Atomic energy level diagrams

Radium energy level diagram

Energy levels and transitions of neutral radium (Ra I): the 22 strongest classified lines below 2 µm from the NIST Atomic Spectra Database and the 18 levels they connect, each line with its vacuum wavelength, frequency and, for 22 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.

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Radium energy level diagram with transition wavelengths and dipole matrix elements

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Key transitions of radium

Transitionλ vac (nm)λ air (nm)ν (THz)|⟨J‖er‖J′⟩| (ea₀)A (s⁻¹)Γ/2π up. (MHz)branch (%)Use
7s2 1S0 – 7s7p 1P°1482.7277482.5928621.038489(15)5.4301.770e+0828.2799.7strong singlet line
7s6d 3D3 – 6d7p 3F°4566.2383566.0812529.44585.8894.300e+076.9298.9566.2 nm
7s6d 3D1 – 6d7p 1D°2581.3199581.1588515.70991.3934.000e+068.3777.6581.3 nm
7s6d 3D3 – 6d7p 1D°2616.8757616.7051485.98522.9081.460e+078.37727.7616.9 nm
7s6d 3D2 – 6d7p 3F°3620.2020620.0304483.37884.5392.500e+075.68470620.2 nm
7s7p 3P°2 – 7s7d 3D3644.7981644.6200464.94005.6943.500e+077.57973.5644.8 nm line used for collinear laser spectroscopy at IS…
7s6d 3D3 – 6d7p 3F°3648.9112648.7319461.99313.0579.900e+065.68427.7648.9 nm
7s6d 3D1 – 6d7p 3F°2698.2151698.0226429.369773(15)3.7341.660e+0710.6131proposed spin-flip repump channel for the blue-slower sch…
7s6d 3D2 – 6d7p 3F°2712.0434711.8472421.031151(15)2.9409.700e+0610.6164proposed spin-flip repump channel for the blue-slower sch…
7s2 1S0 – 7s7p 3P°1714.3185714.1217419.69016(3)1.1312.370e+060.3771100intercombination line
7s6d 1D2 – 6d7p 1D°2722.7157722.5165414.81385.7103.500e+078.37766.5722.7 nm
7s7p 3P°0 – 7s8s 3S1731.2283731.0269409.98482.2188.500e+068.79315.2731.2 nm
7s6d 3D3 – 6d7p 3F°2750.1476749.9411399.64460.054*2.815e+0310.610.4750.1 nm
7s7p 3P°1 – 7s8s 3S1784.0270783.8113382.37523.8712.100e+078.79338.3784.0 nm
7s6d 1D2 – 6d7p 3F°2912.6828912.4323328.473887(15)2.964*4.683e+0610.615proposed spin-flip repump channel for the blue-slower sch…
7s7p 3P°2 – 7s8s 3S1993.4946993.2223301.75556.0252.500e+078.79345.9993.5 nm
7s6d 3D1 – 7s7p 1P°11428.60411428.2136209.8499(6)0.3773.300e+0428.270.0231repumper
7s7p 1P°1 – 7s8s 3S11656.06621655.6140181.02681.458*3.159e+058.7930.5721656 nm

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).

223Ra hyperfine structure (I = 3/2)

LevelA (MHz)B (MHz)Shift of each F level from the centre of gravity (MHz)
7s7p 3P°11202.1(6)-470.2(12)F=1/2: -3593.00 F=3/2: -731.90 F=5/2: +1685.60
7s7p 3P°2700(3)688(4)F=1/2: -2545.76 F=3/2: -2098.80 F=5/2: -780.11 F=7/2: +2270.93
7s7p 1P°1-344.5(9)421.5(16)F=1/2: +1388.12 F=3/2: -77.00 F=5/2: -411.38
7s7d 3D3536(5)74(3)F=3/2: -3169.26 F=5/2: -1885.68 F=7/2: -36.95 F=9/2: +2428.68

