Rubidium-85 energy level diagram
Energy levels and transitions of neutral 85Rb (Rb I, nuclear spin I = 5/2): 36 levels and 94 lines below 2 µm, each with its vacuum wavelength, frequency and, for 92 of them, the reduced dipole matrix element. Level energies come from the NIST Atomic Spectra Database; transition rates are 77 theory, 11 NIST, 4 measured.
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Download: diagram (PDF) diagram (SVG) transitions (CSV) levels (CSV) source code
Key transitions of 85Rb
| 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 |
|---|---|---|---|---|---|---|---|---|---|
| 5S1/2 – 5P3/2 | 780.2414 | 780.0267 | 384.2304 | 12816.547 | 5.978 | 3.811e+07 | 6.065 | 100.0 | D2: MOT, imaging, Rydberg lower leg |
| 5S1/2 – 5P1/2 | 794.9790 | 794.7604 | 377.1074 | 12578.948 | 4.231 | 3.610e+07 | 5.746 | 100.0 | D1: optical pumping, Λ / gray-molasses cooling |
| 5S1/2 – 6P3/2 | 420.2989 | 420.1805 | 713.2839 | 23792.591 | 0.523 | 1.866e+06 | 1.421 | 21.1 | blue leg of 420 + 1013 Rydberg excitation |
| 5S1/2 – 6P1/2 | 421.6726 | 421.5539 | 710.9602 | 23715.081 | 0.324 | 1.414e+06 | 1.273 | 17.4 | blue leg (421 + 1005) |
| 5P3/2 – 5D5/2 | 775.9786 | 775.7651 | 386.3411 | 12886.953 | 1.980* | 2.833e+06 | 0.667 | 66.8 | 780 + 776 ladder; 5S–5D two-photon at 778.1 nm |
| 5P1/2 – 5D3/2 | 762.1030 | 761.8932 | 393.3752 | 13121.586 | 1.353* | 2.095e+06 | 0.646 | 51.0 | 795 + 762 ladder |
| 5P3/2 – 4D5/2 | 1529.3658 | 1528.9480 | 196.0240 | 6538.658 | 10.86* | 1.114e+07 | 1.693 | 100.0 | telecom C-band ladder |
| 5P3/2 – 4D3/2 | 1529.2615 | 1528.8437 | 196.0374 | 6539.104 | 3.618* | 1.854e+06 | 1.851 | 15.5 | telecom C-band ladder |
| 5P1/2 – 4D3/2 | 1475.6447 | 1475.2415 | 203.1603 | 6776.699 | 8.016* | 1.013e+07 | 1.851 | 84.5 | telecom S-band ladder |
| 5P3/2 – 6S1/2 | 1366.8737 | 1366.5000 | 219.3271 | 7315.965 | 6.048* | 1.451e+07 | 3.493 | 65.9 | telecom E-band ladder |
| 5P1/2 – 6S1/2 | 1323.8791 | 1323.5171 | 226.4500 | 7553.560 | 4.146* | 7.506e+06 | 3.493 | 34.1 | telecom O-band ladder |
| 5P3/2 – 6D5/2 | 630.0068 | 629.8326 | 475.8559 | 15872.845 | 1.658 | 3.712e+06 | 0.639 | 77.9 | red ladder |
| 5P3/2 – 7S1/2 | 741.0211 | 740.8171 | 404.5667 | 13494.892 | 1.350* | 4.536e+06 | 1.807 | 40.0 | ladder to 7S |
| 6S1/2 – 7P3/2 | 1292.3904 | 1292.0370 | 231.9674 | 7737.600 | 1.540* | 5.565e+05 | 0.647 | 14.2 | O-band, from 6S |
