Dysprosium-161 energy level diagram
Energy levels and transitions of neutral 161Dy (Dy I, nuclear spin I = 5/2): 39 levels and 55 lines below 2 µm, each with its vacuum wavelength, frequency and, for 54 of them, the reduced dipole matrix element. Level energies come from the NIST Atomic Spectra Database; transition rates are 26 NIST, 23 measured, 5 theory.
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 161Dy
| Transition | λ vac (nm) | λ air (nm) | ν (THz) | |⟨J‖er‖J′⟩| (ea₀) | A (s⁻¹) | Γ/2π up. (MHz) | branch (%) | Use |
|---|---|---|---|---|---|---|---|---|
| 5I8 – (26868)°8 | 372.1890 | 372.0832 | 805.4845 | – | – | – | – | UV ground-state line |
| 5I8 – (8,1)°7 | 404.7113 | 404.5970 | 740.7563 | 9.707 | 1.920e+08 | 30.61 | 99.8 | strong blue J=8->7 line |
| 5I8 – (8,1)°8 | 418.8001 | 418.6821 | 715.8366 | 8.812 | 1.260e+08 | 20.15 | 99.5 | strong blue J=8->8 line |
| 5I8 – (23832)°8 | 419.6028 | 419.4846 | 714.4672 | 7.386 | 8.800e+07 | 13.96 | 100 | strong blue J=8->8 line |
| 5I8 – (8,1)°9 | 421.2902 | 421.1715 | 711.6057 | 11.84 | 2.000e+08 | 33.16 | 100 | main broad cooling line: Zeeman slower, transverse coolin… |
| 5I8 – (7,2)°8 | 456.6373 | 456.5093 | 656.5221 | 0.726 | 6.600e+05 | 0.1315 | 79.9 | pure 6s->6p reference line for King plots |
| 5I8 – (8,2)°9 | 564.1065 | 563.9499 | 531.4466 | 0.908 | 4.900e+05 | 0.07764 | 100 | closed J=8->9 narrow line |
| 5I8 – 7K°9 | 598.1652 | 597.9995 | 501.1867 | 0.393* | 7.700e+04 | 0.01224 | 100 | "598 nm" closed J=8->9 narrow line proposed for narrow-li… |
| 5I8 – (8,1)°7 | 599.0223 | 598.8564 | 500.4696 | 0.944 | 5.600e+05 | 0.08941 | 99.7 | narrow J=8->7 probe line |
| 5I8 – (8,1)°9 | 626.0819 | 625.9088 | 478.8390 | 1.431 | 8.900e+05 | 0.136 | 100 | narrow-line MOT |
| 5I8 – 5H°7 | 658.1186 | 657.9368 | 455.5295 | 1.275 | 7.700e+05 | 0.1294 | 94.7 | narrow probe line used for Doppler thermometry of the 421… |
| 5I8 – 5I°8 | 683.7308 | 683.5421 | 438.4657 | 1.257 | 5.893e+05 | 0.09474 | 99 | narrow J=8->8 optical pumping / demagnetization cooling l… |
| 5I8 – 5K°9 | 740.9640 | 740.7600 | 404.5979 | 0.207 | 1.120e+04 | 0.001782 | 100 | ultra-narrow-line MOT / narrow-line cooling in tweezers |
| 5I8 – 7I°9 | 1000.9034 | 1000.6291 | 299.5219 | 0.010 | 1.150e+01 | 1.825e-06 | 100 | ultra-narrow |
| 5I8 – 7H°8 | 1321.7705 | 1321.4091 | 226.8113 | 0.053* | 1.460e+02 | 2.307e-05 | 100 | proposed ultra-narrow telecom-band line |
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).
