Atomic energy level diagrams

Thulium-169 energy level diagram

Energy levels and transitions of neutral 169Tm (Tm I, nuclear spin I = 1/2): the 73 strongest classified lines below 2 µm from the NIST Atomic Spectra Database and the 72 levels they connect, each line with its vacuum wavelength, frequency and, for 71 of them, the reduced dipole matrix element. Level energies come from NIST and refer to the natural isotope mixture; transition rates are 68 NIST, 3 measured, 1 theory. Hyperfine constants and measured frequencies are those of this isotope.

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Thulium-169 energy level diagram with transition wavelengths and dipole matrix elements

Download: diagram (PDF) diagram (SVG) transitions (CSV) levels (CSV) source code

Key transitions of 169Tm

Transitionλ vac (nm)λ air (nm)ν (THz)|⟨J‖er‖J′⟩| (ea₀)A (s⁻¹)Γ/2π up. (MHz)branch (%)Use
2F°7/2 – (5,3/2)9/2410.6997410.5838729.95544.6416.300e+0710.14100first-stage
2F°7/2 – (4,5/2)9/2420.4914420.3730712.95742.7762.100e+073.87286.3alternative blue cycling line
2F°7/2 – (7/2,2)9/2506.3665506.2253592.0464––––third-stage deep narrow-line MOT
2F°7/2 – (6,5/2)9/2530.8592530.7116564.73061.2692.180e+060.3467100second-stage narrow-line
2F°7/2 – 2F°5/21140.08961139.7776262.955164–7.000e+001.421e-0678.4inner-shell M1 optical clock transition

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).

169Tm hyperfine structure (I = 1/2)

LevelA (MHz)B (MHz)Shift of each F level from the centre of gravity (MHz)
2F°7/2-374.137661(3)–F=3: +841.81 F=4: -654.74
2F°5/2-704.648958–F=2: +1233.14 F=3: -880.81
(6,5/2)9/2-422.11(3)–F=4: +1160.81 F=5: -949.75
(4,5/2)9/2-317.32(16)–F=4: +872.63 F=5: -713.97
(23873)7/2352.75(18)–F=3: -793.69 F=4: +617.31
(5,3/2)9/2-371.50(16)–F=4: +1021.62 F=5: -835.88
(7/2,1)5/2-656.5(4)–F=2: +1148.82 F=3: -820.58

Measured A, B constants; sources in the data file.

Closed and nearly closed transitions of 169Tm

Transitionλ vacuum (nm)Lower levelA (s⁻¹)Leak per scattered photonPhotons before a leakWhere the leak goes
(6,5/2)17/2 → (5,9/2)°19/2358.7090metastable7.100e+07 NISTclosed–no other level can be reached by electric-dipole decay
2F°7/2 → (6,5/2)9/2530.8592ground2.180e+06 measuredclosed–no other level can be reached by electric-dipole decay
2F°7/2 → (7/2,2)9/2506.3665ground–closed–no other level can be reached by electric-dipole decay
2F°7/2 → (5,3/2)9/2410.6997ground6.300e+07 measured1 × 10−5 from theory100,000leak channels not listed

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 169Tm transitions below 2 µm