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

Isotope shifts

Transitionλ vac (nm)IsotopesShift (MHz)
7s2 1S0 – 7s7p 1P°1482.728208-2148485(8)
7s2 1S0 – 7s7p 1P°1482.728209-2148313(8)
7s2 1S0 – 7s7p 1P°1482.728210-2146003(6)
7s2 1S0 – 7s7p 1P°1482.728211-2145522(4)
7s2 1S0 – 7s7p 1P°1482.728212-2143256(3)
7s2 1S0 – 7s7p 1P°1482.728213-2142167(3)
7s2 1S0 – 7s7p 1P°1482.728220-214-21904(8)
7s2 1S0 – 7s7p 1P°1482.728221-214-25945(8)
7s2 1S0 – 7s7p 1P°1482.728222-214-28827(8)
7s2 1S0 – 7s7p 1P°1482.728223-214-32453(9)
7s2 1S0 – 7s7p 1P°1482.728224-214-35123(9)
7s2 1S0 – 7s7p 1P°1482.728225-214-38888(10)
7s2 1S0 – 7s7p 1P°1482.728226-214-41124(11)
7s2 1S0 – 7s7p 1P°1482.728227-214-43937(12)
7s2 1S0 – 7s7p 1P°1482.728228-214-46950(12)
7s2 1S0 – 7s7p 1P°1482.728229-214-50066(15)
7s2 1S0 – 7s7p 1P°1482.728230-214-53634(15)
7s2 1S0 – 7s7p 1P°1482.728232-214-59585(17)
7s2 1S0 – 7s7p 1P°1482.728225-2262236(15)
7s7p 3P°2 – 7s7d 3D3644.798212-214-887(4)
7s7p 3P°2 – 7s7d 3D3644.798221-2147001(7)
7s7p 3P°2 – 7s7d 3D3644.798222-2147781(4)

Shift = ν(first isotope) − ν(second isotope).

Closed and nearly closed transitions of radium

Transitionλ vacuum (nm)Lower levelA (s⁻¹)Leak per scattered photonPhotons before a leakWhere the leak goes
7s2 1S0 → 7s7p 3P°1714.3185ground2.370e+06 measured3.9 × 10−5 from theory25,6007s6d 3D1 3.92 × 10−5*; 7s6d 3D2 7.87 × 10−10* (long-lived)
7s2 1S0 → 7s7p 1P°1482.7277ground1.770e+08 NIST0.272 % from theory3687s6d 1D2 0.181 %*; 7s6d 3D2 6.85 × 10−4* (long-lived); 7s6d 3D1 2.31 × 10−4*