| 4D5/2 – 4F7/2 | 1344.6483 | 1344.2807 | 222.9523 | 7436.889 | 12.56* | 1.643e+07 | 2.618 | 98.2 | strongest line of the diagram |
| 6P3/2 – 7D5/2 | 1541.0626 | 1540.6416 | 194.5362 | 6489.029 | 1.929* | 3.433e+05 | 0.490 | 11.5 | telecom C-band, from 6P |
| 6P3/2 – 8S1/2 | 1903.2303 | 1902.7107 | 157.5177 | 5254.225 | 2.598* | 9.918e+05 | 0.989 | 16.0 | longest 6P line below 2 µm |
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 pairint. | d₇₀ ARC |
|---|---|---|---|---|---|---|---|---|
| 5S1/2 → nP3/2 | 298.113 | 297.510 | 297.247 | 297.029 | 296.918 | 296.817 | 0.0013 | 0.0023 |
| 5P1/2 → nS1/2 | 477.099 | 475.483 | 474.788 | 474.216 | 473.927 | 473.667 | 0.0067 | 0.0067 |
| 5P1/2 → nD3/2 | 476.682 | 475.318 | 474.707 | 474.187 | 473.917 | 473.667 | 0.0173 | 0.0166 |
| 5P3/2 → nS1/2 | 482.570 | 480.916 | 480.205 | 479.620 | 479.324 | 479.059 | 0.0093 | 0.0095 |
| 5P3/2 → nD5/2 | 482.143 | 480.747 | 480.122 | 479.591 | 479.315 | 479.059 | 0.0239 | 0.0230 |
| 4D5/2 → nP3/2 | 704.765 | 701.404 | 699.946 | 698.736 | 698.121 | 697.564 | 0.0100 | 0.0092 |
| 4D5/2 → nF7/2 | 703.548 | 700.913 | 699.701 | 698.649 | 698.092 | 697.564 | 0.0559 | 0.0582 |
| 6S1/2 → nP3/2 | 745.611 | 741.850 | 740.219 | 738.866 | 738.178 | 737.556 | 0.0055 | 0.0061 |
| 6P1/2 → nS1/2 | 1017.930 | 1010.598 | 1007.464 | 1004.891 | 1003.596 | 1002.433 | 0.0130 | 0.0130 |
| 6P1/2 → nD3/2 | 1016.033 | 1009.855 | 1007.100 | 1004.764 | 1003.554 | 1002.433 | 0.0258 | 0.0253 |
| 6P3/2 → nS1/2 | 1026.025 | 1018.576 | 1015.393 | 1012.780 | 1011.464 | 1010.283 | 0.0181 | 0.0181 |
| 6P3/2 → nD5/2 | 1024.097 | 1017.821 | 1015.023 | 1012.651 | 1011.421 | 1010.283 | 0.0361 | 0.0354 |
| 5D5/2 → nP3/2 | 1275.375 | 1264.411 | 1259.681 | 1255.767 | 1253.782 | 1251.986 | 0.0242 | 0.0236 |
| 5D5/2 → nF7/2 | 1271.394 | 1262.817 | 1258.887 | 1255.486 | 1253.687 | 1251.986 | 0.0834 | 0.0846 |
| 7S1/2 → nP3/2 | 1382.573 | 1369.698 | 1364.148 | 1359.560 | 1357.233 | 1355.129 | 0.0114 | 0.0118 |
| 4F7/2 → nD5/2 | 1478.152 | 1465.114 | 1459.322 | 1454.424 | 1451.889 | 1449.545 | 0.0186 | 0.0186 |
| 7P3/2 → nS1/2 | 1764.032 | 1742.128 | 1732.838 | 1725.240 | 1721.425 | 1718.006 | 0.0291 | 0.0291 |
| 7P3/2 → nD5/2 | 1758.339 | 1739.920 | 1731.758 | 1724.865 | 1721.300 | 1718.006 | 0.0491 | 0.0485 |
Rydberg term energies from pairinteraction, 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.
