Caesium-133 energy level diagram
Energy levels and transitions of neutral 133Cs (Cs I, nuclear spin I = 7/2): 31 levels and 79 lines below 2 µm, each with its vacuum wavelength, frequency and, for 75 of them, the reduced dipole matrix element. Level energies come from the NIST Atomic Spectra Database; transition rates are 60 theory, 9 measured, 7 NIST.
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Download: diagram (PDF) diagram (SVG) transitions (CSV) levels (CSV) source code
Key transitions of 133Cs
| Transition | λ vac (nm) | λ air (nm) | ν (THz) | ν̃ (cm⁻¹) | |⟨J‖er‖J′⟩| (ea₀) | A (s⁻¹) | Γ/2π up. (MHz) | branch (%) | Typical use |
|---|---|---|---|---|---|---|---|---|---|
| 6S1/2 – 6P3/2 | 852.3473 | 852.1132 | 351.7257 | 11732.307 | 6.335 | 3.283e+07 | 5.225 | 100.0 | D2: MOT, imaging |
| 6S1/2 – 6P1/2 | 894.5930 | 894.3474 | 335.1160 | 11178.268 | 4.498 | 2.863e+07 | 4.556 | 100.0 | D1: optical pumping, Λ / gray-molasses cooling |
| 6S1/2 – 7P3/2 | 455.6557 | 455.5280 | 657.9364 | 21946.397 | 0.574 | 1.765e+06 | 1.157 | 23.1 | blue leg of 456 + 1038 Rydberg excitation |
| 6S1/2 – 7P1/2 | 459.4459 | 459.3172 | 652.5087 | 21765.348 | 0.278 | 8.079e+05 | 0.963 | 12.5 | blue leg (459 + 1040) |
| 6P3/2 – 6D5/2 | 917.4834 | 917.2317 | 326.7552 | 10899.379 | 6.128* | 1.642e+07 | 2.622 | 99.6 | 852 + 917 ladder |
| 6P3/2 – 8S1/2 | 794.6067 | 794.3882 | 377.2841 | 12584.842 | 1.455* | 4.275e+06 | 1.829 | 39.6 | 852 + 795 ladder |
| 6P3/2 – 7S1/2 | 1469.8919 | 1469.4902 | 203.9555 | 6803.221 | 6.489 | 1.343e+07 | 3.296 | 64.8 | telecom E-band ladder; 6S–7S parity-violation line at 539.5 nm ×2 |
| 6P1/2 – 7S1/2 | 1359.2016 | 1358.8300 | 220.5651 | 7357.260 | 4.249 | 7.284e+06 | 3.296 | 35.2 | telecom O-band ladder |
| 6P3/2 – 7D5/2 | 697.5220 | 697.3296 | 429.7964 | 14336.466 | 2.893* | 8.328e+06 | 1.788 | 76.5 | 852 + 698 ladder |
| 5D5/2 – 7P3/2 | 1360.6267 | 1360.2547 | 220.3341 | 7349.555 | 2.480 | 1.237e+06 | 1.157 | 20.8 | from 5D |
| 5D5/2 – 4F7/2 | 1012.6374 | 1012.3599 | 296.0511 | 9875.203 | 8.630* | 1.817e+07 | 3.979 | 93.2 | 1.01 µm, from 5D |
| 6P1/2 – 6D3/2 | 876.3817 | 876.1411 | 342.0798 | 11410.553 | 4.235* | 1.350e+07 | 2.653 | 82.1 | 895 + 876 ladder |
| 6P3/2 – 9S1/2 | 658.8329 | 658.6510 | 455.0356 | 15178.356 | 0.766* | 2.076e+06 | 1.001 | 34.7 | 852 + 659 ladder |
| 6P3/2 – 8D5/2 | 621.4819 | 621.3100 | 482.3832 | 16090.573 | 1.807* | 4.594e+06 | 1.098 | 67.1 | 852 + 621 ladder |
λ and ν from NIST level energies (centre of gravity, no hyperfine structure); λ air uses standard air (Ciddor). Γ/2π: natural linewidth of the upper level, 1/(2πτ). Branch: share of the upper level's decays that takes this line.