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 Ra 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
7s2 1S07s7p 1P°1482.7277482.5928621.0385E15.430 NIST1.770e+08 NIST99.7NIST ASD (accuracy AA)
7s6d 3D26d7p 3D°2540.1732540.0231554.9932E13.637 NIST3.400e+07 NIST44.2NIST ASD (accuracy D+)
7s6d 3D36d7p 3D°3540.8300540.6796554.3193E14.791 NIST4.200e+07 NIST88.2NIST ASD (accuracy D+)
7s7p 3P°17s7d 3D2555.7395555.5852539.4478E14.268 NIST4.300e+07 NIST81.7NIST ASD (accuracy D+)
7s6d 3D36d7p 3F°4566.2383566.0812529.4458E15.889 NIST4.300e+07 NIST98.9NIST ASD (accuracy C+)
7s6d 3D16d7p 1D°2581.3199581.1588515.7099E1 (intercombination)1.393 NIST4.000e+06 NIST7.6NIST ASD (accuracy C+)
7s6d 3D36d7p 1D°2616.8757616.7051485.9852E1 (intercombination)2.908 NIST1.460e+07 NIST27.7NIST ASD (accuracy C+)
7s6d 3D26d7p 3F°3620.2020620.0304483.3788E14.539 NIST2.500e+07 NIST70NIST ASD (accuracy C+)
7s7p 3P°27s7d 3D3644.7981644.6200464.9400E15.694 NIST3.500e+07 NIST73.5NIST ASD (accuracy D+)
7s6d 3D36d7p 3F°3648.9112648.7319461.9931E13.057 NIST9.900e+06 NIST27.7NIST ASD (accuracy C+)
7s6d 3D16d7p 3F°2698.2151698.0226429.3698E13.734 NIST1.660e+07 NIST31NIST ASD (accuracy C+)
7s6d 3D26d7p 3F°2712.0434711.8472421.0312E12.940 NIST9.700e+06 NIST64NIST ASD (accuracy C+)
7s2 1S07s7p 3P°1714.3185714.1217419.6902E1 (intercombination)1.131 measured2.370e+06 measured100experimental rate 2.37(12)[6] s^-1 attributed to Scielzo et al. 2006 in Table 1 of Bieron…
7s6d 1D26d7p 1D°2722.7157722.5165414.8138E15.710 NIST3.500e+07 NIST66.5NIST ASD (accuracy C+)
7s7p 3P°07s8s 3S1731.2283731.0269409.9848E12.218 NIST8.500e+06 NIST15.2NIST ASD (accuracy C+)
7s6d 3D36d7p 3F°2750.1476749.9411399.6446E10.0541 theory2.815e+03 theory0.4UDel Portal for High-Precision Atomic Data and Computation (Safronova group), Ra I tables…
7s7p 3P°17s8s 3S1784.0270783.8113382.3752E13.871 NIST2.100e+07 NIST38.3NIST ASD (accuracy C+)
7s6d 1D26d7p 3F°2912.6828912.4323328.4739E1 (intercombination)2.964 theory4.683e+06 theory5UDel Portal for High-Precision Atomic Data and Computation (Safronova group), Ra I tables…
7s7p 3P°27s8s 3S1993.4946993.2223301.7555E16.025 NIST2.500e+07 NIST45.9NIST ASD (accuracy C+)
7s6d 3D17s7p 1P°11428.60411428.2136209.8499E1 (intercombination)0.377 NIST3.300e+04 NIST0.0231NIST ASD (accuracy D+)
7s6d 3D27s7p 1P°11487.72461487.3181201.5107E1 (intercombination)0.771 theory1.218e+05 theory0.0685UDel Portal for High-Precision Atomic Data and Computation (Safronova group), Ra I tables…
7s7p 1P°17s8s 3S11656.06621655.6140181.0268E1 (intercombination)1.458 theory3.159e+05 theory0.572UDel Portal for High-Precision Atomic Data and Computation (Safronova group), Ra I tables…

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.

