Atomic energy level diagrams

Niobium energy level diagram

Energy levels and transitions of neutral niobium (Nb I): the 90 strongest classified lines below 2 µm from the NIST Atomic Spectra Database and the 65 levels they connect, each line with its vacuum wavelength, frequency and, for 90 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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Niobium energy level diagram with transition wavelengths and dipole matrix elements

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

Key transitions of niobium

Transitionλ vac (nm)λ air (nm)ν (THz)|⟨J‖er‖J′⟩| (ea₀)A (s⁻¹)Γ/2π up. (MHz)branch (%)Use
a 4H13/2 – 4I°15/2413.1091412.9926725.69801(10)≈6.5507.707e+078.511100second proposed laser-cooling line from metastable a4H13/…
a 4H13/2 – z 4I°15/2463.1405463.0108647.30348(10)≈5.6964.136e+07––proposed laser-cooling line from metastable a4H13/2 at 46…

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).

93Nb hyperfine structure (I = 9/2)

LevelA (MHz)B (MHz)Shift of each F level from the centre of gravity (MHz)
a 6D1/21868.2184(18)–F=4: -5137.60 F=5: +4203.49
a 6D3/2852.5428(21)-64.57(4)F=3: -7063.07 F=4: -3609.85 F=5: +666.31 F=6: +5738.52
a 6D5/2719.4759(18)-47.60(4)F=2: -9914.61 F=3: -7741.90 F=4: -4850.51 F=5: -1245.20 F=6: +3068.09 F=7: +8082.20
a 6D7/2690.1978(16)20.48(8)F=1: -13276.92 F=2: -11899.45 F=3: -9832.64 F=4: -7075.75 F=5: -3627.80 F=6: +512.41 F=7: +5346.35 F=8: +10875.73
a 6D9/2691.6141(22)132.75(12)F=0: -17056.60 F=1: -16372.36 F=2: -15002.97 F=3: -12946.56 F=4: -10200.39 F=5: -6760.75 F=6: -2623.05 F=7: +2218.24 F=8: +7769.60 F=9: +14038.37
a 4F3/2644.2(5)32.80(13)F=3: -5299.29 F=4: -2744.51 F=5: +469.45 F=6: +4356.28
a 4F5/2372.4853(17)33.34(4)F=2: -5106.39 F=3: -3998.94 F=4: -2518.44 F=5: -661.57 F=6: +1575.84 F=7: +4198.80
a 4F7/2292.2022(16)44.93(5)F=1: -5604.30 F=2: -5026.31 F=3: -4158.00 F=4: -2997.75 F=5: -1543.42 F=6: +207.65 F=7: +2258.68 F=8: +4613.42
a 4F9/2269.6320(26)64.31(13)F=0: -6643.91 F=1: -6377.85 F=2: -5845.29 F=3: -5045.33 F=4: -3976.62 F=5: -2637.40 F=6: -1025.41 F=7: +862.01 F=8: +3028.00 F=9: +5476.13
a 4P3/2497.7569(16)59.902(14)F=3: -4079.04 F=4: -2127.95 F=5: +348.36 F=6: +3374.84
a 4P5/2343.1670(5)-80.454(9)F=2: -4755.42 F=3: -3701.78 F=4: -2306.32 F=5: -577.08 F=6: +1475.89 F=7: +3840.51
a 4D1/21997.0(11)–F=4: -5491.75 F=5: +4493.25
a 4D3/2-143.322(22)-10.76(18)F=3: +1177.48 F=4: +611.36 F=5: -103.01 F=6: -970.12
a 4D5/2-407.861(4)35.06(8)F=2: +5624.15 F=3: +4390.05 F=4: +2748.68 F=5: +703.53 F=6: -1741.00 F=7: -4579.67
a 4D7/2-477.037(4)126.90(8)F=1: +9241.13 F=2: +8268.93 F=3: +6814.40 F=4: +4882.08 F=5: +2478.01 F=6: -390.26 F=7: -3713.66 F=8: -7481.61