Lower levelUpper levelλ vacuum (nm)λ air (nm)ν (THz)Type|⟨J‖er‖J′⟩| (ea₀)A (s⁻¹)Branching (%)Source of matrix element / A
2F°7/2(39560)7/2252.7780252.70201185.9913E10.968 NIST1.470e+07 NIST43.2NIST ASD (accuracy B+)
2F°7/2(38502)9/2259.7268259.64911154.2609E11.100 NIST1.400e+07 NIST83.6NIST ASD (accuracy B+)
2F°7/2(38434)5/2260.1868260.10911152.2199E10.882 NIST1.490e+07 NIST76.4NIST ASD (accuracy B+)
2F°5/2(7/2,3)5/2284.1960284.11241054.8793E10.976 NIST1.400e+07 NIST66.9NIST ASD (accuracy D+)
2F°7/2(35026)5/2285.5004285.41651050.0597E11.291 NIST2.420e+07 NIST33.4NIST ASD (accuracy B)
2F°7/2(5/2,1)7/2291.5692291.48391028.2033E10.959 NIST9.400e+06 NIST4.51NIST ASD (accuracy C+)
2F°7/2(33624)7/2297.4086297.32181008.0156E11.501 NIST2.170e+07 NIST97.9NIST ASD (accuracy B+)
2F°7/2(3,5/2)7/2304.7757304.6870983.6496E11.342 NIST1.610e+07 NIST82.1NIST ASD (accuracy B+)
2F°7/2(32446)7/2308.2019308.1124972.7144E11.422 NIST1.750e+07 NIST52.5NIST ASD (accuracy B+)
2F°5/2(40787)5/2312.3439312.2533959.8154E12.346 NIST6.100e+07 NIST99.4NIST ASD (accuracy B+)
2F°7/2(31510)7/2317.3572317.2654944.6532E11.417 NIST1.590e+07 NIST87.6NIST ASD (accuracy B)
2F°5/2(39560)7/2324.7896324.6959923.0360E11.839 NIST2.500e+07 NIST73.5NIST ASD (accuracy D+)
2F°5/2(4,5/2)3/2325.2720325.1782921.6668E11.206 NIST2.140e+07 NIST99.9NIST ASD (accuracy B+)
(6,3/2)9/2(43675)°9/2327.2717327.1774916.0353E11.611 NIST1.500e+07 NIST33NIST ASD (accuracy D)
(6,3/2)9/2(43448)°11/2329.7254329.6305909.2186E11.900 NIST1.700e+07 NIST81.6NIST ASD (accuracy C)
(6,3/2)9/2(43186)°11/2332.5936332.4979901.3777E11.400 NIST9.000e+06 NIST81.2NIST ASD (accuracy D)
(6,3/2)9/2(42962)°11/2335.0951334.9988894.6489E13.835 NIST6.600e+07 NIST48.8NIST ASD (accuracy B)
(6,3/2)9/2(42839)°9/2336.4751336.3784890.9797E11.371 NIST1.000e+07 NIST30.2NIST ASD (accuracy D)
2F°5/2(38343)7/2338.1654338.0683886.5261E11.414 NIST1.310e+07 NIST82.8NIST ASD (accuracy B)
(6,3/2)9/2(42582)°11/2339.4161339.3187883.2595E12.764 NIST3.300e+07 NIST72.9NIST ASD (accuracy C)
(6,3/2)9/2(42541)°11/2339.8845339.7870882.0421E12.812 NIST3.400e+07 NIST81.6NIST ASD (accuracy C)
2F°5/2(38123)7/2340.6949340.5971879.9441E11.380 NIST1.220e+07 NIST80.5NIST ASD (accuracy B)
2F°7/2(4,3/2)9/2341.1026341.0048878.8923E11.386 NIST9.800e+06 NIST100NIST ASD (accuracy B+)
(6,3/2)15/2(44572)°17/2341.2874341.1895878.4164E11.527 NIST6.600e+06 NIST8.84NIST ASD (accuracy C+)
(6,3/2)15/2(44566)°15/2341.3570341.2591878.2374E16.139 NIST1.200e+08 NIST75.6NIST ASD (accuracy D+)
(6,3/2)9/2(42371)°7/2341.8674341.7694876.9262E11.820 NIST2.100e+07 NIST78.3NIST ASD (accuracy C)
(6,5/2)17/2(45609)°15/2343.0312342.9329873.9510E16.002 NIST1.130e+08 NIST70.1NIST ASD (accuracy C)
(6,3/2)9/2(42133)°7/2344.6653344.5666869.8074E11.638 NIST1.660e+07 NIST35NIST ASD (accuracy B+)
(6,3/2)9/2(42119)°11/2344.8339344.7351869.3822E12.424 NIST2.420e+07 NIST64.6NIST ASD (accuracy B+)
(6,3/2)11/2(44419)°13/2346.8503346.7510864.3282E13.982 NIST5.500e+07 NIST48.9NIST ASD (accuracy D+)
(6,3/2)9/2(41874)°11/2347.7685347.6690862.0460E14.085 NIST6.700e+07 NIST79.1NIST ASD (accuracy B+)
(6,3/2)11/2(44307)°13/2348.1970348.0973860.9853E13.932 NIST5.300e+07 NIST31.8NIST ASD (accuracy D+)
(6,3/2)9/2(41786)°9/2348.8375348.7377859.4042E15.790 NIST1.600e+08 NIST94.4NIST ASD (accuracy B+)
(6,3/2)9/2(41687)°11/2350.0445349.9444856.4409E11.702 NIST1.140e+07 NIST57.1NIST ASD (accuracy B)
(6,3/2)9/2(41576)°9/2351.4131351.3126853.1055E11.404 NIST9.200e+06 NIST20.7NIST ASD (accuracy B)
(6,3/2)9/2(41569)°11/2351.5000351.3995852.8947E11.829 NIST1.300e+07 NIST77.7NIST ASD (accuracy B)
(6,3/2)9/2(41525)°7/2352.0434351.9427851.5782E11.731 NIST1.740e+07 NIST78.6NIST ASD (accuracy B+)
