6S5/2 | 4d55s5p 6P°5/2 | 318.4030 | 318.3109 | 941.5504 | E1 | 2.314 NIST | 5.600e+07 NIST | 40.9 | NIST ASD (accuracy n/a) |
| 4d65s 6D9/2 | 4d65p 6P°7/2 | 346.7267 | 346.6274 | 864.6362 | E1 | 4.481 NIST | 1.220e+08 NIST | 54.7 | NIST ASD (accuracy n/a) |
| 4d65s 6D7/2 | 4d65p 4F°5/2 | 347.6580 | 347.5585 | 862.3200 | E1 (intercombination) | 0.585 semi-empirical | 2.746e+06 semi-empirical | 4.05 | Kurucz, R. L., Can. J. Phys. 89, 417 (2011); semi-empirical line list gf4300.pos of 2017-… |
| 4d65s 6D7/2 | 4d65p 4P°5/2 | 348.7225 | 348.6227 | 859.6879 | E1 (intercombination) | 1.834 semi-empirical | 2.679e+07 semi-empirical | 30.5 | Kurucz, R. L., Can. J. Phys. 89, 417 (2011); semi-empirical line list gf4300.pos of 2017-… |
| 4d65s 6D5/2 | 4d65p 4P°3/2 | 350.1705 | 350.0703 | 856.1329 | E1 (intercombination) | 0.992 semi-empirical | 1.160e+07 semi-empirical | 24.8 | Kurucz, R. L., Can. J. Phys. 89, 417 (2011); semi-empirical line list gf4300.pos of 2017-… |
| 4d65s 6D9/2 | 4d65p 4F°9/2 | 350.3708 | 350.2706 | 855.6434 | E1 (intercombination) | 1.171 semi-empirical | 6.458e+06 semi-empirical | 8.29 | Kurucz, R. L., Can. J. Phys. 89, 417 (2011); semi-empirical line list gf4300.pos of 2017-… |
| 4d65s 6D7/2 | 4d65p 4F°7/2 | 352.6828 | 352.5820 | 850.0342 | E1 (intercombination) | 0.777 semi-empirical | 3.486e+06 semi-empirical | 4.79 | Kurucz, R. L., Can. J. Phys. 89, 417 (2011); semi-empirical line list gf4300.pos of 2017-… |
| 4d65s 6D3/2 | 4d65p 4F°3/2 | 353.9688 | 353.8676 | 846.9461 | E1 (intercombination) | 0.313 semi-empirical | 1.122e+06 semi-empirical | 1.75 | Kurucz, R. L., Can. J. Phys. 89, 417 (2011); semi-empirical line list gf4300.pos of 2017-… |
| 4d65s 6D5/2 | 4d65p 4P°5/2 | 354.2774 | 354.1762 | 846.2083 | E1 (intercombination) | 1.610 semi-empirical | 1.969e+07 semi-empirical | 22.4 | Kurucz, R. L., Can. J. Phys. 89, 417 (2011); semi-empirical line list gf4300.pos of 2017-… |
| 4d65s 6D7/2 | 4d65p 6P°7/2 | 355.0740 | 354.9726 | 844.3097 | E1 | 2.988 semi-empirical | 5.051e+07 semi-empirical | 22.7 | Kurucz, R. L., Can. J. Phys. 89, 417 (2011); semi-empirical line list gf4300.pos of 2017-… |
| 4d65s 6D7/2 | 4d55s5p 6P°5/2 | 355.1662 | 355.0648 | 844.0906 | E1 | 2.317 semi-empirical | 4.047e+07 semi-empirical | 29.5 | Kurucz, R. L., Can. J. Phys. 89, 417 (2011); semi-empirical line list gf4300.pos of 2017-… |
| 4d65s 6D1/2 | 4d65p 4P°3/2 | 356.1341 | 356.0324 | 841.7965 | E1 (intercombination) | 0.745 semi-empirical | 6.221e+06 semi-empirical | 13.3 | Kurucz, R. L., Can. J. Phys. 89, 417 (2011); semi-empirical line list gf4300.pos of 2017-… |