a 6S5/2-639.379(8)-0.06(9)F=2: +8791.43 F=3: +6873.31 F=4: +4315.81 F=5: +1118.93 F=6: -2717.35 F=7: -7193.02
a 4H13/2662(20)–F=2: -22342.50 F=3: -20356.50 F=4: -17708.50 F=5: -14398.50 F=6: -10426.50 F=7: -5792.50 F=8: -496.50 F=9: +5461.50 F=10: +12081.50 F=11: +19363.50
b 4F5/2338.500–F=2: -4654.38 F=3: -3638.88 F=4: -2284.88 F=5: -592.38 F=6: +1438.62 F=7: +3808.12
z 6D°1/21713.50(20)–F=4: -4712.12 F=5: +3855.38
z 4D°1/2-794.7(5)–F=4: +2185.43 F=5: -1788.08
z 4D°3/2597.4(3)–F=3: -4928.55 F=4: -2538.95 F=5: +448.05 F=6: +4032.45
z 6D°9/2733.9(4)–F=0: -18164.03 F=1: -17430.12 F=2: -15962.33 F=3: -13760.62 F=4: -10825.02 F=5: -7155.52 F=6: -2752.12 F=7: +2385.18 F=8: +8256.38 F=9: +14861.48
z 4D°5/2809.80(10)–F=2: -11134.75 F=3: -8705.35 F=4: -5466.15 F=5: -1417.15 F=6: +3441.65 F=7: +9110.25
z 4D°7/2872.600–F=1: -16797.55 F=2: -15052.35 F=3: -12434.55 F=4: -8944.15 F=5: -4581.15 F=6: +654.45 F=7: +6762.65 F=8: +13743.45
z 4P°1/2-268.0(20)–F=4: +737.00 F=5: -603.00
z 4G°5/2-78.50(20)–F=2: +1079.38 F=3: +843.88 F=4: +529.88 F=5: +137.38 F=6: -333.62 F=7: -883.12
z 4P°3/2-138.9(3)–F=3: +1145.92 F=4: +590.33 F=5: -104.17 F=6: -937.58
z 4G°7/2430.30(20)–F=1: -8283.27 F=2: -7422.68 F=3: -6131.77 F=4: -4410.57 F=5: -2259.07 F=6: +322.73 F=7: +3334.82 F=8: +6777.23
z 4F°3/2-16.6(3)–F=3: +136.95 F=4: +70.55 F=5: -12.45 F=6: -112.05
z 4G°9/2632.60(10)–F=0: -15656.85 F=1: -15024.25 F=2: -13759.05 F=3: -11861.25 F=4: -9330.85 F=5: -6167.85 F=6: -2372.25 F=7: +2055.95 F=8: +7116.75 F=9: +12810.15
z 4F°5/2514.70(20)–F=2: -7077.12 F=3: -5533.02 F=4: -3474.22 F=5: -900.73 F=6: +2187.47 F=7: +5790.38
z 4P°5/2103.5(4)–F=2: -1423.12 F=3: -1112.62 F=4: -698.62 F=5: -181.12 F=6: +439.88 F=7: +1164.38
y 6F°1/21474.3(6)–F=4: -4054.32 F=5: +3317.18
z 4F°7/2592.20(10)–F=1: -11399.85 F=2: -10215.45 F=3: -8438.85 F=4: -6070.05 F=5: -3109.05 F=6: +444.15 F=7: +4589.55 F=8: +9327.15
y 6F°3/2266.9(5)–F=3: -2201.93 F=4: -1134.33 F=5: +200.18 F=6: +1801.58
z 4G°11/2752.30(10)–F=1: -22004.78 F=2: -20500.17 F=3: -18243.28 F=4: -15234.08 F=5: -11472.58 F=6: -6958.77 F=7: -1692.67 F=8: +4325.73 F=9: +11096.42 F=10: +18619.42
z 6P°3/290.9(4)–F=3: -749.92 F=4: -386.32 F=5: +68.17 F=6: +613.58
y 6F°5/2227.50(10)–F=2: -3128.12 F=3: -2445.62 F=4: -1535.62 F=5: -398.12 F=6: +966.88 F=7: +2559.38
z 4F°9/2593.8(5)–F=0: -14696.55 F=1: -14102.75 F=2: -12915.15 F=3: -11133.75 F=4: -8758.55 F=5: -5789.55 F=6: -2226.75 F=7: +1929.85 F=8: +6680.25 F=9: +12024.45
z 6P°5/2136.80(20)–F=2: -1881.00 F=3: -1470.60 F=4: -923.40 F=5: -239.40 F=6: +581.40 F=7: +1539.00