161Dy hyperfine structure (I = 5/2)
| Level | A (MHz) | B (MHz) | Shift of each F level from the centre of gravity (MHz) |
|---|---|---|---|
| 5I8 | -116.2310(20) | 1091.58(5) | F=11/2: +3004.07 F=13/2: +1911.55 F=15/2: +794.21 F=17/2: -286.54 F=19/2: -1261.11 F=21/2: -2051.73 |
| 5K°9 | -102.090(20) | 3883.0(10) | F=13/2: +3884.65 F=15/2: +1919.82 F=17/2: +210.73 F=19/2: -1048.44 F=21/2: -1640.72 F=23/2: -1326.28 |
| 5I°8 | -108.840(20) | 2251.0(10) | F=11/2: +3250.82 F=13/2: +1848.36 F=15/2: +525.59 F=17/2: -590.89 F=19/2: -1357.56 F=21/2: -1614.05 |
| (8,1)°9 | -187.000 | -317.000 | F=13/2: +4566.23 F=15/2: +3261.62 F=17/2: +1740.81 F=19/2: -12.07 F=21/2: -2014.73 F=23/2: -4286.75 |
| (8,1)°7 | -64.286(17) | 892.2(9) | F=9/2: +1619.07 F=11/2: +990.48 F=13/2: +362.32 F=15/2: -208.06 F=17/2: -654.49 F=19/2: -901.96 |
| (8,2)°9 | -148.004(13) | 1561.0(9) | F=13/2: +4235.74 F=15/2: +2643.63 F=17/2: +1047.38 F=19/2: -474.96 F=21/2: -1836.18 F=23/2: -2939.84 |
| (8,1)°9 | -86.900(20) | 1747.4(5) | F=13/2: +2772.10 F=15/2: +1580.71 F=17/2: +463.46 F=19/2: -492.29 F=21/2: -1188.89 F=23/2: -1518.40 |
| (26868)°8 | -78.7(17) | 1513(58) | F=11/2: +2309.76 F=13/2: +1331.07 F=15/2: +400.39 F=17/2: -397.16 F=19/2: -965.14 F=21/2: -1195.75 |
Measured A, B constants; sources in the data file.
Isotope shifts
| Transition | λ vac (nm) | Isotopes | Shift (MHz) |
|---|---|---|---|
| 5I8 – (26868)°8 | 372.189 | 164-163 | -44(10) |
| 5I8 – (26868)°8 | 372.189 | 164-162 | -178(13) |
| 5I8 – (26868)°8 | 372.189 | 164-161 | -194(13) |
| 5I8 – (26868)°8 | 372.189 | 164-160 | -339(13) |
| 5I8 – (8,1)°9 | 421.290 | 164-163 | -616.3(5) |
| 5I8 – (8,1)°9 | 421.290 | 164-162 | -913.2(8) |
| 5I8 – (8,1)°9 | 421.290 | 164-161 | -1635.0(10) |
| 5I8 – (8,1)°9 | 421.290 | 164-160 | -1895.0(20) |
| 5I8 – (8,1)°9 | 421.290 | 164-158 | -2868(9) |
| 5I8 – (8,1)°9 | 421.290 | 164-156 | -4300(15) |
| 5I8 – (7,2)°8 | 456.637 | 164-163 | -660(3) |
| 5I8 – (7,2)°8 | 456.637 | 164-162 | -971.0(20) |
| 5I8 – (7,2)°8 | 456.637 | 164-161 | -1744(3) |
| 5I8 – (7,2)°8 | 456.637 | 164-160 | -2020(3) |
| 5I8 – (7,2)°8 | 456.637 | 164-158 | -3061(4) |
| 5I8 – (7,2)°8 | 456.637 | 164-156 | -4604(5) |
| 5I8 – (8,2)°9 | 564.106 | 164-163 | -685.0(20) |
| 5I8 – (8,2)°9 | 564.106 | 163-162 | -328(3) |
| 5I8 – (8,2)°9 | 564.106 | 162-161 | -801(3) |
| 5I8 – (8,2)°9 | 564.106 | 161-160 | -284.0(20) |
| 5I8 – (8,2)°9 | 564.106 | 164-162 | -1012.0(20) |
| 5I8 – (8,2)°9 | 564.106 | 162-160 | -1086(5) |
Shift = ν(first isotope) − ν(second isotope).