| 4d65s 6D3/2 | 4d65p 4F°5/2 | 356.9868 | 356.8849 | 839.7858 | E1 (intercombination) | 0.769 semi-empirical | 4.392e+06 semi-empirical | 6.48 | Kurucz, R. L., Can. J. Phys. 89, 417 (2011); semi-empirical line list gf4300.pos of 2017-… |
| 4d65s 6D3/2 | 4d65p 4P°5/2 | 358.1092 | 358.0070 | 837.1536 | E1 (intercombination) | 0.990 semi-empirical | 7.210e+06 semi-empirical | 8.2 | Kurucz, R. L., Can. J. Phys. 89, 417 (2011); semi-empirical line list gf4300.pos of 2017-… |
| 4d65s 6D5/2 | 4d65p 4F°7/2 | 358.3657 | 358.2634 | 836.5547 | E1 (intercombination) | 1.151 semi-empirical | 7.285e+06 semi-empirical | 10 | Kurucz, R. L., Can. J. Phys. 89, 417 (2011); semi-empirical line list gf4300.pos of 2017-… |
| 4d65s 6D7/2 | 4d65p 4F°9/2 | 358.8967 | 358.7943 | 835.3168 | E1 (intercombination) | 2.235 semi-empirical | 2.189e+07 semi-empirical | 28.1 | Kurucz, R. L., Can. J. Phys. 89, 417 (2011); semi-empirical line list gf4300.pos of 2017-… |
| 4d65s 6D5/2 | 4d55s5p 6P°3/2 | 359.6684 | 359.5658 | 833.5247 | E1 | 1.379 semi-empirical | 2.071e+07 semi-empirical | 12.3 | Kurucz, R. L., Can. J. Phys. 89, 417 (2011); semi-empirical line list gf4300.pos of 2017-… |
| 4d65s 6D5/2 | 4d65p 6P°7/2 | 360.8348 | 360.7319 | 830.8301 | E1 | 1.529 semi-empirical | 1.260e+07 semi-empirical | 5.65 | Kurucz, R. L., Can. J. Phys. 89, 417 (2011); semi-empirical line list gf4300.pos of 2017-… |
| 4d65s 6D5/2 | 4d55s5p 6P°5/2 | 360.9300 | 360.8271 | 830.6110 | E1 | 2.515 semi-empirical | 4.541e+07 semi-empirical | 33.1 | Kurucz, R. L., Can. J. Phys. 89, 417 (2011); semi-empirical line list gf4300.pos of 2017-… |
| 4d65s 6D9/2 | 4d65p 6F°9/2 | 362.8398 | 362.7364 | 826.2391 | E1 | 0.945 semi-empirical | 3.791e+06 semi-empirical | 3.88 | Kurucz, R. L., Can. J. Phys. 89, 417 (2011); semi-empirical line list gf4300.pos of 2017-… |
| 4d65s 6D3/2 | 4d55s5p 6P°3/2 | 363.6184 | 363.5148 | 824.4700 | E1 | 2.175 semi-empirical | 4.986e+07 semi-empirical | 29.7 | Kurucz, R. L., Can. J. Phys. 89, 417 (2011); semi-empirical line list gf4300.pos of 2017-… |
| 4d65s 6D9/2 | 4d65p 6F°11/2 | 363.7104 | 363.6068 | 824.2614 | E1 | 6.689 NIST | 1.570e+08 NIST | 100 | NIST ASD (accuracy n/a) |
| 4d65s 6D3/2 | 4d55s5p 6P°5/2 | 364.9080 | 364.8040 | 821.5563 | E1 | 1.616 semi-empirical | 1.814e+07 semi-empirical | 13.2 | Kurucz, R. L., Can. J. Phys. 89, 417 (2011); semi-empirical line list gf4300.pos of 2017-… |
| 4d65s 6D1/2 | 4d55s5p 6P°3/2 | 365.9628 | 365.8586 | 819.1883 | E1 | 2.056 semi-empirical | 4.367e+07 semi-empirical | 26 | Kurucz, R. L., Can. J. Phys. 89, 417 (2011); semi-empirical line list gf4300.pos of 2017-… |
