Atomic energy level diagrams

Holmium energy level diagram

Energy levels and transitions of neutral holmium (Ho I): the 39 strongest classified lines below 2 µm from the NIST Atomic Spectra Database and the 31 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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Holmium energy level diagram with transition wavelengths and dipole matrix elements

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

Key transitions of holmium

Transitionλ vac (nm)λ air (nm)ν (THz)|⟨J‖er‖J′⟩| (ea₀)A (s⁻¹)Γ/2π up. (MHz)branch (%)Use
4I°13/2 – (34366)11/2345.4665345.3675867.79030.9763.900e+066.928.97line from the metastable 4f11 6s2 4Io13/2 level
4I°15/2 – (25273)15/2395.6850395.5730757.65441.7566.300e+061.00799.5ground-state line
4I°15/2 – (24760)13/2403.8751403.7610742.29000.7391.200e+060.192499.2ground-state line
4I°15/2 – (24741)13/2404.1952404.0811741.70214.1253.730e+077.20282.4ground-state line
4I°15/2 – (15/2,1)15/2405.5018405.3873739.31229.2361.620e+0831.8381strong blue line
4I°15/2 – (24377)15/2410.2243410.1085730.80141.7755.780e+060.92100ground-state line
4I°15/2 – (15/2,1)17/2410.4957410.3799730.31811(3)9.7601.550e+0832.4875.9main broad cooling line: MOT, Zeeman slower, imaging
4I°13/2 – (13/2,1)13/2410.9779410.8619729.46139.7942.000e+0831.83100line from the metastable 4f11 6s2 4Io13/2 level
4I°15/2 – (24264)17/2412.1339412.0176727.41522.9721.420e+072.26799.7cycling line 412.1 nm, two-electron jump
4I°13/2 – (13/2,1)15/2412.8325412.7161726.184310.852.120e+0833.8699.6line from the metastable 4f11 6s2 4Io13/2 level
4I°15/2 – (15/2,1)13/2416.4199416.3026719.92826.6908.970e+0716.9384.3strong blue line
4I°15/2 – (13/2,2)13/2417.4374417.3197718.17353.6012.580e+074.97482.6ground-state line
4I°15/2 – (13/2,2)15/2419.5521419.4339714.55351.5043.880e+060.6169100ground-state line
4I°13/2 – (13/2,1)11/2422.8316422.7125709.01167.0181.100e+0816.93100line from the metastable 4f11 6s2 4Io13/2 level
4I°15/2 – (13/2,2)17/2425.5578425.4380704.46942.8061.150e+071.592100cycling line 425.6 nm
4I°15/2 – (5,5/2)15/2426.5251426.4051702.87181.5063.700e+060.593999.2ground-state line
4I°15/2 – (5,5/2)13/2435.1953435.0730688.86882.2518.900e+061.5392.6ground-state line
4I°15/2 – 8F13/2493.6256493.4878607.32770.5323.400e+050.0607589.1ground-state line
4I°15/2 – (6,5/2)13/2494.0392493.9013606.81921.4722.600e+060.3844100ground-state line
4I°15/2 – (6,5/2)15/2498.1347497.9958601.83011.0411.110e+060.184695.7ground-state line
4I°13/2 – (25273)15/2503.7040503.5636595.17590.1742.990e+041.0070.472line from the metastable 4f11 6s2 4Io13/2 level
4I°13/2 – (24760)13/2517.0516516.9076579.81150.0674.700e+030.19240.389line from the metastable 4f11 6s2 4Io13/2 level
4I°13/2 – (24741)13/2517.5764517.4323579.22360.5813.520e+057.2020.778line from the metastable 4f11 6s2 4Io13/2 level
4I°15/2 – (15/2,2)13/2530.2736530.1261565.35430.5272.700e+050.0444696.7ground-state line

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).