Rydberg excitation wavelengths (vacuum, nm)
| Lower → series | n = 30 | n = 40 | n = 50 | n = 70 | n = 100 | n → ∞ | d₇₀ ARC |
|---|---|---|---|---|---|---|---|
| 6S1/2 → nP3/2 | 320.005 | 319.246 | 318.922 | 318.658 | 318.525 | 318.406 | 0.0030 |
| 6P1/2 → nS1/2 | 498.374 | 496.443 | 495.633 | 494.977 | 494.651 | 494.359 | 0.0077 |
| 6P1/2 → nD3/2 | 497.925 | 496.271 | 495.550 | 494.948 | 494.642 | 494.359 | 0.0230 |
| 6P3/2 → nS1/2 | 512.526 | 510.484 | 509.627 | 508.934 | 508.589 | 508.281 | 0.0108 |
| 6P3/2 → nD5/2 | 512.048 | 510.301 | 509.539 | 508.903 | 508.579 | 508.281 | 0.0316 |
| 5D3/2 → nP3/2 | 597.006 | 594.369 | 593.249 | 592.335 | 591.877 | 591.464 | 0.0015 |
| 5D3/2 → nF5/2 | 595.770 | 593.877 | 593.005 | 592.249 | 591.848 | 591.464 | 0.0491 |
| 5D5/2 → nP3/2 | 600.505 | 597.836 | 596.703 | 595.778 | 595.315 | 594.897 | 0.0047 |
| 5D5/2 → nF7/2 | 599.254 | 597.339 | 596.457 | 595.692 | 595.286 | 594.897 | 0.0589 |
| 7S1/2 → nP3/2 | 786.536 | 781.965 | 780.028 | 778.448 | 777.657 | 776.944 | 0.0071 |
| 7P1/2 → nS1/2 | 1055.057 | 1046.440 | 1042.846 | 1039.945 | 1038.508 | 1037.224 | 0.0145 |
| 7P1/2 → nD3/2 | 1053.045 | 1045.677 | 1042.478 | 1039.820 | 1038.467 | 1037.224 | 0.0392 |
| 7P3/2 → nS1/2 | 1075.602 | 1066.648 | 1062.914 | 1059.901 | 1058.408 | 1057.075 | 0.0197 |
| 7P3/2 → nD5/2 | 1073.501 | 1065.851 | 1062.530 | 1059.770 | 1058.365 | 1057.075 | 0.0542 |
| 6D5/2 → nP3/2 | 1160.387 | 1150.464 | 1146.276 | 1142.867 | 1141.164 | 1139.630 | 0.0160 |
| 6D5/2 → nF7/2 | 1155.724 | 1148.622 | 1145.367 | 1142.548 | 1141.057 | 1139.630 | 0.0649 |
| 8S1/2 → nP3/2 | 1442.513 | 1427.209 | 1420.770 | 1415.536 | 1412.924 | 1410.573 | 0.0131 |
| 4F7/2 → nD5/2 | 1472.826 | 1458.464 | 1452.253 | 1447.102 | 1444.484 | 1442.081 | 0.0181 |
Rydberg term energies from ARC quantum defects + NIST ionisation limit, lower level from NIST. d₇₀ = |⟨J‖er‖J′⟩| to n = 70 in ea₀ (calculated). S → nP values come from a near-cancelling integral: treat them as an order of magnitude.