| 4d65s 6D7/2 | 4d65p 6F°7/2 | 368.5800 | 368.4751 | 813.3714 | E1 | 2.082 semi-empirical | 2.193e+07 semi-empirical | 21.9 | Kurucz, R. L., Can. J. Phys. 89, 417 (2011); semi-empirical line list gf4300.pos of 2017-… |
| 4d65s 6D5/2 | 4d65p 6F°3/2 | 371.3320 | 371.2264 | 807.3435 | E1 | 0.769 semi-empirical | 5.855e+06 semi-empirical | 5.91 | Kurucz, R. L., Can. J. Phys. 89, 417 (2011); semi-empirical line list gf4300.pos of 2017-… |
| 4d65s 6D7/2 | 4d65p 6F°9/2 | 371.9913 | 371.8855 | 805.9126 | E1 | 5.165 NIST | 1.050e+08 NIST | 100 | NIST ASD (accuracy n/a) |
| 4d65s 6D5/2 | 4d65p 6F°5/2 | 372.7404 | 372.6345 | 804.2928 | E1 | 2.446 semi-empirical | 3.901e+07 semi-empirical | 39.2 | Kurucz, R. L., Can. J. Phys. 89, 417 (2011); semi-empirical line list gf4300.pos of 2017-… |
| 4d65s 6D3/2 | 4d65p 6F°1/2 | 374.7206 | 374.6141 | 800.0426 | E1 | 0.947 semi-empirical | 1.725e+07 semi-empirical | 17.4 | Kurucz, R. L., Can. J. Phys. 89, 417 (2011); semi-empirical line list gf4300.pos of 2017-… |
| 4d65s 6D5/2 | 4d65p 6F°7/2 | 374.7912 | 374.6847 | 799.8918 | E1 | 3.856 semi-empirical | 7.153e+07 semi-empirical | 71.5 | Kurucz, R. L., Can. J. Phys. 89, 417 (2011); semi-empirical line list gf4300.pos of 2017-… |
| 4d65s 6D3/2 | 4d65p 6F°3/2 | 375.5438 | 375.4371 | 798.2889 | E1 | 2.405 semi-empirical | 5.530e+07 semi-empirical | 55.8 | Kurucz, R. L., Can. J. Phys. 89, 417 (2011); semi-empirical line list gf4300.pos of 2017-… |
| 4d65s 6D3/2 | 4d65p 6F°5/2 | 376.9845 | 376.8774 | 795.2382 | E1 | 2.971 semi-empirical | 5.563e+07 semi-empirical | 56 | Kurucz, R. L., Can. J. Phys. 89, 417 (2011); semi-empirical line list gf4300.pos of 2017-… |
| 4d65s 6D1/2 | 4d65p 6F°1/2 | 377.2109 | 377.1037 | 794.7609 | E1 | 2.070 semi-empirical | 8.090e+07 semi-empirical | 81.6 | Kurucz, R. L., Can. J. Phys. 89, 417 (2011); semi-empirical line list gf4300.pos of 2017-… |
| 4d65s 6D1/2 | 4d65p 6F°3/2 | 378.0451 | 377.9378 | 793.0071 | E1 | 1.961 semi-empirical | 3.606e+07 semi-empirical | 36.4 | Kurucz, R. L., Can. J. Phys. 89, 417 (2011); semi-empirical line list gf4300.pos of 2017-… |
| 4d65s 6D9/2 | 4d65p 6D°7/2 | 398.6095 | 398.4968 | 752.0956 | E1 | 3.241 NIST | 4.200e+07 NIST | 47.2 | NIST ASD (accuracy n/a) |
| 4d65s 6D9/2 | 4d65p 6D°9/2 | 403.2762 | 403.1623 | 743.3924 | E1 | 5.718 NIST | 1.010e+08 NIST | 100 | NIST ASD (accuracy n/a) |
| 4d65s 6D7/2 | 4d65p 6D°5/2 | 405.0252 | 404.9108 | 740.1822 | E1 | 3.228 semi-empirical | 5.297e+07 semi-empirical | 61.5 | Kurucz, R. L., Can. J. Phys. 89, 417 (2011); semi-empirical line list gf4300.pos of 2017-… |
| 4d65s 6D5/2 | 4d65p 6D°3/2 | 408.9856 | 408.8702 | 733.0147 | E1 | 2.898 semi-empirical | 6.218e+07 semi-empirical | 73.8 | Kurucz, R. L., Can. J. Phys. 89, 417 (2011); semi-empirical line list gf4300.pos of 2017-… |