165Ho hyperfine structure (I = 7/2)

LevelA (MHz)B (MHz)Shift of each F level from the centre of gravity (MHz)
4I°15/2800.583645(6)-1668.0053(3)F=4: -24424.99 F=5: -20115.71 F=6: -15019.45 F=7: -9177.08 F=8: -2636.25 F=9: +4548.58 F=10: +12316.13 F=11: +20598.32
(15/2,1)17/2654.9(3)-620(20)F=5: -21991.97 F=6: -17945.34 F=7: -13253.91 F=8: -7931.35 F=9: -1993.29 F=10: +4542.69 F=11: +11657.04 F=12: +19328.28

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

Closed and nearly closed transitions of holmium

Transitionλ vacuum (nm)Lower levelA (s⁻¹)Leak per scattered photonPhotons before a leakWhere the leak goes
4I°15/2 → (15/2,1)17/2598.4505ground9.200e+05 measuredclosed–no other level can be reached by electric-dipole decay
4I°15/2 → (7,5/2)17/2608.3461ground–closed–no other level can be reached by electric-dipole decay
4I°15/2 → (15/2,1)15/2592.3371ground3.600e+05 measured1.63 % from measured data614I°13/2 1.63 % (long-lived)
4I°15/2 → (15/2,2)13/2530.2736ground2.700e+05 measured≥ 3.26 % from measured data≤ 314I°13/2 3.26 % (long-lived); 2 more possible paths without a listed rate
4I°15/2 → (6,3/2)15/2533.1565ground2.200e+05 measured≥ 8.03 % from measured data≤ 124I°13/2 8.06 % (long-lived); 2 more possible paths 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 Ho 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
4I°13/2(34366)11/2345.4665345.3675867.7903E10.976 measured3.900e+06 measured8.97G. Nave, J. Opt. Soc. Am. B 20, 2193 (2003), Table 2
4I°15/2(25273)15/2395.6850395.5730757.6544E11.756 measured6.300e+06 measured99.5G. Nave, J. Opt. Soc. Am. B 20, 2193 (2003), Table 2
4I°15/2(24760)13/2403.8751403.7610742.2900E10.739 measured1.200e+06 measured99.2G. Nave, J. Opt. Soc. Am. B 20, 2193 (2003), Table 2
4I°15/2(24741)13/2404.1952404.0811741.7021E14.125 NIST3.730e+07 NIST82.4NIST ASD (accuracy n/a)
4I°15/2(15/2,1)15/2405.5018405.3873739.3122E19.236 NIST1.620e+08 NIST81NIST ASD (accuracy n/a)
4I°15/2(24377)15/2410.2243410.1085730.8014E11.775 measured5.780e+06 measured100G. Nave, J. Opt. Soc. Am. B 20, 2193 (2003), Table 2
4I°15/2(15/2,1)17/2410.4957410.3799730.3181E19.760 NIST1.550e+08 NIST75.9NIST ASD (accuracy n/a)
4I°13/2(13/2,1)13/2410.9779410.8619729.4613E19.794 measured2.000e+08 measured100G. Nave, J. Opt. Soc. Am. B 20, 2193 (2003), Table 2
4I°15/2(24264)17/2412.1339412.0176727.4152E12.972 measured1.420e+07 measured99.7G. Nave, J. Opt. Soc. Am. B 20, 2193 (2003), Table 2
4I°13/2(13/2,1)15/2412.8325412.7161726.1843E110.85 measured2.120e+08 measured99.6G. Nave, J. Opt. Soc. Am. B 20, 2193 (2003), Table 2
4I°15/2(15/2,1)13/2416.4199416.3026719.9282E16.690 NIST8.970e+07 NIST84.3NIST ASD (accuracy n/a)
4I°15/2(13/2,2)13/2417.4374417.3197718.1735E13.601 NIST2.580e+07 NIST82.6NIST ASD (accuracy n/a)
4I°15/2(13/2,2)15/2419.5521419.4339714.5535E11.504 measured3.880e+06 measured100G. Nave, J. Opt. Soc. Am. B 20, 2193 (2003), Table 2
4I°13/2(13/2,1)11/2422.8316422.7125709.0116E17.018 NIST1.100e+08 NIST100NIST ASD (accuracy n/a)
