Atomic energy level diagrams

Bismuth energy level diagram

Energy levels and transitions of neutral bismuth (Bi I): the 39 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 37 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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Bismuth energy level diagram with transition wavelengths and dipole matrix elements

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

Key transitions of bismuth

Transitionλ vac (nm)λ air (nm)ν (THz)|⟨J‖er‖J′⟩| (ea₀)A (s⁻¹)Γ/2π up. (MHz)branch (%)Use
4S°3/2 – 2[0]1/2306.8593306.7702976.97032.1821.670e+0833.8678.5resonance line for collinear and in-source laser spectros…
4S°3/2 – 2D°5/2647.7732647.5943462.8046––1.054e-06–magnetic-dipole line used for parity-nonconservation opti…
4S°3/2 – 2D°3/2875.7304875.4900342.3342–2.250e+014.421e-0681magnetic-dipole line of the Oxford parity-nonconservation…

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).

209Bi hyperfine structure (I = 9/2)

LevelA (MHz)B (MHz)Shift of each F level from the centre of gravity (MHz)
4S°3/2-446.9420(10)-304.6540(20)F=3: +3547.64 F=4: +1962.97 F=5: -208.27 F=6: -3093.02
2D°3/2-1231.020-652.500F=3: +9856.85 F=4: +5367.77 F=5: -651.39 F=6: -8472.51
2D°5/22502.86023.000F=2: -34403.78 F=3: -26902.10 F=4: -16897.18 F=5: -4386.71 F=6: +10632.17 F=7: +28162.92
2P°1/211260.200–F=4: -30965.55 F=5: +25335.45
2[0]1/24920.8(6)–F=4: -13532.20 F=5: +11071.80
2P°3/2491.028978.640F=3: -3602.44 F=4: -2290.75 F=5: -39.50 F=6: +3559.10

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

Closed and nearly closed transitions of bismuth

Transitionλ vacuum (nm)Lower levelA (s⁻¹)Leak per scattered photonPhotons before a leakWhere the leak goes
4S°3/2 → 2[0]1/2306.8593ground1.670e+08 NIST≥ 4.42 % from NIST data≤ 232D°3/2 4.42 % (long-lived); 1 more possible path without a listed rate
4S°3/2 → 2[2]5/2223.1304ground2.340e+08 NIST≥ 6.21 % from this site's HFR fit≤ 162D°3/2 5.51 % (long-lived); 2D°5/2 0.57 % (long-lived); 2[1]°3/2 ≈ 0.133 %; 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.