133Cs hyperfine structure (I = 7/2)
| Level | A (MHz) | B (MHz) | Shift of each F level from the centre of gravity (MHz) |
|---|---|---|---|
| 6S1/2 | 2298.158 | – | F=3: -5170.85 F=4: +4021.78 |
| 6P1/2 | 291.9263(25) | – | F=3: -656.83 F=4: +510.87 |
| 6P3/2 | 50.2878(11) | -0.496(6) | F=2: -339.71 F=3: -188.49 F=4: +12.80 F=5: +263.89 |
| 5D3/2 | 48.78(7) | 0.1(7) | F=2: -329.21 F=3: -182.94 F=4: +12.15 F=5: +256.12 |
| 5D5/2 | -21.24(5) | 0.2(5) | F=1: +239.06 F=2: +196.52 F=3: +132.74 F=4: +47.73 F=5: -58.46 F=6: -185.80 |
| 7S1/2 | 545.856(14) | – | F=3: -1228.18 F=4: +955.25 |
| 7P1/2 | 94.37(3) | – | F=3: -212.33 F=4: +165.15 |
| 7P3/2 | 16.605(4) | -0.16(3) | F=2: -112.17 F=3: -62.24 F=4: +4.23 F=5: +87.14 |
| 6D3/2 | 16.338(3) | -0.136(24) | F=2: -110.35 F=3: -61.24 F=4: +4.15 F=5: +85.74 |
| 6D5/2 | -4.629(11) | -0.10(15) | F=1: +52.02 F=2: +42.79 F=3: +28.94 F=4: +10.45 F=5: -12.70 F=6: -40.53 |
| 8S1/2 | 219.125(3) | – | F=3: -493.03 F=4: +383.47 |
| 8P1/2 | 42.96(9) | – | F=3: -96.66 F=4: +75.18 |
| 8P3/2 | 7.58(3) | -0.14(5) | F=2: -51.24 F=3: -28.40 F=4: +1.96 F=5: +39.76 |
| 7D3/2 | 7.380(8) | -0.17(7) | F=2: -49.91 F=3: -27.64 F=4: +1.92 F=5: +38.70 |
| 7D5/2 | -1.717(15) | -0.2(5) | F=1: +19.22 F=2: +15.84 F=3: +10.74 F=4: +3.92 F=5: -4.67 F=6: -15.07 |
| 8D3/2 | 3.950(10) | – | F=2: -26.66 F=3: -14.81 F=4: +0.99 F=5: +20.74 |
| 8D5/2 | -0.85(20) | – | F=1: +9.56 F=2: +7.86 F=3: +5.31 F=4: +1.91 F=5: -2.34 F=6: -7.44 |
A, B: magnetic-dipole and electric-quadrupole constants (measured; see data file for sources).
Closed and nearly closed transitions of 133Cs
| Transition | λ vacuum (nm) | Lower level | A (s⁻¹) | Leak per scattered photon | Photons before a leak | Where the leak goes |
|---|---|---|---|---|---|---|
| 6S1/2 → 6P3/2 | 852.3473 | ground | 3.283e+07 measured | closed | – | no other level can be reached by electric-dipole decay |
| 6S1/2 → 6P1/2 | 894.5930 | ground | 2.863e+07 measured | closed | – | no other level can be reached by electric-dipole decay |
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 133Cs transitions below 2 µm
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.
133Cs energy levels
Cs⁺ ionisation limit 31406.47 cm⁻¹ = 3.89391 eV = 941.542 THz (318.406 nm)
Sources
- ARC model potential
- Allegrini, Arimondo, Orozco, J. Phys. Chem. Ref. Data 51, 043102 (2022), Table VII; origi…
- Allegrini, Arimondo, Orozco, J. Phys. Chem. Ref. Data 51, 043102 (2022), Table VII; origi…
- Allegrini, Arimondo, Orozco, J. Phys. Chem. Ref. Data 51, 043102 (2022), Table VII; origi…
- Allegrini, Arimondo, Orozco, J. Phys. Chem. Ref. Data 51, 043102 (2022), Table VII; origi…
- Allegrini, Arimondo, Orozco, J. Phys. Chem. Ref. Data 51, 043102 (2022), Table VII; origi…
- Allegrini, Arimondo, Orozco, J. Phys. Chem. Ref. Data 51, 043102 (2022), Table VII; origi…
- Allegrini, Arimondo, Orozco, J. Phys. Chem. Ref. Data 51, 043102 (2022), Table VII; origi…
- Allegrini, Arimondo, Orozco, J. Phys. Chem. Ref. Data 51, 043102 (2022), Table VII; origi…
- Allegrini, Arimondo, Orozco, J. Phys. Chem. Ref. Data 51, 043102 (2022), Table VII; origi…
- Allegrini, Arimondo, Orozco, J. Phys. Chem. Ref. Data 51, 043102 (2022), Table VII; origi…
- Allegrini, Arimondo, Orozco, J. Phys. Chem. Ref. Data 51, 043102 (2022), Table VII; origi…