(6,5/2)17/2(44572)°17/2355.6832355.5816842.8637E15.097 NIST6.500e+07 NIST87.1NIST ASD (accuracy B+)
(6,3/2)9/2(41124)°9/2357.0826356.9807839.5605E12.526 NIST2.840e+07 NIST81.5NIST ASD (accuracy B+)
(6,3/2)9/2(41081)°11/2357.6311357.5290838.2729E12.016 NIST1.500e+07 NIST69.9NIST ASD (accuracy B+)
(6,5/2)17/2(5,9/2)°19/2358.7090358.6067835.7538E15.688 NIST7.100e+07 NIST100NIST ASD (accuracy B+)
(6,3/2)9/2(40596)°7/2363.9448363.8411823.7305E14.555 NIST1.090e+08 NIST92.7NIST ASD (accuracy B+)
(6,3/2)9/2(40534)°7/2364.7743364.6703821.8575E13.363 NIST5.900e+07 NIST96.2NIST ASD (accuracy B+)
2F°7/2(5,5/2)9/2371.8976371.7918806.1157E16.046 NIST1.440e+08 NIST99.4NIST ASD (accuracy B+)
2F°7/2(26701)7/2374.5132374.4068800.4856E14.531 NIST9.900e+07 NIST100NIST ASD (accuracy B+)
2F°7/2(26646)9/2375.2878375.1812798.8334E12.131 NIST1.740e+07 NIST99.9NIST ASD (accuracy B)
2F°5/2(35090)3/2379.9619379.8541789.0066E13.650 NIST1.230e+08 NIST99.6NIST ASD (accuracy B+)
(6,3/2)11/2(41882)°9/2380.3159380.2080788.2721E12.376 NIST2.080e+07 NIST46.8NIST ASD (accuracy B+)
2F°5/2(35026)5/2380.8802380.7721787.1044E12.802 NIST4.800e+07 NIST66.2NIST ASD (accuracy B+)
(6,3/2)15/2(41299)°17/2384.1962384.0872780.3108E14.512 NIST4.040e+07 NIST67.1NIST ASD (accuracy B+)
2F°7/2(25745)5/2388.4232388.3131771.8192E14.289 NIST1.060e+08 NIST99.6NIST ASD (accuracy B+)
2F°7/2(5,5/2)7/2388.8449388.7347770.9822E12.939 NIST3.720e+07 NIST97.5NIST ASD (accuracy B+)
2F°5/2(5/2,1)7/2391.7585391.6476765.2480E16.856 NIST1.980e+08 NIST95NIST ASD (accuracy B+)
2F°5/2(5/2,1)5/2395.0390394.9272758.8933E15.001 NIST1.370e+08 NIST91.8NIST ASD (accuracy B+)
(6,5/2)17/2(41299)°17/2402.5367402.4229744.7581E13.212 NIST1.780e+07 NIST29.5NIST ASD (accuracy B+)
2F°5/2(5/2,2)3/2404.5616404.4473741.0305E11.854 NIST2.630e+07 NIST99.9NIST ASD (accuracy B+)
(6,3/2)9/2(37769)°9/2405.6951405.5806738.9600E11.572 NIST7.500e+06 NIST58.7NIST ASD (accuracy B+)
2F°7/2(7/2,1)5/2409.5336409.4181732.0338E14.465 NIST9.800e+07 NIST100NIST ASD (accuracy B+)
2F°7/2(5,3/2)9/2410.6997410.5838729.9554E14.641 measured6.300e+07 measured100Kolachevsky, Akimov, Tolstikhina, Chebakov, Sokolov, Rodionov, Kanorski, Sorokin, Appl. P…
2F°5/2(3,5/2)3/2413.9498413.8331724.2241E13.326 NIST7.900e+07 NIST100NIST ASD (accuracy B+)
(6,3/2)9/2(37277)°11/2413.9558413.8391724.2137E12.633 NIST1.650e+07 NIST74.4NIST ASD (accuracy B+)
2F°7/2(23873)7/2418.8796418.7616715.7007E14.310 NIST6.400e+07 NIST99.8NIST ASD (accuracy B+)
2F°7/2(4,5/2)9/2420.4914420.3730712.9574E12.776 measured2.100e+07 measured86.3Kolachevsky, Akimov, Tolstikhina, Chebakov, Sokolov, Rodionov, Kanorski, Sorokin, Appl. P…
2F°5/2(32446)7/2422.3862422.2672709.7591E12.161 NIST1.570e+07 NIST47.1NIST ASD (accuracy B+)
(6,3/2)9/2(36378)°9/2429.9573429.8364697.2610E11.879 NIST9.000e+06 NIST60.9NIST ASD (accuracy B+)
(6,3/2)15/2(38013)°13/2439.7191439.5956681.7818E11.781 NIST5.400e+06 NIST56.7NIST ASD (accuracy B+)
(6,3/2)11/2(37646)°13/2453.3426453.2155661.2935E11.982 NIST6.100e+06 NIST63.4NIST ASD (accuracy B+)
(6,3/2)15/2(6,3/2)°15/2467.6629467.5321641.0439E12.510 NIST7.800e+06 NIST85.8NIST ASD (accuracy B+)
(6,3/2)15/2(36274)°15/2476.1239475.9908629.6522E12.185 NIST5.600e+06 NIST77.3NIST ASD (accuracy B+)
2F°7/2(7/2,2)9/2506.3665506.2253592.0464E1––––
(6,5/2)17/2(6,5/2)°17/2521.4826521.3374574.8849E12.680 NIST5.700e+06 NIST63.8NIST ASD (accuracy B+)
2F°7/2(6,5/2)9/2530.8592530.7116564.7306E11.269 measured2.180e+06 measured100Anderson, Den Hartog, Lawler, J. Opt. Soc. Am. B 13, 2382 (1996), Table 1
2F°7/22F°5/21140.08961139.7776262.9552M1–7.000e+00 theory78.4Kolachevsky, Akimov, Tolstikhina, Chebakov, Sokolov, Rodionov, Kanorski, Sorokin, Appl. P…