y 6F°7/2138.6(3)–F=1: -2668.05 F=2: -2390.85 F=3: -1975.05 F=4: -1420.65 F=5: -727.65 F=6: +103.95 F=7: +1074.15 F=8: +2182.95
z 6P°7/2194.7(3)–F=1: -3747.97 F=2: -3358.57 F=3: -2774.47 F=4: -1995.67 F=5: -1022.17 F=6: +146.03 F=7: +1508.92 F=8: +3066.53
y 6F°9/2112.4(4)–F=0: -2781.90 F=1: -2669.50 F=2: -2444.70 F=3: -2107.50 F=4: -1657.90 F=5: -1095.90 F=6: -421.50 F=7: +365.30 F=8: +1264.50 F=9: +2276.10
y 6F°11/244.90(10)–F=1: -1313.33 F=2: -1223.53 F=3: -1088.83 F=4: -909.23 F=5: -684.73 F=6: -415.32 F=7: -101.03 F=8: +258.18 F=9: +662.27 F=10: +1111.28
y 6D°1/21537.900–F=4: -4229.23 F=5: +3460.28
y 4F°3/2559.7(4)–F=3: -4617.52 F=4: -2378.72 F=5: +419.77 F=6: +3777.97
y 4F°5/2265.9(9)–F=2: -3656.12 F=3: -2858.43 F=4: -1794.83 F=5: -465.32 F=6: +1130.08 F=7: +2991.38
y 6D°3/2933(13)–F=3: -7698.90 F=4: -3966.10 F=5: +699.90 F=6: +6299.10
y 4F°7/2297.6(7)–F=1: -5728.80 F=2: -5133.60 F=3: -4240.80 F=4: -3050.40 F=5: -1562.40 F=6: +223.20 F=7: +2306.40 F=8: +4687.20
y 6D°5/2804(6)–F=2: -11056.38 F=3: -8644.08 F=4: -5427.68 F=5: -1407.17 F=6: +3417.43 F=7: +9046.12
y 4F°9/2337.4(8)–F=0: -8350.65 F=1: -8013.25 F=2: -7338.45 F=3: -6326.25 F=4: -4976.65 F=5: -3289.65 F=6: -1265.25 F=7: +1096.55 F=8: +3795.75 F=9: +6832.35
x 6D°1/2430.300–F=4: -1183.33 F=5: +968.17
x 6D°3/2104(5)–F=3: -854.70 F=4: -440.30 F=5: +77.70 F=6: +699.30
y 4D°1/2506(4)–F=4: -1391.50 F=5: +1138.50
y 6D°7/2378.400–F=1: -7284.20 F=2: -6527.40 F=3: -5392.20 F=4: -3878.60 F=5: -1986.60 F=6: +283.80 F=7: +2932.60 F=8: +5959.80
z 2G°7/2181.300-21.000F=1: -3499.65 F=2: -3134.05 F=3: -2586.28 F=4: -1857.08 F=5: -947.45 F=6: +141.35 F=7: +1407.83 F=8: +2850.22
y 4D°3/239.9(6)–F=3: -329.18 F=4: -169.57 F=5: +29.93 F=6: +269.32
x 6D°5/2196(4)–F=2: -2700.50 F=3: -2111.30 F=4: -1325.70 F=5: -343.70 F=6: +834.70 F=7: +2209.50
y 6D°9/2405.70047.000F=0: -10019.53 F=1: -9616.44 F=2: -8809.94 F=3: -7599.37 F=4: -5983.75 F=5: -3961.78 F=6: -1531.82 F=7: +1308.08 F=8: +4560.21 F=9: +8227.17
x 6D°7/2384.7(22)–F=1: -7405.48 F=2: -6636.07 F=3: -5481.98 F=4: -3943.18 F=5: -2019.67 F=6: +288.52 F=7: +2981.43 F=8: +6059.02
y 4D°7/2-144.0(4)–F=1: +2772.00 F=2: +2484.00 F=3: +2052.00 F=4: +1476.00 F=5: +756.00 F=6: -108.00 F=7: -1116.00 F=8: -2268.00
x 6D°9/2525.10(10)–F=0: -12996.23 F=1: -12471.12 F=2: -11420.92 F=3: -9845.62 F=4: -7745.23 F=5: -5119.73 F=6: -1969.12 F=7: +1706.58 F=8: +5907.38 F=9: +10633.27
z 4I°15/2627(20)–F=3: -23986.58 F=4: -21478.17 F=5: -18342.67 F=6: -14580.08 F=7: -10190.38 F=8: -5173.57 F=9: +470.32 F=10: +6741.32 F=11: +13639.42 F=12: +21164.62
4I°15/2299(20)–F=3: -11429.10 F=4: -10233.90 F=5: -8739.90 F=6: -6947.10 F=7: -4855.50 F=8: -2465.10 F=9: +224.10 F=10: +3212.10 F=11: +6498.90 F=12: +10084.50