| 4d65s 6D7/2 | 4d65p 6D°7/2 | 409.6818 | 409.5662 | 731.7691 | E1 | 3.647 NIST | 4.900e+07 NIST | 55.1 | NIST ASD (accuracy n/a) |
| 4d65s 6D3/2 | 4d65p 6D°1/2 | 411.6226 | 411.5065 | 728.3188 | E1 | 2.168 semi-empirical | 6.825e+07 semi-empirical | 82 | Kurucz, R. L., Can. J. Phys. 89, 417 (2011); semi-empirical line list gf4300.pos of 2017-… |
| 4d65s 6D5/2 | 4d65p 6D°5/2 | 412.5380 | 412.4217 | 726.7026 | E1 | 1.728 semi-empirical | 1.436e+07 semi-empirical | 16.7 | Kurucz, R. L., Can. J. Phys. 89, 417 (2011); semi-empirical line list gf4300.pos of 2017-… |
| 4d65s 6D3/2 | 4d65p 6D°3/2 | 414.1008 | 413.9840 | 723.9601 | E1 | 0.386 semi-empirical | 1.064e+06 semi-empirical | 1.26 | Kurucz, R. L., Can. J. Phys. 89, 417 (2011); semi-empirical line list gf4300.pos of 2017-… |
| 4d65s 6D7/2 | 4d65p 6D°9/2 | 414.6130 | 414.4961 | 723.0658 | E1 | 1.542 semi-empirical | 6.759e+06 semi-empirical | 7.47 | Kurucz, R. L., Can. J. Phys. 89, 417 (2011); semi-empirical line list gf4300.pos of 2017-… |
| 4d65s 6D1/2 | 4d65p 6D°1/2 | 414.6295 | 414.5126 | 723.0371 | E1 | 1.013 semi-empirical | 1.458e+07 semi-empirical | 17.5 | Kurucz, R. L., Can. J. Phys. 89, 417 (2011); semi-empirical line list gf4300.pos of 2017-… |
| 4d65s 6D1/2 | 4d65p 6D°3/2 | 417.1441 | 417.0266 | 718.6784 | E1 | 1.714 semi-empirical | 2.049e+07 semi-empirical | 24.3 | Kurucz, R. L., Can. J. Phys. 89, 417 (2011); semi-empirical line list gf4300.pos of 2017-… |
| 4d65s 6D5/2 | 4d65p 6D°7/2 | 417.3699 | 417.2523 | 718.2895 | E1 | 1.938 semi-empirical | 1.309e+07 semi-empirical | 14.7 | Kurucz, R. L., Can. J. Phys. 89, 417 (2011); semi-empirical line list gf4300.pos of 2017-… |
| 4d65s 6D3/2 | 4d65p 6D°5/2 | 417.7431 | 417.6253 | 717.6480 | E1 | 1.998 semi-empirical | 1.850e+07 semi-empirical | 21.5 | Kurucz, R. L., Can. J. Phys. 89, 417 (2011); semi-empirical line list gf4300.pos of 2017-… |
| 4d55s2 6S5/2 | 4d55s5p 6P°3/2 | 423.9372 | 423.8178 | 707.1624 | E1 | 2.391 NIST | 3.800e+07 NIST | 100 | NIST ASD (accuracy n/a) |
| 4d55s2 6S5/2 | 4d55s5p 6P°5/2 | 426.3445 | 426.2245 | 703.1695 | E1 | 3.030 NIST | 4.000e+07 NIST | 100 | NIST ASD (accuracy n/a) |
| 4d55s2 6S5/2 | 4d55s5p 6P°7/2 | 429.8243 | 429.7034 | 697.4768 | E1 | 3.629 NIST | 4.200e+07 NIST | 100 | NIST ASD (accuracy n/a) |
| 4d55s2 6S5/2 | 4d55s5p 8P°7/2 | 592.6098 | 592.4456 | 505.8851 | E1 (intercombination) | 0.392 semi-empirical | 1.873e+05 semi-empirical | 99.6 | Kurucz, R. L., Can. J. Phys. 89, 417 (2011); semi-empirical line list gf4300.pos of 2017-… |