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, or a model calculation.

169Tm energy levels

LevelEnergy (cm⁻¹)JParityLifetimegJHyperfine A (MHz)Hyperfine B (MHz)Lifetime sourceHyperfine source
2F°7/20.0007/2oddstable1.1412-374.138––Giglberger, Penselin, Z. Phys. 199, 244 (1967) (abstract)
2F°5/28771.2435/2odd> 112 ms measured0.855-704.649–Sukachev, Fedorov, Tolstikhina, Tregubov, Kalganova, Vishnyakova, Golovizin, Kolachevsky,…Mishin, Tregubov, Golovizin, Kolachevsky, arXiv:2406.20002 (2024)
(6,3/2)9/213119.6109/2even–1.305––––
(6,3/2)15/215271.00215/2even–1.08––––
(6,3/2)11/215587.81111/2even–1.255––––
(6,5/2)17/216456.91317/2even–1.175––––
(6,5/2)9/218837.3859/2even459 ns measured1.1318-422.112–Anderson, Den Hartog, Lawler, J. Opt. Soc. Am. B 13, 2382 (1996), Table 1Fedorov, Vishnyakova, Kalganova, Sukachev, Golovizin, Tregubov, Khabarova, Akimov, Kolach…
(7/2,2)9/219748.5439/2even–1.29––––
(4,5/2)9/223781.6989/2even41.1 ns measured1.1499-317.32–Anderson, Den Hartog, Lawler, J. Opt. Soc. Am. B 13, 2382 (1996), Table 1Kolachevsky, Akimov, Tolstikhina, Chebakov, Sokolov, Rodionov, Kanorski, Sorokin, Appl. P…
(23873)7/223873.2077/2even15.6 ns measured1.135352.75–Anderson, Den Hartog, Lawler, J. Opt. Soc. Am. B 13, 2382 (1996), Table 1Kolachevsky, Akimov, Tolstikhina, Chebakov, Sokolov, Rodionov, Kanorski, Sorokin, Appl. P…
(5,3/2)9/224348.6929/2even15.7 ns measured1.12-371.5–Anderson, Den Hartog, Lawler, J. Opt. Soc. Am. B 13, 2382 (1996), Table 1Kolachevsky, Akimov, Tolstikhina, Chebakov, Sokolov, Rodionov, Kanorski, Sorokin, Appl. P…
(7/2,1)5/224418.0185/2even10.2 ns measured1.06-656.467–Anderson, Den Hartog, Lawler, J. Opt. Soc. Am. B 13, 2382 (1996), Table 1Kolachevsky, Akimov, Tolstikhina, Chebakov, Sokolov, Rodionov, Kanorski, Sorokin, Appl. P…
(5,5/2)7/225717.1977/2even26.2 ns measured1.02––Anderson, Den Hartog, Lawler, J. Opt. Soc. Am. B 13, 2382 (1996), Table 1–
(25745)5/225745.1175/2even9.4 ns measured1.09––Anderson, Den Hartog, Lawler, J. Opt. Soc. Am. B 13, 2382 (1996), Table 1–
(26646)9/226646.2149/2even57.4 ns measured0.961––Anderson, Den Hartog, Lawler, J. Opt. Soc. Am. B 13, 2382 (1996), Table 1–
(26701)7/226701.3257/2even10.1 ns measured1.076––Anderson, Den Hartog, Lawler, J. Opt. Soc. Am. B 13, 2382 (1996), Table 1–
(5,5/2)9/226889.1259/2even6.9 ns measured1.11––Anderson, Den Hartog, Lawler, J. Opt. Soc. Am. B 13, 2382 (1996), Table 1–
(4,3/2)9/229316.6909/2even102 ns measured0.978––Anderson, Den Hartog, Lawler, J. Opt. Soc. Am. B 13, 2382 (1996), Table 1–
(31510)7/231510.2407/2even55.1 ns measured1.11––Anderson, Den Hartog, Lawler, J. Opt. Soc. Am. B 13, 2382 (1996), Table 1–
(32446)7/232446.2607/2even30 ns measured0.89––Anderson, Den Hartog, Lawler, J. Opt. Soc. Am. B 13, 2382 (1996), Table 1–
(3,5/2)7/232811.0207/2even51 ns measured1.04––Anderson, Den Hartog, Lawler, J. Opt. Soc. Am. B 13, 2382 (1996), Table 1–
(3,5/2)3/232928.7603/2even12.7 ns measured0.935––Anderson, Den Hartog, Lawler, J. Opt. Soc. Am. B 13, 2382 (1996), Table 1–