Closed and nearly closed transitions of 161Dy
| Transition | λ vacuum (nm) | Lower level | A (s⁻¹) | Leak per scattered photon | Photons before a leak | Where the leak goes |
|---|---|---|---|---|---|---|
| 5I8 → (8,1)°9 | 626.0819 | ground | 8.900e+05 NIST | closed | – | no other level can be reached by electric-dipole decay |
| 5I8 → 7K°9 | 598.1652 | ground | 7.700e+04 theory | closed | – | no other level can be reached by electric-dipole decay |
| 5I8 → 5K°9 | 740.9640 | ground | 1.120e+04 measured | closed | – | no other level can be reached by electric-dipole decay |
| 5I8 → 7I°9 | 1000.9034 | ground | 1.150e+01 measured | closed | – | no other level can be reached by electric-dipole decay |
| 5I8 → (8,1)°9 | 421.2902 | ground | 2.000e+08 measured | 7 × 10−6 from measured data | 143,000 | 3[8]9 2.08 × 10−5*; 3[9]10 1.89 × 10−5*; 3[10]10 6.82 × 10−6*; 10 weaker lines; the listed lines add up to 6.09 × 10−5* |
| 5I8 → 7H°8 | 1321.7705 | ground | 1.460e+02 theory | 9.38 × 10−5 from theory | 10,700 | 5I7 9.38 × 10−5* (long-lived) |
| 5I8 → 5I°8 | 683.7308 | ground | 5.893e+05 measured | 1 % from measured data | 100 | 5I7 1 % (long-lived) |
| 5I8 → (8,2)°8 | 554.8808 | ground | 3.000e+05 NIST | ≥ 2.12 % from measured data | ≤ 47 | 5I7 2.12 % (long-lived); 2 more possible paths without a listed rate |
| 5I7 → 5I°6 | 608.9946 | metastable | 1.460e+06 NIST | ≥ 2.72 % from measured data | ≤ 37 | 5I6 2.72 % (long-lived); 3 more possible paths without a listed rate |
| 5I8 → (8,1)°8 | 597.6143 | ground | 4.200e+05 NIST | 3.11 % from measured data | 32 | 5I7 3.11 % (long-lived) |
| 5I8 → (18857)°7 | 530.3059 | ground | 8.500e+05 NIST | ≥ 3.28 % from measured data | ≤ 30 | 5I7 3.28 % (long-lived); 3 more possible paths without a listed rate |
| 5I8 → 5H°7 | 658.1186 | ground | 7.700e+05 NIST | ≥ 5.29 % from measured data | ≤ 19 | 5I7 5.29 % (long-lived); 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.
All 161Dy 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 |
|---|---|---|---|---|---|---|---|---|---|
| 5I8 | (26868)°8 | 372.1890 | 372.0832 | 805.4845 | E1 | – | – | – | – |
| 5I8 | (25012)°8 | 399.8047 | 399.6917 | 749.8472 | E1 | 0.445 measured | 3.700e+05 measured | 77.3 | Li, Wyart, Dulieu, Nascimbene, Lepers, J. Phys. B 50 (2017), arXiv:1607.05628, Tables 3-4… |
| 5I8 | (6,2)°8 | 400.0067 | 399.8936 | 749.4686 | E1 | 0.296 measured | 1.630e+05 measured | 12.3 | Li, Wyart, Dulieu, Nascimbene, Lepers, J. Phys. B 50 (2017), arXiv:1607.05628, Tables 3-4… |
| 5I8 | (6,2)°7 | 401.4958 | 401.3823 | 746.6889 | E1 | 1.185 NIST | 2.930e+06 NIST | 91.7 | NIST ASD (accuracy B+) |