Listed Bi 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
4S°3/22[2]5/2195.4710–1533.6931E11.138 NIST5.860e+07 NIST–NIST ASD (accuracy B)
4S°3/22[2]3/2196.0051–1529.5138E10.478 NIST1.540e+07 NIST–NIST ASD (accuracy C+)
4S°3/22[2]3/2202.1799202.11471482.8008E10.307 NIST5.790e+06 NIST–NIST ASD (accuracy C+)
4S°3/22[2]5/2206.2286206.16281453.6897E11.581 NIST9.620e+07 NIST52.9NIST ASD (accuracy B)
4S°3/22[0]1/2211.0886211.02171420.2211E10.916 NIST9.040e+07 NIST–NIST ASD (accuracy B)
4S°3/22[1]1/2217.7896217.72141376.5235E10.163 NIST2.600e+06 NIST–NIST ASD (accuracy D+)
4S°3/22[1]3/2222.8905222.82121345.0211E11.387 NIST8.800e+07 NIST37.8NIST ASD (accuracy C+)
4S°3/22[2]5/2223.1304223.06111343.5751E12.775 NIST2.340e+08 NIST88.9NIST ASD (accuracy C+)
4S°3/22[2]3/2227.7262227.65591316.4598E10.742 NIST2.360e+07 NIST63.7NIST ASD (accuracy B)
2D°5/257075/2240.1612240.08811248.2968E11.542 NIST5.800e+07 NIST–NIST ASD (accuracy C+)
2D°3/22[2]5/2251.6391251.56341191.3589E10.317 NIST2.130e+06 NIST–NIST ASD (accuracy C)
2D°3/22[2]3/2252.5249252.44901187.1797E10.523 NIST8.600e+06 NIST–NIST ASD (accuracy C+)
2D°3/22[2]3/2262.8682262.78991140.4666E11.279 NIST4.560e+07 NIST–NIST ASD (accuracy B)
2D°3/22[2]5/2269.7539269.67381111.3555E10.600 NIST6.200e+06 NIST3.41NIST ASD (accuracy C+)
2P°1/258273/2273.1302273.04941097.6172E10.901 NIST2.020e+07 NIST–NIST ASD (accuracy C+)
2D°3/22[0]1/2278.1298278.04771077.8869E10.810 NIST3.090e+07 NIST–NIST ASD (accuracy B)
2D°5/22[2]5/2279.9474279.86491070.8884E10.337 NIST1.750e+06 NIST–NIST ASD (accuracy D+)
2D°5/22[2]3/2281.0442280.96151066.7092E10.766 NIST1.340e+07 NIST–NIST ASD (accuracy C+)
2P°1/256573/2286.4628286.37871046.5319E10.705 NIST1.070e+07 NIST–NIST ASD (accuracy C+)
2D°3/22[1]1/2289.8816289.79671034.1894E11.918 NIST1.530e+08 NIST–NIST ASD (accuracy B)
2D°5/22[2]3/2293.9153293.82941019.9961E12.453 NIST1.200e+08 NIST–NIST ASD (accuracy B)
2D°3/22[1]3/2298.9891298.90191002.6870E11.688 NIST5.400e+07 NIST23.2NIST ASD (accuracy C+)
2D°3/22[2]5/2299.4209299.33361001.2409E11.074 NIST1.450e+07 NIST5.51NIST ASD (accuracy C+)
2D°5/22[2]5/2302.5502302.4621990.8851E12.659 NIST8.620e+07 NIST47.4NIST ASD (accuracy B)
4S°3/22[0]1/2306.8593306.7702976.9703E12.182 NIST1.670e+08 NIST78.5NIST ASD (accuracy B)
2D°3/22[2]3/2307.7554307.6660974.1257E10.436 NIST3.310e+06 NIST8.94NIST ASD (accuracy C+)
2D°5/22[1]3/2339.8173339.7198882.2165E11.178 NIST1.790e+07 NIST7.7NIST ASD (accuracy C)
2D°5/22[2]5/2340.3752340.2776880.7705E10.418 NIST1.500e+06 NIST0.57NIST ASD (accuracy C)
2P°1/22[2]3/2340.6206340.5229880.1360E10.707 NIST6.400e+06 NIST–NIST ASD (accuracy D+)
2D°5/22[2]3/2351.1868351.0864853.6552E10.746 NIST6.500e+06 NIST17.5NIST ASD (accuracy C+)
2P°1/22[2]3/2359.7123359.6097833.4229E11.332 NIST1.930e+07 NIST–NIST ASD (accuracy C+)
2P°1/22[0]1/2388.9149388.8048770.8433E10.488 NIST4.100e+06 NIST–NIST ASD (accuracy D+)
2P°1/22[1]1/2412.2867412.1704727.1457E11.065 NIST1.640e+07 NIST–NIST ASD (accuracy C+)
2P°1/22[1]3/2430.9572430.8360695.6433E10.503 NIST1.600e+06 NIST0.688NIST ASD (accuracy D)
2P°1/22[2]3/2449.4087449.2827667.0820E10.506 NIST1.430e+06 NIST3.86NIST ASD (accuracy D+)
2D°3/22[0]1/2472.3848472.2527634.6361E10.989 NIST9.400e+06 NIST4.42NIST ASD (accuracy B)
2P°3/22[2]3/2613.6436613.4738488.5449E10.891 NIST1.740e+06 NIST–NIST ASD (accuracy D+)
4S°3/22D°5/2647.7732647.5943462.8046M1––––
4S°3/22D°3/2875.7304875.4900342.3342M1–2.250e+01 NIST81NIST ASD (accuracy B+)

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, this site's own Cowan-code calculation with the parameters fitted to the NIST energies (HFR fit; inputs and fit report in the repository folder cowan/; used only where nothing else gives a rate; strong lines typically within a factor 2, weak lines worse), or a model calculation.