| 4d55s2 6S5/2 | 4d55s5p 8P°5/2 | 608.6905 | 608.5220 | 492.5203 | E1 (intercombination) | 0.254 semi-empirical | 9.665e+04 semi-empirical | 99.7 | Kurucz, R. L., Can. J. Phys. 89, 417 (2011); semi-empirical line list gf4300.pos of 2017-… |
Reduced dipole matrix elements follow the convention A = ω³|d|²/(3πε₀ħc³(2J′+1)), with J′ the upper level. Tags show where a number comes from: measured, NIST compilation, high-accuracy theory, a semi-empirical calculation (Kurucz line list, used only where no measurement or NIST value exists; typically within a factor 2), or a model calculation.
Tc energy levels
Tc⁺ ionisation limit 57421.68 cm⁻¹ = 7.11938 eV (174.150 nm)
Sources
- Kron, Beerwerth, Raeder, Fritzsche, Heinke, Schoenberg, Truemper, Wendt, Phys. Rev. C 102…
- Kurucz semi-empirical calculation (K17), life4300.dat
- Kurucz, R. L., Can. J. Phys. 89, 417 (2011); semi-empirical line list gf4300.pos of 2017-…
- NIST ASD
- NIST ASD level energies
Hyperfine constants and isotope shifts are from resonance ionization spectroscopy with ~100 MHz resolution (Kron et al. 2020, open access via the GSI repository). Isotope shifts are nu(first) - nu(second). All level lifetimes in this file are THEORY (Kurucz) because no measurement exists; treat them as ~25 % estimates. nuclear_moments is an extra top-level block (not in the schema) with the moments derived in the same paper.
Atoms with measured data
- Lithium-632 levels, 85 lines
- Lithium-732 levels, 85 lines
- Beryllium-917 levels, 26 lines
- Sodium-2336 levels, 106 lines
- Magnesium-2418 levels, 61 lines
- Magnesium-2518 levels, 61 lines
- Potassium-3934 levels, 84 lines
- Potassium-4034 levels, 84 lines
- Potassium-4134 levels, 84 lines
- Calcium-4035 levels, 61 lines
- Calcium-4335 levels, 61 lines
- Chromium-5256 levels, 87 lines
- Chromium-5356 levels, 87 lines
- Rubidium-8536 levels, 94 lines
- Rubidium-8736 levels, 94 lines
- Strontium-8440 levels, 70 lines
- Strontium-8640 levels, 70 lines
- Strontium-8740 levels, 70 lines
- Strontium-8840 levels, 70 lines
- Cadmium-11115 levels, 21 lines
- Cadmium-11315 levels, 21 lines
- Cadmium-11415 levels, 21 lines
- Caesium-13331 levels, 79 lines
- Barium-13744 levels, 89 lines
- Barium-13844 levels, 89 lines
- Dysprosium-16139 levels, 55 lines
- Dysprosium-16239 levels, 55 lines
- Dysprosium-16339 levels, 55 lines
- Dysprosium-16439 levels, 55 lines
- Erbium-16673 levels, 90 lines
- Erbium-16773 levels, 90 lines
- Erbium-16873 levels, 90 lines
- Thulium-16972 levels, 73 lines
- Ytterbium-17118 levels, 26 lines
- Ytterbium-17318 levels, 26 lines
- Ytterbium-17418 levels, 26 lines
- Mercury-19927 levels, 47 lines
- Mercury-20127 levels, 47 lines
- Mercury-20227 levels, 47 lines