Atomic energy level diagrams

Germanium energy level diagram

Energy levels and transitions of neutral germanium (Ge I): the 54 strongest classified lines below 2 µm from the NIST Atomic Spectra Database and the 20 levels they connect, each line with its vacuum wavelength, frequency and, for 48 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.

Hover a line or a level to isolate it, click to keep it selected. Scroll to zoom, drag to move.

Germanium energy level diagram with transition wavelengths and dipole matrix elements

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

Key transitions of germanium

Transitionλ vac (nm)λ air (nm)ν (THz)|⟨J‖er‖J′⟩| (ea₀)A (s⁻¹)Γ/2π up. (MHz)branch (%)Use
4p2 3P1 – 4p5s 3P°1269.2140269.13411113.58421.3286.100e+0734.0122.1269.13 nm line used for collinear laser spectroscopy of G…
4p2 3P1 – 4p2 1S0632.5031632.3282473.9778–1.000e+003.452e-0746.1forbidden line within the ground configuration
4p2 3P2 – 4p2 1S0668.5666668.3821448.4107–6.800e-023.452e-073.14forbidden line within the ground configuration
4p2 1D2 – 4p2 1S01082.01291081.7165277.0692–1.100e+003.452e-0750.7forbidden line within the ground configuration
4p2 3P0 – 4p2 1D21403.44991403.0663213.6111–3.000e-052.361e-080.0202forbidden line within the ground configuration
4p2 3P1 – 4p2 1D21522.49531522.0793196.9086–5.030e-022.361e-0833.9forbidden line within the ground configuration
4p2 3P2 – 4p2 1D21749.67781749.2001171.3415–9.800e-022.361e-0866forbidden line within the ground configuration

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).

73Ge hyperfine structure (I = 9/2)

LevelA (MHz)B (MHz)Shift of each F level from the centre of gravity (MHz)
4p2 3P115.5480(18)-54.566(9)F=7/2: -110.52 F=9/2: +20.83 F=11/2: +56.32
4p2 3P2-64.4270(7)111.825(13)F=5/2: +759.95 F=7/2: +485.53 F=9/2: +160.66 F=11/2: -193.68 F=13/2: -551.89
4p5s 3P°1-262.2(12)40(6)F=7/2: +1460.43 F=9/2: +235.53 F=11/2: -1169.90

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

Isotope shifts

Transitionλ vac (nm)IsotopesShift (MHz)
4p2 3P1 – 4p5s 3P°1269.21470-72-35.0(20)
4p2 3P1 – 4p5s 3P°1269.21473-728(4)
4p2 3P1 – 4p5s 3P°1269.21474-7252.0(20)

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

Closed and nearly closed transitions of germanium

Transitionλ vacuum (nm)Lower levelA (s⁻¹)Leak per scattered photonPhotons before a leakWhere the leak goes
4p2 3P1 → 4p5s 3P°0271.0427metastable2.800e+08 NISTclosed–no other level can be reached by electric-dipole decay
4p2 1D2 → 4p4d 1F°3219.9401metastable2.630e+08 measured7 × 10−4 from measured data1,4304p5p 1D2 ≈ 0.682 %; 4p5p 3P2 ≈ 0.274 %; 4p2 3P2 7.46 × 10−4 (long-lived); 1 weaker lines; the listed lines add up to ≈ 1.03 %
4p2 3P2 → 4p4d 3D°3209.4924metastable9.700e+07 NIST2.5 % from measured data404p2 1D2 2.54 % (long-lived); 4p5p 3D2 ≈ 0.183 %; 4p5p 3D3 ≈ 2.73 × 10−5; 1 weaker lines
4p2 3P1 → 4p4d 3P°0194.4730metastable7.000e+07 NIST≥ 3.78 % from this site's HFR fit≤ 264p5p 3D1 ≈ 2.86 %; 4p5p 3S1 ≈ 0.596 %; 4p5p 3P1 ≈ 0.472 %; 1 more possible path without a listed rate
4p2 3P2 → 4p4d 3P°2199.8887metastable5.500e+07 NIST6.8 % from measured data154p2 1D2 4.94 % (long-lived); 4p2 3P1 1.86 % (long-lived); 4p5p 3S1 ≈ 0.304 %; 6 weaker lines
4p2 3P2 → 4p4d 3F°3204.4425metastable8.620e+07 measured6.9 % from measured data144p2 1D2 6.94 % (long-lived); 4p5p 3D2 ≈ 1.21 %; 4p5p 3D3 ≈ 0.144 %; 2 weaker lines
4p2 3P1 → 4p4d 3D°2206.9317metastable1.200e+08 NIST9.2 % from measured data114p2 3P2 8.96 % (long-lived); 4p2 1D2 2 % (long-lived); 4p5p 3D1 ≈ 0.371 %; 3 weaker lines