4I°15/2(13/2,2)17/2425.5578425.4380704.4694E12.806 NIST1.150e+07 NIST100NIST ASD (accuracy n/a)
4I°15/2(5,5/2)15/2426.5251426.4051702.8718E11.506 measured3.700e+06 measured99.2G. Nave, J. Opt. Soc. Am. B 20, 2193 (2003), Table 2
4I°15/2(5,5/2)13/2435.1953435.0730688.8688E12.251 NIST8.900e+06 NIST92.6NIST ASD (accuracy n/a)
4I°15/28F13/2493.6256493.4878607.3277E1 (intercombination)0.532 measured3.400e+05 measured89.1G. Nave, J. Opt. Soc. Am. B 20, 2193 (2003), Table 2
4I°15/2(6,5/2)13/2494.0392493.9013606.8192E11.472 NIST2.600e+06 NIST100NIST ASD (accuracy n/a)
4I°15/2(6,5/2)15/2498.1347497.9958601.8301E11.041 measured1.110e+06 measured95.7G. Nave, J. Opt. Soc. Am. B 20, 2193 (2003), Table 2
4I°13/2(25273)15/2503.7040503.5636595.1759E10.174 measured2.990e+04 measured0.472G. Nave, J. Opt. Soc. Am. B 20, 2193 (2003), Table 2
4I°13/2(24760)13/2517.0516516.9076579.8115E10.067 measured4.700e+03 measured0.389G. Nave, J. Opt. Soc. Am. B 20, 2193 (2003), Table 2
4I°13/2(24741)13/2517.5764517.4323579.2236E10.581 measured3.520e+05 measured0.778G. Nave, J. Opt. Soc. Am. B 20, 2193 (2003), Table 2
4I°15/2(15/2,2)13/2530.2736530.1261565.3543E10.527 measured2.700e+05 measured96.7G. Nave, J. Opt. Soc. Am. B 20, 2193 (2003), Table 2
4I°15/2(6,3/2)15/2533.1565533.0082562.2973E10.513 measured2.200e+05 measured92.4G. Nave, J. Opt. Soc. Am. B 20, 2193 (2003), Table 2
4I°15/2(15/2,2)15/2536.1490536.0000559.1588E10.603 measured2.990e+05 measured99.9G. Nave, J. Opt. Soc. Am. B 20, 2193 (2003), Table 2
4I°13/2(5,5/2)13/2569.5251569.3671526.3903E10.576 measured2.600e+05 measured2.7G. Nave, J. Opt. Soc. Am. B 20, 2193 (2003), Table 2
4I°15/2(15/2,1)13/2586.1888586.0264511.4264E10.951 measured6.500e+05 measured99.5G. Nave, J. Opt. Soc. Am. B 20, 2193 (2003), Table 2
4I°13/2(13/2,1)11/2588.4624588.2993509.4505E11.025 measured8.700e+05 measured100G. Nave, J. Opt. Soc. Am. B 20, 2193 (2003), Table 2
4I°15/2(15/2,1)15/2592.3371592.1730506.1180E10.769 measured3.600e+05 measured97.9G. Nave, J. Opt. Soc. Am. B 20, 2193 (2003), Table 2
4I°15/2(15/2,1)17/2598.4505598.2848500.9478E11.324 measured9.200e+05 measured100G. Nave, J. Opt. Soc. Am. B 20, 2193 (2003), Table 2
4I°15/2(7,5/2)17/2608.3461608.1778492.7991E1––––
4I°15/2(7,3/2)15/2660.6739660.4915453.7677E1––––
4I°13/28F13/2673.9194673.7334444.8491E1 (intercombination)0.298 measured4.200e+04 measured11G. Nave, J. Opt. Soc. Am. B 20, 2193 (2003), Table 2
4I°13/2(6,5/2)13/2674.6905674.5043444.3407E10.740 measured2.580e+05 measured10.7G. Nave, J. Opt. Soc. Am. B 20, 2193 (2003), Table 2
4I°13/2(6,5/2)15/2682.3521682.1639439.3515E10.368 measured5.400e+04 measured4.66G. Nave, J. Opt. Soc. Am. B 20, 2193 (2003), Table 2
4I°13/2(15/2,2)13/2744.1312743.9263402.8758E10.161 measured9.100e+03 measured3.26G. Nave, J. Opt. Soc. Am. B 20, 2193 (2003), Table 2
4I°13/2(6,3/2)15/2749.8208749.6144399.8188E10.253 measured1.920e+04 measured8.06G. Nave, J. Opt. Soc. Am. B 20, 2193 (2003), Table 2
4I°13/2(15/2,1)15/2872.4039872.1644343.6395E10.177 measured6.000e+03 measured1.63G. Nave, J. Opt. Soc. Am. B 20, 2193 (2003), Table 2