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

Closed and nearly closed transitions of niobium

Transitionλ vacuum (nm)Lower levelA (s⁻¹)Leak per scattered photonPhotons before a leakWhere the leak goes
a 4H13/2 → 4I°15/2413.1091metastable7.707e+07 semi-empiricalclosed–no other level can be reached by electric-dipole decay
a 4H13/2 → z 4I°15/2463.1405metastable4.136e+07 semi-empiricalclosed–no other level can be reached by electric-dipole decay
a 6D9/2 → y 6F°11/2406.0075metastable1.280e+08 measured0.286 % from semi-empirical calc.350a 4F9/2 0.281 % (long-lived); b 4F9/2 ≈ 2.12 × 10−5 (long-lived); a 4G9/2 ≈ 1.91 × 10−5 (long-lived); 14 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 Nb 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
a 6D7/2x 6D°9/2366.5732366.4688817.8242E12.080 measured1.780e+07 measured20.3Duquette, Den Hartog, Lawler, JQSRT 35, 281 (1986), as compiled in R. L. Kurucz gf4100ddl…
a 6D5/2y 4D°7/2367.5829367.4782815.5779E1 (intercombination)0.899 measured4.120e+06 measured12Duquette, Den Hartog, Lawler, JQSRT 35, 281 (1986), as compiled in R. L. Kurucz gf4100ddl…
a 6D5/2x 6D°7/2369.8898369.7845810.4913E12.827 measured4.000e+07 measured30Duquette, Den Hartog, Lawler, JQSRT 35, 281 (1986), as compiled in R. L. Kurucz gf4100ddl…
a 6D1/2y 4D°3/2371.2388371.1332807.5462E1 (intercombination)1.064 measured1.120e+07 measured25.8Duquette, Den Hartog, Lawler, JQSRT 35, 281 (1986), as compiled in R. L. Kurucz gf4100ddl…
a 6D9/2x 6D°9/2371.4069371.3012807.1807E14.326 measured7.400e+07 measured84.4Duquette, Den Hartog, Lawler, JQSRT 35, 281 (1986), as compiled in R. L. Kurucz gf4100ddl…
a 6D3/2x 6D°5/2372.7289372.6229804.3177E13.033 measured6.000e+07 measured42Duquette, Den Hartog, Lawler, JQSRT 35, 281 (1986), as compiled in R. L. Kurucz gf4100ddl…
a 6D7/2x 6D°7/2374.0856373.9793801.4007E13.486 measured5.880e+07 measured44.1Duquette, Den Hartog, Lawler, JQSRT 35, 281 (1986), as compiled in R. L. Kurucz gf4100ddl…
a 6D7/2y 6D°9/2374.1903374.0839801.1765E11.709 measured1.130e+07 measured17.1Duquette, Den Hartog, Lawler, JQSRT 35, 281 (1986), as compiled in R. L. Kurucz gf4100ddl…
a 6D1/2y 4D°1/2374.2834374.1771800.9771E1 (intercombination)0.979 measured1.850e+07 measured27.6Duquette, Den Hartog, Lawler, JQSRT 35, 281 (1986), as compiled in R. L. Kurucz gf4100ddl…
a 6D1/2x 6D°3/2374.3452374.2388800.8449E12.440 measured5.750e+07 measured42Duquette, Den Hartog, Lawler, JQSRT 35, 281 (1986), as compiled in R. L. Kurucz gf4100ddl…
a 6D5/2x 6D°5/2376.0621375.9553797.1886E12.166 measured2.980e+07 measured20.9Duquette, Den Hartog, Lawler, JQSRT 35, 281 (1986), as compiled in R. L. Kurucz gf4100ddl…
a 6D3/2y 4D°1/2376.4558376.3489796.3549E1 (intercombination)1.257 measured3.000e+07 measured44.7Duquette, Den Hartog, Lawler, JQSRT 35, 281 (1986), as compiled in R. L. Kurucz gf4100ddl…
a 6D1/2x 6D°1/2376.6138376.5068796.0209E11.014 measured1.950e+07 measured15.6Duquette, Den Hartog, Lawler, JQSRT 35, 281 (1986), as compiled in R. L. Kurucz gf4100ddl…