| 5I8 | (8,1)°7 | 404.7113 | 404.5970 | 740.7563 | E1 | 9.707 NIST | 1.920e+08 NIST | 99.8 | NIST ASD (accuracy B+) |
| 5I8 | (24229)°9 | 412.7248 | 412.6084 | 726.3737 | E1 | 0.779 measured | 9.200e+05 measured | 100 | Li, Wyart, Dulieu, Nascimbene, Lepers, J. Phys. B 50 (2017), arXiv:1607.05628, Tables 3-4… |
| 5I8 | (24204)°8 | 413.1516 | 413.0351 | 725.6234 | E1 | 1.020 NIST | 1.760e+06 NIST | 100 | NIST ASD (accuracy B+) |
| 5I8 | (8,1)°8 | 418.8001 | 418.6821 | 715.8366 | E1 | 8.812 NIST | 1.260e+08 NIST | 99.5 | NIST ASD (accuracy B+) |
| 5I8 | (23832)°8 | 419.6028 | 419.4846 | 714.4672 | E1 | 7.386 NIST | 8.800e+07 NIST | 100 | NIST ASD (accuracy B+) |
| 5I8 | (8,1)°9 | 421.2902 | 421.1715 | 711.6057 | E1 | 11.84 measured | 2.000e+08 measured | 100 | Lu, Youn, Lev, Phys. Rev. A 83, 012510 (2011) |
| 5I8 | (7,2)°8 | 456.6373 | 456.5093 | 656.5221 | E1 | 0.726 NIST | 6.600e+05 NIST | 79.9 | NIST ASD (accuracy B+) |
| 5I8 | (7,2)°9 | 457.9059 | 457.7776 | 654.7033 | E1 | 1.328 NIST | 1.960e+06 NIST | 100 | NIST ASD (accuracy B+) |
| 5I8 | 5K°7 | 459.0650 | 458.9364 | 653.0501 | E1 | 3.132 NIST | 1.370e+07 NIST | 99.6 | NIST ASD (accuracy B+) |
| 5I8 | 5H°7 | 461.3551 | 461.2259 | 649.8085 | E1 | 2.442 NIST | 8.200e+06 NIST | 98.4 | NIST ASD (accuracy B+) |
| 5I7 | (25012)°8 | 478.9734 | 478.8395 | 625.9063 | E1 | 0.316 measured | 1.080e+05 measured | 22.6 | Li, Wyart, Dulieu, Nascimbene, Lepers, J. Phys. B 50 (2017), arXiv:1607.05628, Tables 3-4… |
| 5I7 | (6,2)°8 | 479.2633 | 479.1293 | 625.5277 | E1 | 1.035 NIST | 1.160e+06 NIST | 87.6 | NIST ASD (accuracy B+) |
| 5I7 | (6,2)°7 | 481.4025 | 481.2680 | 622.7480 | E1 | 1.460 measured | 2.580e+06 measured | 80.8 | Li, Wyart, Dulieu, Nascimbene, Lepers, J. Phys. B 50 (2017), arXiv:1607.05628, Tables 3-4… |
| 5I7 | (8,1)°7 | 486.0327 | 485.8969 | 616.8155 | E1 | 0.469 measured | 2.590e+05 measured | 0.135 | Li, Wyart, Dulieu, Nascimbene, Lepers, J. Phys. B 50 (2017), arXiv:1607.05628, Tables 3-4… |
| 5I8 | 7G°7 | 488.1525 | 488.0162 | 614.1368 | E1 (intercombination) | 0.669 NIST | 5.200e+05 NIST | 90 | NIST ASD (accuracy B+) |
| 5I7 | 5H°6 | 502.3518 | 502.2117 | 596.7779 | E1 | 1.016 NIST | 1.270e+06 NIST | 94.9 | NIST ASD (accuracy B+) |
| 5I8 | 5K°8 | 507.9083 | 507.7667 | 590.2492 | E1 | 0.671 NIST | 4.100e+05 NIST | 90.6 | NIST ASD (accuracy B) |
| 5I8 | (18857)°7 | 530.3059 | 530.1584 | 565.3198 | E1 | 0.969 NIST | 8.500e+05 NIST | 96 | NIST ASD (accuracy B+) |
| 5I8 | (8,2)°8 | 554.8808 | 554.7267 | 540.2827 | E1 | 0.656 NIST | 3.000e+05 NIST | 97.8 | NIST ASD (accuracy B) |