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.

Ho energy levels

LevelEnergy (cm⁻¹)JParityLifetimegJHyperfine A (MHz)Hyperfine B (MHz)Lifetime sourceHyperfine source
4I°15/20.00015/2oddstable1.1951800.584-1668.01–Dankwort, Ferch, Gebauer, Z. Phys. 267, 229 (1974) (abstract)
4I°13/25419.70013/2odd––––––
(7,3/2)15/215136.06015/2even––––––
(7,5/2)17/216438.01017/2even––––––
(15/2,1)17/216709.82017/2even1.09 µs measured–––Den Hartog, Wiese, Lawler, J. Opt. Soc. Am. B 16, 2278 (1999), Table 2–
(15/2,1)15/216882.28015/2even2.72 µs measured–––Den Hartog, Wiese, Lawler, J. Opt. Soc. Am. B 16, 2278 (1999), Table 2–
(15/2,1)13/217059.35013/2even1.53 µs measured–––Den Hartog, Wiese, Lawler, J. Opt. Soc. Am. B 16, 2278 (1999), Table 2–
(15/2,2)15/218651.53015/2even3.34 µs measured–––Den Hartog, Wiese, Lawler, J. Opt. Soc. Am. B 16, 2278 (1999), Table 2–
(6,3/2)15/218756.22015/2even4.2 µs measured1.03––Den Hartog, Wiese, Lawler, J. Opt. Soc. Am. B 16, 2278 (1999), Table 2–
(15/2,2)13/218858.19013/2even3.58 µs measured–––Den Hartog, Wiese, Lawler, J. Opt. Soc. Am. B 16, 2278 (1999), Table 2–
(6,5/2)15/220074.89015/2even862 ns measured–––Den Hartog, Wiese, Lawler, J. Opt. Soc. Am. B 16, 2278 (1999), Table 2–
(6,5/2)13/220241.31013/2even414 ns measured–––Den Hartog, Wiese, Lawler, J. Opt. Soc. Am. B 16, 2278 (1999), Table 2–
8F13/220258.27013/2even2.62 µs measured–––Den Hartog, Wiese, Lawler, J. Opt. Soc. Am. B 16, 2278 (1999), Table 2–
(13/2,1)11/222413.14011/2even1.15 µs measured–––Den Hartog, Wiese, Lawler, J. Opt. Soc. Am. B 16, 2278 (1999), Table 2–
(5,5/2)13/222978.19013/2even104 ns measured–––Den Hartog, Wiese, Lawler, J. Opt. Soc. Am. B 16, 2278 (1999), Table 2–
(5,5/2)15/223445.28015/2even268 ns measured1.012––Den Hartog, Wiese, Lawler, J. Opt. Soc. Am. B 16, 2278 (1999), Table 2–
(13/2,2)17/223498.57017/2even100 ns measured–––Den Hartog, Wiese, Lawler, J. Opt. Soc. Am. B 16, 2278 (1999), Table 2–
(13/2,2)15/223834.94015/2even258 ns measured–––Den Hartog, Wiese, Lawler, J. Opt. Soc. Am. B 16, 2278 (1999), Table 2–
(13/2,2)13/223955.69013/2even32 ns measured–––Den Hartog, Wiese, Lawler, J. Opt. Soc. Am. B 16, 2278 (1999), Table 2–
(15/2,1)13/224014.22013/2even9.4 ns measured–––Den Hartog, Wiese, Lawler, J. Opt. Soc. Am. B 16, 2278 (1999), Table 2–
(24264)17/224263.96017/2even70.2 ns measured–––Den Hartog, Wiese, Lawler, J. Opt. Soc. Am. B 16, 2278 (1999), Table 2–
(15/2,1)17/224360.79017/2even4.9 ns measured–654.9-620Den Hartog, Wiese, Lawler, J. Opt. Soc. Am. B 16, 2278 (1999), Table 2Miao, Hostetter, Stratis, Saffman, Phys. Rev. A 89, 041401(R) (2014)
(24377)15/224376.91015/2even173 ns measured–––Den Hartog, Wiese, Lawler, J. Opt. Soc. Am. B 16, 2278 (1999), Table 2–
(15/2,1)15/224660.80015/2even5 ns measured–––Den Hartog, Wiese, Lawler, J. Opt. Soc. Am. B 16, 2278 (1999), Table 2–
(24741)13/224740.52013/2even22.1 ns measured–––Den Hartog, Wiese, Lawler, J. Opt. Soc. Am. B 16, 2278 (1999), Table 2–
(24760)13/224760.13013/2even827 ns measured–––Den Hartog, Wiese, Lawler, J. Opt. Soc. Am. B 16, 2278 (1999), Table 2–
(25273)15/225272.63015/2even158 ns measured–––Den Hartog, Wiese, Lawler, J. Opt. Soc. Am. B 16, 2278 (1999), Table 2–
(13/2,1)11/229069.78011/2even9.4 ns measured–––Den Hartog, Wiese, Lawler, J. Opt. Soc. Am. B 16, 2278 (1999), Table 2–
(13/2,1)15/229642.60015/2even4.7 ns measured–––Den Hartog, Wiese, Lawler, J. Opt. Soc. Am. B 16, 2278 (1999), Table 2–
(13/2,1)13/229751.91013/2even5 ns measured–––Den Hartog, Wiese, Lawler, J. Opt. Soc. Am. B 16, 2278 (1999), Table 2–
(34366)11/234366.07011/2even23 ns measured1.104––Den Hartog, Wiese, Lawler, J. Opt. Soc. Am. B 16, 2278 (1999), Table 2–