(5/2,2)3/233489.3603/2even38 ns measured1.468––Anderson, Den Hartog, Lawler, J. Opt. Soc. Am. B 13, 2382 (1996), Table 1–
(33624)7/233623.7807/2even45.1 ns measured0.92––Anderson, Den Hartog, Lawler, J. Opt. Soc. Am. B 13, 2382 (1996), Table 1–
(5/2,1)5/234085.2005/2even6.7 ns measured0.95––Anderson, Den Hartog, Lawler, J. Opt. Soc. Am. B 13, 2382 (1996), Table 1–
(5/2,1)7/234297.1707/2even4.8 ns measured0.915––Anderson, Den Hartog, Lawler, J. Opt. Soc. Am. B 13, 2382 (1996), Table 1–
(35026)5/235026.2205/2even13.8 ns measured1.022––Anderson, Den Hartog, Lawler, J. Opt. Soc. Am. B 13, 2382 (1996), Table 1–
(35090)3/235089.6703/2even8.1 ns measured0.85––Anderson, Den Hartog, Lawler, J. Opt. Soc. Am. B 13, 2382 (1996), Table 1–
(6,5/2)°17/235633.01017/2odd112 ns measured1.18––Anderson, Den Hartog, Lawler, J. Opt. Soc. Am. B 13, 2382 (1996), Table 2–
(36274)°15/236273.94015/2odd138 ns measured1.13––Anderson, Den Hartog, Lawler, J. Opt. Soc. Am. B 13, 2382 (1996), Table 2–
(36378)°9/236377.7339/2odd67.7 ns measured1.21––Anderson, Den Hartog, Lawler, J. Opt. Soc. Am. B 13, 2382 (1996), Table 2–
(6,3/2)°15/236653.92415/2odd110 ns measured1.13––Anderson, Den Hartog, Lawler, J. Opt. Soc. Am. B 13, 2382 (1996), Table 2–
(37277)°11/237276.77811/2odd45.1 ns measured1.25––Anderson, Den Hartog, Lawler, J. Opt. Soc. Am. B 13, 2382 (1996), Table 2–
(37646)°13/237646.18613/2odd104 ns measured1.175––Anderson, Den Hartog, Lawler, J. Opt. Soc. Am. B 13, 2382 (1996), Table 2–
(37769)°9/237768.6629/2odd78.3 ns measured1.215––Anderson, Den Hartog, Lawler, J. Opt. Soc. Am. B 13, 2382 (1996), Table 2–
(38013)°13/238012.79513/2odd105 ns measured1.09––Anderson, Den Hartog, Lawler, J. Opt. Soc. Am. B 13, 2382 (1996), Table 2–
(38123)7/238123.0207/2even66 ns measured1.14––Anderson, Den Hartog, Lawler, J. Opt. Soc. Am. B 13, 2382 (1996), Table 1–
(38343)7/238342.5707/2even63.2 ns measured1.108––Anderson, Den Hartog, Lawler, J. Opt. Soc. Am. B 13, 2382 (1996), Table 1–
(38434)5/238433.9205/2even51.3 ns measured–––Anderson, Den Hartog, Lawler, J. Opt. Soc. Am. B 13, 2382 (1996), Table 1–
(38502)9/238502.0009/2even59.7 ns measured1.1––Anderson, Den Hartog, Lawler, J. Opt. Soc. Am. B 13, 2382 (1996), Table 1–
(4,5/2)3/239514.7403/2even46.7 ns measured0.8––Anderson, Den Hartog, Lawler, J. Opt. Soc. Am. B 13, 2382 (1996), Table 1–
(39560)7/239560.4107/2even29.4 ns measured0.895––Anderson, Den Hartog, Lawler, J. Opt. Soc. Am. B 13, 2382 (1996), Table 1–
(40534)°7/240533.8257/2odd16.3 ns measured1.24––Anderson, Den Hartog, Lawler, J. Opt. Soc. Am. B 13, 2382 (1996), Table 2–
(40596)°7/240596.3027/2odd8.5 ns measured1.305––Anderson, Den Hartog, Lawler, J. Opt. Soc. Am. B 13, 2382 (1996), Table 2–
(40787)5/240787.2405/2even16.3 ns measured0.91––Anderson, Den Hartog, Lawler, J. Opt. Soc. Am. B 13, 2382 (1996), Table 1–
(41081)°11/241081.38411/2odd46.6 ns measured1.295––Anderson, Den Hartog, Lawler, J. Opt. Soc. Am. B 13, 2382 (1996), Table 2–
(41124)°9/241124.3349/2odd28.7 ns measured1.244––Anderson, Den Hartog, Lawler, J. Opt. Soc. Am. B 13, 2382 (1996), Table 2–