- Allegrini, Arimondo, Orozco, J. Phys. Chem. Ref. Data 51, 043102 (2022), Table VII; origi…
- Allegrini, Arimondo, Orozco, J. Phys. Chem. Ref. Data 51, 043102 (2022), Table VII; origi…
- Allegrini, Arimondo, Orozco, J. Phys. Chem. Ref. Data 51, 043102 (2022), Table VII; origi…
- Allegrini, Arimondo, Orozco, J. Phys. Chem. Ref. Data 51, 043102 (2022), Table VII; origi…
- Allegrini, Arimondo, Orozco, J. Phys. Chem. Ref. Data 51, 043102 (2022), Table VII; origi…
- Allegrini, Arimondo, Orozco, J. Phys. Chem. Ref. Data 51, 043102 (2022), Table VII; origi…
- Allegrini, Arimondo, Orozco, J. Phys. Chem. Ref. Data 51, 043102 (2022), Table VII; origi…
- Allegrini, Arimondo, Orozco, J. Phys. Chem. Ref. Data 51, 043102 (2022), Table VII; origi…
- Allegrini, Arimondo, Orozco, J. Phys. Chem. Ref. Data 51, 043102 (2022), Table VII; origi…
- Allegrini, Arimondo, Orozco, J. Phys. Chem. Ref. Data 51, 043102 (2022), Table VII; origi…
- Damitz, Toh, Putney, Tanner, Elliott, Phys. Rev. A 99, 062510 (2019)
- NIST ASD
- NIST ASD A = 1.43e+05 s^-1
- NIST ASD A = 2.2e+04 s^-1
- NIST ASD A = 3.9e+05 s^-1
- NIST ASD A = 6.3e+03 s^-1
- NIST ASD A = 6.3e+04 s^-1
- NIST ASD A = 9e+04 s^-1
- NIST ASD level energies
- Patterson, Sell, Ehrenreich, Gearba, Brooke, Scoville, Knize, Phys. Rev. A 91, 012506 (20…
- Pucher, Schneeweiss, Rauschenbeutel, Dareau, Phys. Rev. A 101, 042510 (2020)
- Safronova, Safronova, Clark, Phys. Rev. A 94, 012505 (2016), Table II, column "Recomm." (…
- Safronova, Safronova, Clark, Phys. Rev. A 94, 012505 (2016), Table II; original: DiBerard…
- Safronova, Safronova, Clark, Phys. Rev. A 94, 012505 (2016), Table II; original: Marek & …
- Safronova, Safronova, Clark, Phys. Rev. A 94, 012505 (2016), Table II; original: Marek & …
- Safronova, Safronova, Clark, Phys. Rev. A 94, 012505 (2016), Table II; original: Marek, J…
- Safronova, Safronova, Clark, Phys. Rev. A 94, 012505 (2016), Table II; original: Marek, P…
- Safronova, Safronova, Clark, Phys. Rev. A 94, 012505 (2016), Table II; original: Neil & A…
- Safronova, Safronova, Clark, Phys. Rev. A 94, 012505 (2016), Table II; original: Sieradza…
- Steck, Cesium D Line Data, rev. 2.3.4 (8 Aug 2025), Table 3 (hyperfine centre of gravity;…
- Steck, Cesium D Line Data, rev. 2.3.4 (8 Aug 2025), Table 4 (hyperfine centre of gravity;…
- Steck, Cesium D Line Data, rev. 2.3.4 (8 Aug 2025), Table 5 (exact: follows from the SI d…
- Toh, Chalus, Burgess, Damitz, Imany, Leaird, Weiner, Tanner, Elliott, Phys. Rev. A 100, 0…
- Toh, Chalus, Burgess, Damitz, Imany, Leaird, Weiner, Tanner, Elliott, Phys. Rev. A 100, 0…
- Toh, Chalus, Burgess, Damitz, Imany, Leaird, Weiner, Tanner, Elliott, Phys. Rev. A 100, 0…
- Toh, Damitz, Glotzbach, Quirk, Stevenson, Choi, Safronova, Elliott, Phys. Rev. A 99, 0325…
- Toh, Jaramillo-Villegas, Glotzbach, Quirk, Stevenson, Choi, Weiner, Elliott, Phys. Rev. A…
- UDel Portal for High-Precision Atomic Data and Computation (Safronova group), read 2026-1…
- UDel Portal for High-Precision Atomic Data and Computation (Safronova group), read 2026-1…
- UDel Portal for High-Precision Atomic Data and Computation (Safronova group), read 2026-1…
- UDel Portal for High-Precision Atomic Data and Computation (Safronova group), read 2026-1…
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
- 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