a 6D5/2y 4D°3/2376.7206376.6136795.7952E1 (intercombination)0.875 measured7.250e+06 measured16.7Duquette, Den Hartog, Lawler, JQSRT 35, 281 (1986), as compiled in R. L. Kurucz gf4100ddl…
a 6D5/2z 2G°7/2377.2917377.1846794.5906E1 (intercombination)0.990 measured4.620e+06 measured26Duquette, Den Hartog, Lawler, JQSRT 35, 281 (1986), as compiled in R. L. Kurucz gf4100ddl…
a 6D5/2y 6D°7/2378.2085378.1011792.6644E11.627 measured1.240e+07 measured32Duquette, Den Hartog, Lawler, JQSRT 35, 281 (1986), as compiled in R. L. Kurucz gf4100ddl…
a 6D3/2x 6D°1/2378.8136378.7060791.3984E12.312 measured9.960e+07 measured79.7Duquette, Den Hartog, Lawler, JQSRT 35, 281 (1986), as compiled in R. L. Kurucz gf4100ddl…
a 6D9/2x 6D°7/2379.1209379.0133790.7569E12.432 measured2.750e+07 measured20.6Duquette, Den Hartog, Lawler, JQSRT 35, 281 (1986), as compiled in R. L. Kurucz gf4100ddl…
a 6D9/2y 6D°9/2379.2280379.1204790.5335E13.813 measured5.400e+07 measured81.5Duquette, Den Hartog, Lawler, JQSRT 35, 281 (1986), as compiled in R. L. Kurucz gf4100ddl…
a 6D5/2x 6D°3/2379.9200379.8122789.0936E12.653 measured6.500e+07 measured47.4Duquette, Den Hartog, Lawler, JQSRT 35, 281 (1986), as compiled in R. L. Kurucz gf4100ddl…
a 6D7/2x 6D°5/2380.4004380.2924788.0971E12.903 measured5.170e+07 measured36.2Duquette, Den Hartog, Lawler, JQSRT 35, 281 (1986), as compiled in R. L. Kurucz gf4100ddl…
a 6D9/2z 2G°9/2380.4952380.3872787.9008E1 (intercombination)1.887 measured1.310e+07 measured74.3Duquette, Den Hartog, Lawler, JQSRT 35, 281 (1986), as compiled in R. L. Kurucz gf4100ddl…
a 6D3/2y 6D°5/2381.2113381.1031786.4207E11.248 measured9.500e+06 measured37Duquette, Den Hartog, Lawler, JQSRT 35, 281 (1986), as compiled in R. L. Kurucz gf4100ddl…
a 6D7/2z 2G°7/2381.6586381.5503785.4991E1 (intercombination)1.294 measured7.630e+06 measured42.9Duquette, Den Hartog, Lawler, JQSRT 35, 281 (1986), as compiled in R. L. Kurucz gf4100ddl…
a 6D7/2y 6D°7/2382.5967382.4882783.5729E11.933 measured1.690e+07 measured43.6Duquette, Den Hartog, Lawler, JQSRT 35, 281 (1986), as compiled in R. L. Kurucz gf4100ddl…
a 6D1/2y 6D°3/2383.6259383.5171781.4708E10.867 measured6.750e+06 measured37Duquette, Den Hartog, Lawler, JQSRT 35, 281 (1986), as compiled in R. L. Kurucz gf4100ddl…
a 6D3/2y 4F°5/2386.0041385.8947776.6561E1 (intercombination)1.039 measured6.340e+06 measured26.3Duquette, Den Hartog, Lawler, JQSRT 35, 281 (1986), as compiled in R. L. Kurucz gf4100ddl…
a 6D9/2y 6D°7/2387.8649387.7550772.9300E11.368 measured8.120e+06 measured20.9Duquette, Den Hartog, Lawler, JQSRT 35, 281 (1986), as compiled in R. L. Kurucz gf4100ddl…
a 6D5/2y 4F°7/2387.9912387.8813772.6785E1 (intercombination)1.549 measured1.040e+07 measured39.4Duquette, Den Hartog, Lawler, JQSRT 35, 281 (1986), as compiled in R. L. Kurucz gf4100ddl…