Ra energy levels

LevelEnergy (cm⁻¹)JParityLifetimegJHyperfine A (MHz)Hyperfine B (MHz)Lifetime sourceHyperfine source
7s2 1S00.0000evenstable–––––
7s7p 3P°013078.4000odd34 s theory–––Bieron, Indelicato, Jonsson, Eur. Phys. J. Special Topics 144, 75 (2007) [arXiv:physics/0…–
7s6d 3D113715.7791even> 510 µs measured0.5 theory––Guest, Scielzo, Ahmad, Bailey, Greene, Holt, Lu, O'Connor, Potterveld, Phys. Rev. Lett. 9…–
7s6d 3D213993.9402even3.3 s theory1.16 theory––Dzuba & Ginges, Phys. Rev. A 73, 032503 (2006) [arXiv:physics/0511199], Table VI (CI + ma…–
7s7p 3P°113999.3571odd422 ns measured1.47 theory1202.1-470.2Scielzo, Guest, Schulte, Ahmad, Bailey, Bowers, Holt, Lu, O'Connor, Potterveld, Phys. Rev…Wendt, Ahmad, Klempt, Neugart, Otten, Stroke, Z. Phys. D 4, 227 (1987) (collinear laser s…
7s6d 3D314707.2903even157 s theory1.33 theory––Bieron, Indelicato, Jonsson, Eur. Phys. J. Special Topics 144, 75 (2007) [arXiv:physics/0…–
7s7p 3P°216688.5402odd5.53 µs theory1.5 theory699.6688.5UDel Portal for High-Precision Atomic Data and Computation (Safronova group), Ra I tables…Wendt, Ahmad, Klempt, Neugart, Otten, Stroke, Z. Phys. D 4, 227 (1987) (collinear laser s…
7s6d 1D217081.3102even385 µs measured1.01 theory––Trimble, Sulai, Ahmad, Bailey, Graner, Greene, Holt, Korsch, Lu, Mueller, O'Connor, Phys.…–
7s7p 1P°120715.6141odd5.63 ns theory1.02 theory-344.5421.5UDel Portal for High-Precision Atomic Data and Computation (Safronova group), Ra I tables…Wendt, Ahmad, Klempt, Neugart, Otten, Stroke, Z. Phys. D 4, 227 (1987) (collinear laser s…
7s8s 3S126754.0201even18.1 ns theory2 theory––UDel Portal for High-Precision Atomic Data and Computation (Safronova group), Ra I tables…–
6d7p 3F°228038.0002odd15 ns measured0.74 theory––Booth, Rabga, Ready, Bailey, Bishof, Dietrich, Greene, Mueller, O'Connor, Singh, Spectroc…–
6d7p 3F°330117.7203odd28 ns theory1.09 theory––Dzuba & Flambaum, J. Phys. B 40, 227 (2007) [arXiv:physics/0610119]; Table 3 (CI + MBPT)–
6d7p 1D°230918.0102odd19 ns theory1.07 theory––Dzuba & Flambaum, J. Phys. B 40, 227 (2007) [arXiv:physics/0610119]; Table 3 (CI + MBPT)–
7s7d 3D231993.4002even19 ns theory1.16 theory––Dzuba & Flambaum, J. Phys. B 40, 227 (2007) [arXiv:physics/0610119]; Table 3 (CI + MBPT)–
7s7d 3D332197.2703even21 ns theory1.33 theory535.673.9Dzuba & Flambaum, J. Phys. B 40, 227 (2007) [arXiv:physics/0610119]; Table 3 (CI + MBPT)Wendt, Ahmad, Klempt, Neugart, Otten, Stroke, Z. Phys. D 4, 227 (1987) (collinear laser s…
6d7p 3F°432367.7004odd23 ns theory1.25 theory––Dzuba & Flambaum, J. Phys. B 40, 227 (2007) [arXiv:physics/0610119]; Table 3 (CI + MBPT)–
6d7p 3D°232506.5202odd13 ns theory1.17 theory––Dzuba & Flambaum, J. Phys. B 40, 227 (2007) [arXiv:physics/0610119]; Table 3 (CI + MBPT)–
6d7p 3D°333197.3903odd21 ns theory1.17 theory––Dzuba & Flambaum, J. Phys. B 40, 227 (2007) [arXiv:physics/0610119]; Table 3 (CI + MBPT)–

Ra⁺ ionisation limit 42573.36 cm⁻¹ = 5.27842 eV (234.889 nm)

Sources

Level energies are the NIST ASD values (226Ra; NIST adopts Santra et al. for 1P1 and Guest/Scielzo et al. for 3P1). rme_J_ea0 is |<J||D||J'>| in e a0 in the symmetric convention of the Safronova papers / UDel portal, A = 2.02613e18 |d|^2 / ((2J'+1) lambda^3[Angstrom]), J' = upper level; Dzuba & Flambaum (their Eq. 12) and Dzuba & Ginges use the same convention, so no conversion was needed. The UDel portal does carry neutral Ra (element key "Ra1": 48 matrix elements, 24 rates, lifetimes; data service https://atom.ece.udel.edu/graphql behind https://www1.udel.edu/atom/); all its Ra I numbers are theory except the 3P1 lifetime, which it attributes to Scielzo et al. It also carries Ra+ (key "Ra2"), not used here. Isotope shifts are nu(first) - nu(second); the ISOLDE tables are referenced to 214Ra, and for odd isotopes refer to hyperfine centres of gravity. Hyperfine A, B signs as printed in the compilation. frequency_THz entries are for 226Ra (I = 0, no hyperfine structure); frequency_THz_225 entries are centres of gravity derived here from the measured hyperfine component and A, and the measured components themselves are under hyperfine_component_frequency_THz. Extra fields beyond the schema: ionization_energy, linewidth_MHz and measured_energy_cm on levels, oscillator_strength, hyperfine_component_frequency_THz, wavenumber_cm inside frequency entries, half_life / mu / Q in isotopes (abundance_percent is null: no stable isotope). Radium has no stable isotope; 226Ra (1600 y) and

Atoms with measured data

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