(41299)°17/241299.37017/2odd16.6 ns measured1.08––Anderson, Den Hartog, Lawler, J. Opt. Soc. Am. B 13, 2382 (1996), Table 2–
(41525)°7/241525.2007/2odd45.2 ns measured1.105––Anderson, Den Hartog, Lawler, J. Opt. Soc. Am. B 13, 2382 (1996), Table 2–
(41569)°11/241569.11411/2odd59.8 ns measured1.205––Anderson, Den Hartog, Lawler, J. Opt. Soc. Am. B 13, 2382 (1996), Table 2–
(41576)°9/241576.1469/2odd22.5 ns measured1.249––Anderson, Den Hartog, Lawler, J. Opt. Soc. Am. B 13, 2382 (1996), Table 2–
(41687)°11/241687.40411/2odd50.1 ns measured1.145––Anderson, Den Hartog, Lawler, J. Opt. Soc. Am. B 13, 2382 (1996), Table 2–
(41786)°9/241786.2499/2odd5.9 ns measured1.25––Anderson, Den Hartog, Lawler, J. Opt. Soc. Am. B 13, 2382 (1996), Table 2–
(41874)°11/241874.36911/2odd11.8 ns measured1.16––Anderson, Den Hartog, Lawler, J. Opt. Soc. Am. B 13, 2382 (1996), Table 2–
(41882)°9/241881.7399/2odd22.5 ns measured1.18––Anderson, Den Hartog, Lawler, J. Opt. Soc. Am. B 13, 2382 (1996), Table 2–
(42119)°11/242119.08011/2odd26.7 ns measured1.1––Anderson, Den Hartog, Lawler, J. Opt. Soc. Am. B 13, 2382 (1996), Table 2–
(42133)°7/242133.2637/2odd21.1 ns measured1.17––Anderson, Den Hartog, Lawler, J. Opt. Soc. Am. B 13, 2382 (1996), Table 2–
(42371)°7/242370.7187/2odd37.3 ns measured1.043––Anderson, Den Hartog, Lawler, J. Opt. Soc. Am. B 13, 2382 (1996), Table 2–
(42541)°11/242541.36711/2odd24 ns measured1.1––Anderson, Den Hartog, Lawler, J. Opt. Soc. Am. B 13, 2382 (1996), Table 2–
(42582)°11/242581.97411/2odd22.1 ns measured1.135––Anderson, Den Hartog, Lawler, J. Opt. Soc. Am. B 13, 2382 (1996), Table 2–
(42839)°9/242839.4939/2odd30.2 ns measured1.086––Anderson, Den Hartog, Lawler, J. Opt. Soc. Am. B 13, 2382 (1996), Table 2–
(42962)°11/242961.88411/2odd7.4 ns measured1.205––Anderson, Den Hartog, Lawler, J. Opt. Soc. Am. B 13, 2382 (1996), Table 2–
(43186)°11/243186.33511/2odd90.2 ns measured1.196––Anderson, Den Hartog, Lawler, J. Opt. Soc. Am. B 13, 2382 (1996), Table 2–
(43448)°11/243447.87811/2odd48 ns measured1.105––Anderson, Den Hartog, Lawler, J. Opt. Soc. Am. B 13, 2382 (1996), Table 2–
(43675)°9/243675.2589/2odd22 ns measured1.04––Anderson, Den Hartog, Lawler, J. Opt. Soc. Am. B 13, 2382 (1996), Table 2–
(7/2,3)5/243958.2305/2even47.8 ns measured–––Anderson, Den Hartog, Lawler, J. Opt. Soc. Am. B 13, 2382 (1996), Table 1–
(44307)°13/244307.18813/2odd6 ns measured1.13––Anderson, Den Hartog, Lawler, J. Opt. Soc. Am. B 13, 2382 (1996), Table 2–
(5,9/2)°19/244334.66019/2odd14.1 ns measured1.18––Anderson, Den Hartog, Lawler, J. Opt. Soc. Am. B 13, 2382 (1996), Table 2–
(44419)°13/244418.69513/2odd8.9 ns measured1.145––Anderson, Den Hartog, Lawler, J. Opt. Soc. Am. B 13, 2382 (1996), Table 2–
(44566)°15/244565.85015/2odd6.3 ns measured1.135––Anderson, Den Hartog, Lawler, J. Opt. Soc. Am. B 13, 2382 (1996), Table 2–
(44572)°17/244571.82017/2odd13.4 ns measured1.18––Anderson, Den Hartog, Lawler, J. Opt. Soc. Am. B 13, 2382 (1996), Table 2–
(45609)°15/245608.78015/2odd6.2 ns measured1.15––Anderson, Den Hartog, Lawler, J. Opt. Soc. Am. B 13, 2382 (1996), Table 2–