Bi energy levels

LevelEnergy (cm⁻¹)JParityLifetimegJHyperfine A (MHz)Hyperfine B (MHz)Lifetime sourceHyperfine source
4S°3/20.0003/2oddstable–-446.942-304.654–Hull, Brink, Phys. Rev. A 1, 685 (1970) (atomic-beam magnetic resonance); Pearson et al.,…
2D°3/211419.0393/2odd36 ms theory1.225-1231.02-652.5Liu, Yu, Suo, Liu, Sahoo, "Investigating properties of heavy and superheavy atomic system…values labelled 'Exp. 2021' with reference Wilman, Elantkowska, Ruczkowski, J. Quant. Spe…
2D°5/215437.5015/2odd151 ms theory1.22502.8623Liu, Yu, Suo, Liu, Sahoo, "Investigating properties of heavy and superheavy atomic system…values labelled 'Exp. 2021' with reference Wilman, Elantkowska, Ruczkowski, J. Quant. Spe…
2P°1/221660.9141/2odd11.3 ms measured0.66711260.2–Krogulec, Wojtkowiak, Heldt, Acta Phys. Pol. A 60, 591 (1981) (time-of-flight on an elect…values labelled 'Exp. 2021' with reference Wilman, Elantkowska, Ruczkowski, J. Quant. Spe…
2[0]1/232588.2211/2even4.7 ns measured2.0884920.8–Andersen, Madsen, Sørensen, "Radiative Lifetimes in Sn I and Bi I", J. Opt. Soc. Am. 62, …Hull, Brink, Phys. Rev. A 1, 685 (1970) (atomic-beam magnetic resonance); Pearson et al.,…
2P°3/233164.8053/2odd5.8 ms theory–491.028978.64Liu, Yu, Suo, Liu, Sahoo, "Investigating properties of heavy and superheavy atomic system…values labelled 'Exp. 2021' with reference Wilman, Elantkowska, Ruczkowski, J. Quant. Spe…
2[2]3/243912.3743/2even27 ns measured0.79––Andersen, Madsen, Sørensen, "Radiative Lifetimes in Sn I and Bi I", J. Opt. Soc. Am. 62, …–
2[2]5/244816.8415/2even3.8 ns measured1.2––Andersen, Madsen, Sørensen, "Radiative Lifetimes in Sn I and Bi I", J. Opt. Soc. Am. 62, …–
2[1]3/244865.0763/2even4.3 ns measured1.676––Andersen, Madsen, Sørensen, "Radiative Lifetimes in Sn I and Bi I", J. Opt. Soc. Am. 62, …–
2[1]1/245915.8831/2even–1.3––––
2[0]1/247373.4771/2even––––––
2[2]5/248489.8695/2even5.5 ns measured1.41––Andersen, Madsen, Sørensen, "Radiative Lifetimes in Sn I and Bi I", J. Opt. Soc. Am. 62, …–
2[2]3/249460.9103/2even–0.98––––
2[2]3/251019.0903/2even––––––
2[2]5/251158.4945/2even––––––
56573/256569.4603/2even––––––
57075/257076.2005/2even––––––
58273/258273.4833/2even––––––

Bi⁺ ionisation limit 58761.65 cm⁻¹ = 7.28552 eV (170.179 nm)

Sources

NIST labels the even levels in J1K notation; the LS names used in the literature are given in brackets. The 1972 beam-foil lifetimes were read from the publisher's abstract page by an automated reader: verify before relying on them, and prefer Luo et al. 1995 once accessible. Hyperfine constants of the 6p3 2D and 2P levels are second-hand and printed without uncertainties. The 'use' strings of the two M1 lines carry the parity-violation results because the schema has no field for them.

Atoms with measured data

All elements: periodic table