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 Ge 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
4p2 3P04p4d 1P°1189.2247–1584.3196E1 (intercombination)0.032 measured1.020e+05 measured0.1branching ratio / lifetime
4p2 3P14p4d 1P°1191.2409–1567.6172E1 (intercombination)0.188 measured3.410e+06 measured3.34Li, Norin, Persson, Wahlstrom, Svanberg, Doidge, Biemont, Phys. Rev. A 60, 198 (1999), Ta…
4p2 3P04p4d 3P°1193.4048–1550.0775E10.271 measured6.850e+06 measured5.89Li, Norin, Persson, Wahlstrom, Svanberg, Doidge, Biemont, Phys. Rev. A 60, 198 (1999), Ta…
4p2 3P24p4d 1P°1194.4116–1542.0501E1 (intercombination)0.134 measured1.640e+06 measured1.61Li, Norin, Persson, Wahlstrom, Svanberg, Doidge, Biemont, Phys. Rev. A 60, 198 (1999), Ta…
4p2 3P14p4d 3P°0194.4730–1541.5633E10.504 NIST7.000e+07 NIST100NIST ASD (accuracy C)
4p2 3P24p4d 1F°3195.3802–1534.4056E1 (intercombination)0.0711 measured1.960e+05 measured0.0746Li, Norin, Persson, Wahlstrom, Svanberg, Doidge, Biemont, Phys. Rev. A 60, 198 (1999), Ta…
4p2 3P14p4d 3P°1195.5115–1533.3750E10.557 NIST2.800e+07 NIST37NIST ASD (accuracy C)
4p2 3P14p4d 3P°2196.5383–1525.3640E10.216 measured2.480e+06 measured1.86Li, Norin, Persson, Wahlstrom, Svanberg, Doidge, Biemont, Phys. Rev. A 60, 198 (1999), Ta…
4p2 3P24p4d 3P°1198.8267–1507.8079E10.539 NIST2.500e+07 NIST35.4NIST ASD (accuracy C)
4p2 3P24p4d 3P°2199.8887–1499.7969E11.041 NIST5.500e+07 NIST93.2NIST ASD (accuracy C)
4p2 3P14p4d 3F°2201.9720201.90691484.3270E11.023 measured5.150e+07 measured67.4Li, Norin, Persson, Wahlstrom, Svanberg, Doidge, Biemont, Phys. Rev. A 60, 198 (1999), Ta…
4p2 3P04p4d 3D°1204.2368204.17121467.8673E11.178 NIST1.100e+08 NIST67.2NIST ASD (accuracy C)
4p2 3P24p4d 3F°3204.4425204.37701466.3900E11.595 measured8.620e+07 measured93.1Li, Norin, Persson, Wahlstrom, Svanberg, Doidge, Biemont, Phys. Rev. A 60, 198 (1999), Ta…
4p2 3P24p4d 3F°2205.5119205.44611458.7599E10.522 measured1.270e+07 measured16.6Li, Norin, Persson, Wahlstrom, Svanberg, Doidge, Biemont, Phys. Rev. A 60, 198 (1999), Ta…
4p2 3P14p4d 3D°1206.5875206.52151451.1648E11.053 NIST8.500e+07 NIST31.4NIST ASD (accuracy C)
4p2 3P14p4d 3D°2206.9317206.86561448.7509E11.620 NIST1.200e+08 NIST90.8NIST ASD (accuracy C)
4p2 3P14p4d 1D°2208.6684208.60211436.6928E1 (intercombination)0.947 NIST4.000e+07 NIST19.8NIST ASD (accuracy C)
4p2 3P24p4d 3D°3209.4924209.42581431.0424E11.755 NIST9.700e+07 NIST97.5NIST ASD (accuracy C)