| 5I7 | (7,2)°8 | 562.9047 | 562.7484 | 532.5812 | E1 | 0.498 NIST | 1.660e+05 NIST | 20.1 | NIST ASD (accuracy B+) |
| 5I8 | (8,2)°9 | 564.1065 | 563.9499 | 531.4466 | E1 (intercombination) | 0.908 NIST | 4.900e+05 NIST | 100 | NIST ASD (accuracy B) |
| 5I8 | 7K°7 | 565.3582 | 565.2014 | 530.2699 | E1 (intercombination) | 0.772 NIST | 4.460e+05 NIST | 79.8 | NIST ASD (accuracy B+) |
| 5I7 | 5K°7 | 566.5984 | 566.4412 | 529.1093 | E1 | 0.211 measured | 3.300e+04 measured | 0.24 | Li, Wyart, Dulieu, Nascimbene, Lepers, J. Phys. B 50 (2017), arXiv:1607.05628, Tables 3-4… |
| 5I7 | 5H°7 | 570.0910 | 569.9329 | 525.8677 | E1 | 0.479 measured | 1.670e+05 measured | 2 | Li, Wyart, Dulieu, Nascimbene, Lepers, J. Phys. B 50 (2017), arXiv:1607.05628, Tables 3-4… |
| 5I6 | 5H°6 | 588.5820 | 588.4189 | 509.3470 | E1 | 0.292 measured | 6.500e+04 measured | 4.86 | Li, Wyart, Dulieu, Nascimbene, Lepers, J. Phys. B 50 (2017), arXiv:1607.05628, Tables 3-4… |
| 5I8 | (8,1)°8 | 597.6143 | 597.4488 | 501.6487 | E1 | 0.867 NIST | 4.200e+05 NIST | 96.2 | NIST ASD (accuracy B) |
| 5I8 | 7K°9 | 598.1652 | 597.9995 | 501.1867 | E1 (intercombination) | 0.393 theory | 7.700e+04 theory | 100 | Lu, Youn, Lev, Phys. Rev. A 83, 012510 (2011) |
| 5I8 | (8,1)°7 | 599.0223 | 598.8564 | 500.4696 | E1 (intercombination) | 0.944 NIST | 5.600e+05 NIST | 99.7 | NIST ASD (accuracy B+) |
| 5I7 | (7,1)°7 | 601.2481 | 601.0817 | 498.6168 | E1 | 0.974 NIST | 5.900e+05 NIST | 90.9 | NIST ASD (accuracy B) |
| 5I7 | 5I°6 | 608.9946 | 608.8260 | 492.2745 | E1 | 1.455 NIST | 1.460e+06 NIST | 96.9 | NIST ASD (accuracy B+) |
| 5I7 | 7G°7 | 611.5767 | 611.4075 | 490.1960 | E1 (intercombination) | 0.311 measured | 5.700e+04 measured | 9.86 | Li, Wyart, Dulieu, Nascimbene, Lepers, J. Phys. B 50 (2017), arXiv:1607.05628, Tables 3-4… |
| 5I7 | (7,1)°8 | 617.0136 | 616.8429 | 485.8766 | E1 | 1.264 NIST | 8.100e+05 NIST | 89.1 | NIST ASD (accuracy B+) |
| 5I8 | (8,1)°9 | 626.0819 | 625.9088 | 478.8390 | E1 (intercombination) | 1.431 NIST | 8.900e+05 NIST | 100 | NIST ASD (accuracy B+) |
| 5I7 | 5K°8 | 642.9060 | 642.7284 | 466.3084 | E1 | 0.317 measured | 4.500e+04 measured | 9.95 | Li, Wyart, Dulieu, Nascimbene, Lepers, J. Phys. B 50 (2017), arXiv:1607.05628, Tables 3-4… |
| 5I8 | 5H°7 | 658.1186 | 657.9368 | 455.5295 | E1 | 1.275 NIST | 7.700e+05 NIST | 94.7 | NIST ASD (accuracy B) |
| 5I6 | 5K°7 | 678.7574 | 678.5701 | 441.6784 | E1 | 0.176 measured | 1.340e+04 measured | 0.0974 | Li, Wyart, Dulieu, Nascimbene, Lepers, J. Phys. B 50 (2017), arXiv:1607.05628, Tables 3-4… |