85Rb hyperfine structure (I = 5/2)
| Level | A (MHz) | B (MHz) | Shift of each F level from the centre of gravity (MHz) |
|---|---|---|---|
| 5S1/2 | 1011.910815 | – | F=2: -1770.84 F=3: +1264.89 |
| 5P1/2 | 120.605(29) | – | F=2: -211.06 F=3: +150.76 |
| 5P3/2 | 25.0401(11) | 26.000(22) | F=1: -113.26 F=2: -83.98 F=3: -20.56 F=4: +100.40 |
| 4D5/2 | -4.983(7) | 6.70(21) | F=0: +48.29 F=1: +41.70 F=2: +29.12 F=3: +11.76 F=4: -8.57 F=5: -29.47 |
| 4D3/2 | 7.33(4) | 4.52(23) | F=1: -35.31 F=2: -24.27 F=3: -4.32 F=4: +28.61 |
| 6S1/2 | 239.069(26) | – | F=2: -418.37 F=3: +298.84 |
| 6P1/2 | 39.122(9) | – | F=2: -68.46 F=3: +48.90 |
| 6P3/2 | 8.171(7) | 8.16(4) | F=1: -37.19 F=2: -27.37 F=3: -6.53 F=4: +32.68 |
| 5D3/2 | 4.26990(20) | 1.9106(8) | F=1: -21.08 F=2: -14.07 F=3: -2.12 F=4: +16.49 |
| 5D5/2 | -2.2112(12) | 2.680(20) | F=0: +21.22 F=1: +18.37 F=2: +12.90 F=3: +5.30 F=4: -3.70 F=5: -13.15 |
| 7S1/2 | 94.6813(15) | – | F=2: -165.69 F=3: +118.35 |
| 7P1/2 | 17.68(8) | – | F=2: -30.94 F=3: +22.10 |
| 7P3/2 | 3.710(10) | 3.68(8) | F=1: -16.90 F=2: -12.43 F=3: -2.95 F=4: +14.83 |
| 6D3/2 | 2.30(4) | 1.62(6) | F=1: -10.94 F=2: -7.64 F=3: -1.47 F=4: +9.03 |
| 6D5/2 | -1.069(18) | -0.4(4) | F=0: +9.07 F=1: +8.10 F=2: +6.12 F=3: +3.06 F=4: -1.19 F=5: -6.78 |
| 7D3/2 | 1.350(20) | 0.31(6) | F=1: -6.87 F=2: -4.42 F=3: -0.51 F=4: +5.14 |
| 7D5/2 | -0.55(10) | – | F=0: +4.81 F=1: +4.26 F=2: +3.16 F=3: +1.51 F=4: -0.69 F=5: -3.44 |
A, B: magnetic-dipole and electric-quadrupole constants (measured; see data file for sources).
Closed and nearly closed transitions of 85Rb
| Transition | λ vacuum (nm) | Lower level | A (s⁻¹) | Leak per scattered photon | Photons before a leak | Where the leak goes |
|---|---|---|---|---|---|---|
| 5S1/2 → 5P3/2 | 780.2414 | ground | 3.811e+07 measured | closed | – | no other level can be reached by electric-dipole decay |
| 5S1/2 → 5P1/2 | 794.9790 | ground | 3.610e+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 85Rb 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.