Tm⁺ ionisation limit 49880.57 cm⁻¹ = 6.18440 eV (200.479 nm)

Sources

169Tm has I=1/2: every level is a hyperfine doublet F=J+-1/2 with splitting A(J+1/2), no B. Signed splittings follow Kolachevsky et al. 2007 (negative = larger F lower). The Anderson et al. 1996 lifetime tables (68 even + 126 odd levels) were read from the publisher abstract page, whose HTML embeds the tables, through an automated page reader (direct download is captcha-blocked), not from the PDF; every row was matched to a NIST level by energy (0.02 cm^-1) and J, and all lifetimes were checked to be <= 1/sum(A) from the NIST lines file within 15%; rows used on the site were read twice. No per-level uncertainty is printed in those tables (so no unc is given). Extra fields beyond SCHEMA.md: top-level ionization_limit; level fields lifetime_other, hfs_splitting_MHz; transition fields linewidth_MHz / linewidth_kHz / linewidth_Hz, leak_to_metastable, frequency_component_THz, magic_wavelength_nm, differential_frequency_MHz. frequency_THz of the clock line is the hyperfine centre of gravity derived from the measured F=4->F=3 component. rme_J_ea0 values are derived from the A coefficient of the same entry (schema convention). Entries flagged LOWER BOUND / UPPER BOUND / LOWER LIMIT in their note are bounds. g_J without a literature source is copied from the NIST levels file.

Atoms with measured data

All elements: periodic table