| 5I7 | (18857)°7 | 679.2178 | 679.0304 | 441.3790 | E1 | 0.259 measured | 2.900e+04 measured | 3.28 | Li, Wyart, Dulieu, Nascimbene, Lepers, J. Phys. B 50 (2017), arXiv:1607.05628, Tables 3-4… |
| 5I8 | 5I°8 | 683.7308 | 683.5421 | 438.4657 | E1 | 1.257 measured | 5.893e+05 measured | 99 | branching ratio / lifetime |
| 5I7 | (8,2)°8 | 720.0633 | 719.8649 | 416.3418 | E1 | 0.143 measured | 6.500e+03 measured | 2.12 | Li, Wyart, Dulieu, Nascimbene, Lepers, J. Phys. B 50 (2017), arXiv:1607.05628, Tables 3-4… |
| 5I6 | (7,1)°7 | 729.0922 | 728.8913 | 411.1859 | E1 | 0.288 measured | 2.900e+04 measured | 4.47 | Li, Wyart, Dulieu, Nascimbene, Lepers, J. Phys. B 50 (2017), arXiv:1607.05628, Tables 3-4… |
| 5I7 | 7K°7 | 737.8071 | 737.6039 | 406.3290 | E1 (intercombination) | 0.572 NIST | 1.100e+05 NIST | 19.7 | NIST ASD (accuracy B+) |
| 5I6 | 5I°6 | 740.5144 | 740.3104 | 404.8435 | E1 | 0.327 measured | 4.100e+04 measured | 2.72 | Li, Wyart, Dulieu, Nascimbene, Lepers, J. Phys. B 50 (2017), arXiv:1607.05628, Tables 3-4… |
| 5I8 | 5K°9 | 740.9640 | 740.7600 | 404.5979 | E1 | 0.207 measured | 1.120e+04 measured | 100 | Lu, Youn, Lev, Phys. Rev. A 83, 012510 (2011) |
| 5I7 | (8,1)°8 | 793.7152 | 793.4969 | 377.7079 | E1 | 0.239 measured | 1.360e+04 measured | 3.11 | Li, Wyart, Dulieu, Nascimbene, Lepers, J. Phys. B 50 (2017), arXiv:1607.05628, Tables 3-4… |
| 5I7 | 5H°7 | 904.1094 | 903.8613 | 331.5887 | E1 | 0.485 measured | 4.300e+04 measured | 5.29 | Li, Wyart, Dulieu, Nascimbene, Lepers, J. Phys. B 50 (2017), arXiv:1607.05628, Tables 3-4… |
| 5I7 | 5I°8 | 953.1600 | 952.8986 | 314.5248 | E1 | 0.208 measured | 5.952e+03 measured | 1 | branching ratio / lifetime |
| 5I8 | 7I°9 | 1000.9034 | 1000.6291 | 299.5219 | E1 (intercombination) | 0.0104 measured | 1.150e+01 measured | 100 | Petersen, Truemper, Windpassinger, Phys. Rev. A 101, 042502 (2020) |
| 5I8 | 7H°8 | 1321.7705 | 1321.4091 | 226.8113 | E1 (intercombination) | 0.0532 theory | 1.460e+02 theory | 100 | Dzuba, Flambaum, Phys. Rev. A 81, 052515 (2010) |
| 3[8]9 | (8,1)°9 | 1607.1718 | 1606.7329 | 186.5342 | E1 | 0.411 theory | 4.340e+03 theory | 0.00208 | Dzuba, Flambaum, Phys. Rev. A 81, 052515 (2010) |
| 3[7]8 | (8,1)°9 | 1633.1197 | 1632.6736 | 183.5704 | E1 | 0.221 theory | 1.200e+03 theory | 0.000576 | Dzuba, Flambaum, Phys. Rev. A 81, 052515 (2010) |
| 3[9]10 | (8,1)°9 | 1896.1084 | 1895.5908 | 158.1093 | E1 | 0.502 theory | 3.940e+03 theory | 0.00189 | Dzuba, Flambaum, Phys. Rev. A 81, 052515 (2010) |
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.