Ho⁺ ionisation limit 48567.00 cm⁻¹ = 6.02154 eV (205.901 nm)

Sources

165Ho has I=7/2; hyperfine convention E = A K/2 + B [3K(K+1)/4 - I(I+1)J(J+1)] / [2I(2I-1)J(2J-1)], K = F(F+1)-I(I+1)-J(J+1) (ground state F=4..11, cooling on F=11 -> F'=12). The Den Hartog et al. 1999 lifetime table and the Nave 2003 transition-rate table were read from the publisher abstract pages, whose HTML embeds the tables, through an automated page reader (direct download is captcha-blocked), not from the PDFs; the even-parity lifetime table was read twice with identical results, every row was matched to a NIST level by energy and J, and the Nave A values reproduce 1/tau for the single-branch levels (e.g. 204e6 s^-1 <-> 4.9 ns, 0.92e6 <-> 1090 ns). Lifetime uncertainties are the blanket +-5% (+-10%/+-15% where footnoted). Nave wavelengths quoted in notes are air wavelengths. Extra fields beyond SCHEMA.md: top-level ionization_limit; level fields lifetime_other, level_energy_measured, C_kHz/D_kHz inside the ground-state hyperfine entry; transition fields linewidth_MHz / linewidth_kHz, wavenumber_cm, leak_to_metastable, alternatives. rme_J_ea0 values are derived from the Nave A coefficient of the same entry (schema convention, J' = upper level). g_J without a literature source is copied from the NIST levels file (few exist for Ho I).

Atoms with measured data

All elements: periodic table