4p2 3P24p4d 3D°1210.2925210.22581425.5977E10.113 measured9.300e+05 measured0.4Li, Norin, Persson, Wahlstrom, Svanberg, Doidge, Biemont, Phys. Rev. A 60, 198 (1999), Ta…
4p2 3P24p4d 3D°2210.6491210.58241423.1838E10.626 NIST1.700e+07 NIST8.96NIST ASD (accuracy C)
4p2 3P24p4d 1D°2212.4492212.38201411.1257E1 (intercombination)0.269 measured3.060e+06 measured4.04Li, Norin, Persson, Wahlstrom, Svanberg, Doidge, Biemont, Phys. Rev. A 60, 198 (1999), Ta…
4p2 1D24p4d 1P°1218.7135218.64511370.7086E10.522 measured1.760e+07 measured17.2Li, Norin, Persson, Wahlstrom, Svanberg, Doidge, Biemont, Phys. Rev. A 60, 198 (1999), Ta…
4p2 1D24p4d 1F°3219.9401219.87141363.0641E13.109 measured2.630e+08 measured99.9Li, Norin, Persson, Wahlstrom, Svanberg, Doidge, Biemont, Phys. Rev. A 60, 198 (1999), Ta…
4p2 1D24p4d 3P°1224.3172224.24771336.4664E1 (intercombination)0.520 measured1.620e+07 measured13.9Li, Norin, Persson, Wahlstrom, Svanberg, Doidge, Biemont, Phys. Rev. A 60, 198 (1999), Ta…
4p2 1D24p4d 3P°2225.6699225.60011328.4554E1 (intercombination)0.301 NIST3.200e+06 NIST4.94NIST ASD (accuracy C)
4p2 1D24p4d 3F°3231.4913231.42021295.0484E1 (intercombination)0.525 measured6.430e+06 measured6.94Li, Norin, Persson, Wahlstrom, Svanberg, Doidge, Biemont, Phys. Rev. A 60, 198 (1999), Ta…
4p2 1D24p4d 3F°2232.8633232.79181287.4184E1 (intercombination)0.617 measured1.220e+07 measured16Li, Norin, Persson, Wahlstrom, Svanberg, Doidge, Biemont, Phys. Rev. A 60, 198 (1999), Ta…
4p2 1D24p4d 3D°3237.9870237.91441259.7009E1 (intercombination)0.444 measured4.230e+06 measured2.54Li, Norin, Persson, Wahlstrom, Svanberg, Doidge, Biemont, Phys. Rev. A 60, 198 (1999), Ta…
4p2 1D24p4d 3D°1239.0201238.94731254.2562E1 (intercombination)0.164 measured1.330e+06 measured0.57Li, Norin, Persson, Wahlstrom, Svanberg, Doidge, Biemont, Phys. Rev. A 60, 198 (1999), Ta…
4p2 1D24p4d 3D°2239.4810239.40811251.8423E1 (intercombination)0.105 measured3.280e+05 measured2Li, Norin, Persson, Wahlstrom, Svanberg, Doidge, Biemont, Phys. Rev. A 60, 198 (1999), Ta…
4p2 1D24p4d 1D°2241.8102241.73671239.7842E11.830 NIST9.600e+07 NIST76.1NIST ASD (accuracy C)
4p2 3P04p5s 1P°1249.8716249.79621199.7862E1 (intercombination)0.548 NIST1.300e+07 NIST4.64NIST ASD (accuracy C)
4p2 3P14p5s 1P°1253.3992253.32301183.0838E1 (intercombination)0.491 NIST1.000e+07 NIST3.62NIST ASD (accuracy C)
4p2 3P24p5s 1P°1258.9962258.91881157.5167E1 (intercombination)0.362 NIST5.100e+06 NIST1.68NIST ASD (accuracy C)
4p2 3P14p5s 3P°2259.3309259.25341156.0227E11.748 NIST7.100e+07 NIST27.2NIST ASD (accuracy C)