85Rb energy levels
Rb⁺ ionisation limit 33690.81 cm⁻¹ = 4.17713 eV = 1010.025 THz (296.817 nm)
Sources
- ARC (sum of calculated rates, 0 K)
- Allegrini, Arimondo, Orozco, J. Phys. Chem. Ref. Data 51, 043102 (2022), Table IV; origin…
- Allegrini, Arimondo, Orozco, J. Phys. Chem. Ref. Data 51, 043102 (2022), Table IV; origin…
- Allegrini, Arimondo, Orozco, J. Phys. Chem. Ref. Data 51, 043102 (2022), Table IV; origin…
- Allegrini, Arimondo, Orozco, J. Phys. Chem. Ref. Data 51, 043102 (2022), Table IV; origin…
- Allegrini, Arimondo, Orozco, J. Phys. Chem. Ref. Data 51, 043102 (2022), Table IV; origin…
- Allegrini, Arimondo, Orozco, J. Phys. Chem. Ref. Data 51, 043102 (2022), Table IV; origin…
- Allegrini, Arimondo, Orozco, J. Phys. Chem. Ref. Data 51, 043102 (2022), Table IV; origin…
- Allegrini, Arimondo, Orozco, J. Phys. Chem. Ref. Data 51, 043102 (2022), Table IV; origin…
- Allegrini, Arimondo, Orozco, J. Phys. Chem. Ref. Data 51, 043102 (2022), Table IV; origin…
- Allegrini, Arimondo, Orozco, J. Phys. Chem. Ref. Data 51, 043102 (2022), Table IV; origin…
- Allegrini, Arimondo, Orozco, J. Phys. Chem. Ref. Data 51, 043102 (2022), Table IV; origin…
- Allegrini, Arimondo, Orozco, J. Phys. Chem. Ref. Data 51, 043102 (2022), Table IV; origin…
- Allegrini, Arimondo, Orozco, J. Phys. Chem. Ref. Data 51, 043102 (2022), Table IV; origin…
- Allegrini, Arimondo, Orozco, J. Phys. Chem. Ref. Data 51, 043102 (2022), Table IV; origin…
- Allegrini, Arimondo, Orozco, J. Phys. Chem. Ref. Data 51, 043102 (2022), Table IV; origin…
- Allegrini, Arimondo, Orozco, J. Phys. Chem. Ref. Data 51, 043102 (2022), Table IV; origin…
- Allegrini, Arimondo, Orozco, J. Phys. Chem. Ref. Data 51, 043102 (2022), Table IV; origin…
- Allegrini, Arimondo, Orozco, J. Phys. Chem. Ref. Data 51, 043102 (2022), Table IV; origin…
- Allegrini, Arimondo, Orozco, J. Phys. Chem. Ref. Data 51, 043102 (2022), Table IV; origin…
- Herold, Vaidya, Li, Rolston, Porto, Safronova, Phys. Rev. Lett. 109, 243003 (2012) (light…
- NIST ASD A = 1.37e+05 s^-1
- NIST ASD A = 2.01e+04 s^-1
- NIST ASD A = 2.89e+05 s^-1
- NIST ASD A = 2.95e+06 s^-1
- NIST ASD A = 3.38e+04 s^-1
- NIST ASD A = 3.71e+06 s^-1
- NIST ASD A = 3.84e+04 s^-1
- NIST ASD A = 3.96e+05 s^-1
- NIST ASD A = 6.3e+05 s^-1
- NIST ASD A = 6.4e+04 s^-1
- NIST ASD A = 8.91e+04 s^-1
- NIST ASD level energies
- Safronova & Safronova, Phys. Rev. A 83, 052508 (2011), Table IV, column "Present" (relati…
- Safronova & Safronova, Phys. Rev. A 83, 052508 (2011), Table IV; original: Ekers, Glodz, …
- Safronova & Safronova, Phys. Rev. A 83, 052508 (2011), Table IV; original: Gomez, Aubin, …
- Safronova & Safronova, Phys. Rev. A 83, 052508 (2011), Table IV; original: Gomez, Baumer,…
- Safronova & Safronova, Phys. Rev. A 83, 052508 (2011), Table IV; original: Lundberg & Sva…
- Safronova & Safronova, Phys. Rev. A 83, 052508 (2011), Table IV; original: Marek & Munste…
- Safronova & Safronova, Phys. Rev. A 83, 052508 (2011), Table IV; original: experimental v…
- Safronova & Safronova, Phys. Rev. A 83, 052508 (2011), Table IV; original: van Wijngaarde…
- Safronova, Johnson, Derevianko (all-order theory), as listed in the hyperfine table of th…
- Sheng, Perez Galvan, Orozco, Phys. Rev. A 78, 062506 (2008)
- Steck, Rubidium 85 D Line Data, rev. 2.3.4 (8 Aug 2025), Table 3 (hyperfine centre of gra…
- Steck, Rubidium 85 D Line Data, rev. 2.3.4 (8 Aug 2025), Table 4 (hyperfine centre of gra…
- 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…
- pairinteraction
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-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