161Dy energy levels
Dy⁺ ionisation limit 47901.76 cm⁻¹ = 5.93906 eV (208.761 nm)
Sources
- Curry, Den Hartog, Lawler, J. Opt. Soc. Am. B 14, 2788 (1997), Table 1
- Dzuba, Flambaum, Phys. Rev. A 81, 052515 (2010)
- Gustavsson, Lundberg, Nilsson, Svanberg, J. Opt. Soc. Am. 69, 984 (1979), Table II
- Leefer, Cingoz, Budker, Opt. Lett. 34, 2548 (2009)
- Li, Wyart, Dulieu, Nascimbene, Lepers, J. Phys. B 50 (2017), arXiv:1607.05628, Tables 3-4…
- Lu, Youn, Lev, Phys. Rev. A 83, 012510 (2011)
- NIST ASD
- NIST ASD level energies
- Ng et al., 'Two-dimensional shelving spectroscopy of ultraviolet ground state transitions…
- Petersen, Truemper, Windpassinger, Phys. Rev. A 101, 042502 (2020)
- Petersen, Truemper, Windpassinger, Phys. Rev. A 101, 042502 (2020). Note: LOWER LIMIT (ta…
- Petersen, Truemper, Windpassinger, Phys. Rev. A 101, 042502 (2020). Note: UPPER LIMIT, = …
- Schmitt, Henn, Billy, Kadau, Maier, Griesmaier, Pfau, Opt. Lett. 38, 637 (2013)
- T. Maier, PhD thesis, Univ. Stuttgart (2015), Tab. 2.2
- White, Bulstrode, Forest, Honeyball, Evans, Butt, J. Phys. B 58, 035001 (2025)
- branching ratio / lifetime
Isotope shifts are nu(first)-nu(second) as in the schema; where a source tabulated nu(A)-nu(164) the sign was flipped and this is stated in the entry note. Keys other than 164-x (e.g. 162-164 for Petersen et al., 163-162 for White et al.) are kept as printed. Extra fields beyond SCHEMA.md are used where the schema had no slot: top-level ionization_limit; level fields lifetime_other, hyperfine_other, level_energy_measured; transition fields linewidth_MHz / linewidth_kHz, wavenumber_cm, reduced_dipole_au (|<f||D||i>| in atomic units, theory), leak_to_metastable, isotope_shift_other, frequency_other, polarizability_ratio_1064nm, note. Entries flagged LOWER LIMIT / UPPER LIMIT / LOWER BOUND in their note are bounds, not central values. g_J values are copied from the NIST levels file (Lande column). Hyperfine A, B follow the usual convention E = A K/2 + B [3K(K+1)/4 - I(I+1)J(J+1)] / [2I(2I-1)J(2J-1)], K = F(F+1)-I(I+1)-J(J+1); 161Dy has negative A (inverted structure). The Curry 1997 and Gustavsson 1979 lifetime tables were read from the publisher HTML pages through an automated page reader (direct download is captcha-blocked), not from a PDF; the Curry values were spot-checked against 1/sum(A) from the NIST lines file for 15194.83, 15972.35, 16693.87, 16733.20, 23832.06, 23877.74 and 24708.97 cm-1 and agree. Curry uncertainties are the blanket +-5% (+-10% or +-8% where flagged). Rows of Curry Table 1 above 28200 cm-1 were not transcribed, and levels the reader may have skipped a
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-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