4p2 3P24p5s 3P°2265.1961265.11721130.4556E13.034 NIST2.000e+08 NIST72.1NIST ASD (accuracy C)
4p2 3P04p5s 3P°1265.2358265.15681130.2867E11.532 NIST8.500e+07 NIST32.5NIST ASD (accuracy C)
4p2 3P14p5s 3P°1269.2140269.13411113.5842E11.328 NIST6.100e+07 NIST22.1NIST ASD (accuracy C)
4p2 3P14p5s 3P°0271.0427270.96241106.0709E11.659 NIST2.800e+08 NIST100NIST ASD (accuracy C)
4p2 1S04p4d 1P°1274.1237274.04261093.6393E11.556 measured7.940e+07 measured77.8Li, Norin, Persson, Wahlstrom, Svanberg, Doidge, Biemont, Phys. Rev. A 60, 198 (1999), Ta…
4p2 3P24p5s 3P°1275.5402275.45881088.0171E11.846 NIST1.100e+08 NIST37.1NIST ASD (accuracy C)
4p2 1S04p4d 3P°1282.9840282.90081059.3972E1 (intercombination)0.549 measured9.000e+06 measured7.78Li, Norin, Persson, Wahlstrom, Svanberg, Doidge, Biemont, Phys. Rev. A 60, 198 (1999), Ta…
4p2 1D24p5s 1P°1303.9952303.9067986.1751E13.413 NIST2.800e+08 NIST86.1NIST ASD (accuracy C)
4p2 1S04p4d 3D°1306.7913306.7021977.1870E1 (intercombination)0.199 measured9.300e+05 measured0.4Li, Norin, Persson, Wahlstrom, Svanberg, Doidge, Biemont, Phys. Rev. A 60, 198 (1999), Ta…
4p2 1D24p5s 3P°2312.5723312.4817959.1141E1 (intercombination)0.483 NIST3.100e+06 NIST0.715NIST ASD (accuracy C)
4p2 1D24p5s 3P°1327.0431326.9489916.6756E1 (intercombination)1.226 NIST2.900e+07 NIST8.06NIST ASD (accuracy C)
4p2 1S04p5s 1P°1422.7753422.6563709.1059E11.533 NIST2.100e+07 NIST3.99NIST ASD (accuracy C)
4p2 1S04p5s 3P°1468.7140468.5828639.6064E1 (intercombination)1.204 NIST9.500e+06 NIST0.233NIST ASD (accuracy C)
4p2 3P14p2 1S0632.5031632.3282473.9778M1–1.000e+00 theory46.1R. H. Garstang, J. Res. Natl. Bur. Stand. 68A, 61 (1964), Table 16 (intermediate-coupling…
4p2 3P24p2 1S0668.5666668.3821448.4107E2–6.800e-02 theory3.14R. H. Garstang, J. Res. Natl. Bur. Stand. 68A, 61 (1964), Table 16 (intermediate-coupling…
4p2 1D24p2 1S01082.01291081.7165277.0692E2–1.100e+00 theory50.7R. H. Garstang, J. Res. Natl. Bur. Stand. 68A, 61 (1964), Table 16 (intermediate-coupling…
4p2 3P04p2 1D21403.44991403.0663213.6111E2–3.000e-05 theory0.0202R. H. Garstang, J. Res. Natl. Bur. Stand. 68A, 61 (1964), Table 16 (intermediate-coupling…
4p2 3P14p2 1D21522.49531522.0793196.9086M1–5.030e-02 theory33.9R. H. Garstang, J. Res. Natl. Bur. Stand. 68A, 61 (1964), Table 16 (intermediate-coupling…
4p2 3P24p2 1D21749.67781749.2001171.3415M1–9.800e-02 theory66R. H. Garstang, J. Res. Natl. Bur. Stand. 68A, 61 (1964), Table 16 (intermediate-coupling…

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.

Ge energy levels

LevelEnergy (cm⁻¹)JParityLifetimegJHyperfine A (MHz)Hyperfine B (MHz)Lifetime sourceHyperfine source
4p2 3P00.0000evenstable–––––
4p2 3P1557.1341even323 s theory1.501115.548-54.566R. H. Garstang, J. Res. Natl. Bur. Stand. 68A, 61 (1964), Table 16. Note: derived: 1/A of…Childs and Goodman, Phys. Rev. 141, 15 (1966) (atomic-beam magnetic resonance; values rea…
4p2 3P21409.9612even122 s theory1.4946-64.427111.825R. H. Garstang, J. Res. Natl. Bur. Stand. 68A, 61 (1964), Table 16. Note: derived: 1/sum …Childs and Goodman, Phys. Rev. 141, 15 (1966) (atomic-beam magnetic resonance; values rea…
4p2 1D27125.2992even6.74 s theory1.0064––R. H. Garstang, J. Res. Natl. Bur. Stand. 68A, 61 (1964), Table 16. Note: derived: 1/sum …–
4p2 1S016367.3330even461 ms theory–––R. H. Garstang, J. Res. Natl. Bur. Stand. 68A, 61 (1964), Table 16. Note: derived: 1/sum …–
4p5s 3P°037451.6890odd4.81 ns measured–––Biemont, Lynga, Li, Svanberg, Garnir, Doidge, Mon. Not. R. Astron. Soc. 303, 721 (1999), …–
4p5s 3P°137702.3051odd4.68 ns measured1.435-262.240Biemont, Lynga, Li, Svanberg, Garnir, Doidge, Mon. Not. R. Astron. Soc. 303, 721 (1999), …Kanellakopoulos et al., Phys. Rev. C 102, 054331 (2020), arXiv:2011.01659, Table I (colli…
4p5s 3P°239117.9022odd4.5 ns measured1.5––Biemont, Lynga, Li, Svanberg, Garnir, Doidge, Mon. Not. R. Astron. Soc. 303, 721 (1999), …–
4p5s 1P°140020.5601odd4.23 ns measured1.068––Biemont, Lynga, Li, Svanberg, Garnir, Doidge, Mon. Not. R. Astron. Soc. 303, 721 (1999), …–
4p4d 1D°248480.0482odd13.2 ns measured0.981––Li, Norin, Persson, Wahlstrom, Svanberg, Doidge, Biemont, Phys. Rev. A 60, 198 (1999), Ta…–
4p4d 3D°248882.2632odd6.1 ns measured1.008––Li, Norin, Persson, Wahlstrom, Svanberg, Doidge, Biemont, Phys. Rev. A 60, 198 (1999), Ta…–
4p4d 3D°148962.7831odd4.3 ns measured0.556––Li, Norin, Persson, Wahlstrom, Svanberg, Doidge, Biemont, Phys. Rev. A 60, 198 (1999), Ta…–
4p4d 3D°349144.3973odd6 ns measured1.24––Li, Norin, Persson, Wahlstrom, Svanberg, Doidge, Biemont, Phys. Rev. A 60, 198 (1999), Ta…–
4p4d 3F°250068.9542odd13.1 ns measured0.867––Li, Norin, Persson, Wahlstrom, Svanberg, Doidge, Biemont, Phys. Rev. A 60, 198 (1999), Ta…–
4p4d 3F°350323.4653odd10.8 ns measured1.194––Li, Norin, Persson, Wahlstrom, Svanberg, Doidge, Biemont, Phys. Rev. A 60, 198 (1999), Ta…–
4p4d 3P°251437.8022odd7.5 ns measured1.46––Li, Norin, Persson, Wahlstrom, Svanberg, Doidge, Biemont, Phys. Rev. A 60, 198 (1999), Ta…–
4p4d 3P°151705.0201odd8.6 ns measured1.391––Li, Norin, Persson, Wahlstrom, Svanberg, Doidge, Biemont, Phys. Rev. A 60, 198 (1999), Ta…–
4p4d 3P°051978.1500odd8 ns measured–––Li, Norin, Persson, Wahlstrom, Svanberg, Doidge, Biemont, Phys. Rev. A 60, 198 (1999), Ta…–
4p4d 1F°352592.2243odd3.8 ns measured1.01––Li, Norin, Persson, Wahlstrom, Svanberg, Doidge, Biemont, Phys. Rev. A 60, 198 (1999), Ta…–
4p4d 1P°152847.2151odd9.8 ns measured1.14––Li, Norin, Persson, Wahlstrom, Svanberg, Doidge, Biemont, Phys. Rev. A 60, 198 (1999), Ta…–

Ge⁺ ionisation limit 63713.24 cm⁻¹ = 7.89943 eV (156.953 nm)

Sources

Level energies are the NIST ASD values (data/nist/Ge_I_levels.tsv); Li et al. and Biemont et al. quote the same levels rounded to 0.01 cm^-1. A_s of E1 lines = measured branching ratio x 1/(measured laser lifetime) as printed by the authors; rme_J_ea0 is derived from that A with the NIST energies (convention of SCHEMA.md, J' = upper level). 4p5s lifetimes and 4p2-4p5s A values come from Biemont et al. 1999 (read directly; Li et al. 1999 reprints them), 4p4d / 4p6s / 4p5d lifetimes and 4p2-4p4d A values from Li et al. 1999. Forbidden-line rates and the metastable lifetimes derived from them are 1964 intermediate-coupling THEORY (Garstang), not measurements. Isotope shifts are nu(first) - nu(second), centre of gravity, natural reference isotope 72Ge. Hyperfine constants refer to 73Ge (I = 9/2). Deverall, Meissner, Zissis, Phys. Rev. 95, 1463 (1954) (abstract) report no resolvable structure in eight Ge I lines and estimate the shift between consecutive even isotopes as smaller than 0.005 cm^-1 (bound).

Atoms with measured data

All elements: periodic table