a 6D7/2y 4F°9/2388.4236388.3135771.8184E1 (intercombination)1.709 measured1.010e+07 measured36Duquette, Den Hartog, Lawler, JQSRT 35, 281 (1986), as compiled in R. L. Kurucz gf4100ddl…
a 6D3/2y 6D°1/2388.7176388.6074771.2347E10.817 measured1.150e+07 measured72.1Duquette, Den Hartog, Lawler, JQSRT 35, 281 (1986), as compiled in R. L. Kurucz gf4100ddl…
a 6D7/2y 6D°5/2389.2393389.1290770.2010E11.354 measured1.050e+07 measured40.8Duquette, Den Hartog, Lawler, JQSRT 35, 281 (1986), as compiled in R. L. Kurucz gf4100ddl…
a 6D5/2y 6D°3/2389.4829389.3725769.7192E11.107 measured1.050e+07 measured57.5Duquette, Den Hartog, Lawler, JQSRT 35, 281 (1986), as compiled in R. L. Kurucz gf4100ddl…
a 4F3/2y 4D°1/2391.0078390.8970766.7174E10.892 measured1.350e+07 measured20.1Duquette, Den Hartog, Lawler, JQSRT 35, 281 (1986), as compiled in R. L. Kurucz gf4100ddl…
a 4F3/2x 6D°1/2393.5519393.4405761.7609E1 (intercombination)0.520 measured4.500e+06 measured3.6Duquette, Den Hartog, Lawler, JQSRT 35, 281 (1986), as compiled in R. L. Kurucz gf4100ddl…
a 6D9/2y 4F°9/2393.8549393.7434761.1748E1 (intercombination)1.665 measured9.190e+06 measured32.7Duquette, Den Hartog, Lawler, JQSRT 35, 281 (1986), as compiled in R. L. Kurucz gf4100ddl…
a 4F5/2y 4D°3/2394.4778394.3662759.9730E11.348 measured1.500e+07 measured34.5Duquette, Den Hartog, Lawler, JQSRT 35, 281 (1986), as compiled in R. L. Kurucz gf4100ddl…
a 4F9/2y 4D°7/2403.3660403.2521743.2269E12.282 measured2.010e+07 measured58.5Duquette, Den Hartog, Lawler, JQSRT 35, 281 (1986), as compiled in R. L. Kurucz gf4100ddl…
a 4F3/2y 4F°3/2403.4335403.3196743.1025E11.002 measured7.750e+06 measured36.9Duquette, Den Hartog, Lawler, JQSRT 35, 281 (1986), as compiled in R. L. Kurucz gf4100ddl…
a 6D9/2y 6F°11/2406.0075405.8928738.3915E17.123 measured1.280e+08 measured96Duquette, Den Hartog, Lawler, JQSRT 35, 281 (1986), as compiled in R. L. Kurucz gf4100ddl…
a 6D7/2y 6F°9/2408.0875407.9723734.6279E15.763 measured9.900e+07 measured81.2Duquette, Den Hartog, Lawler, JQSRT 35, 281 (1986), as compiled in R. L. Kurucz gf4100ddl…
a 4F5/2y 4F°5/2408.6010408.4857733.7046E11.022 measured5.170e+06 measured21.5Duquette, Den Hartog, Lawler, JQSRT 35, 281 (1986), as compiled in R. L. Kurucz gf4100ddl…
a 6D5/2y 6F°7/2410.2074410.0917730.8314E14.557 measured7.620e+07 measured64.8Duquette, Den Hartog, Lawler, JQSRT 35, 281 (1986), as compiled in R. L. Kurucz gf4100ddl…
a 6D1/2z 6P°3/2411.8056411.6895727.9950E10.767 measured4.270e+06 measured19.9Duquette, Den Hartog, Lawler, JQSRT 35, 281 (1986), as compiled in R. L. Kurucz gf4100ddl…
a 6D3/2y 6F°5/2412.4970412.3807726.7749E13.484 measured5.840e+07 measured51.4Duquette, Den Hartog, Lawler, JQSRT 35, 281 (1986), as compiled in R. L. Kurucz gf4100ddl…
a 6D7/2z 6P°7/2413.0589412.9425725.7862E11.251 measured5.620e+06 measured22.8Duquette, Den Hartog, Lawler, JQSRT 35, 281 (1986), as compiled in R. L. Kurucz gf4100ddl…
a 4H13/24I°15/2413.1091412.9926725.6980E16.550 semi-empirical7.707e+07 semi-empirical100Kurucz, R. L., Can. J. Phys. 89, 417 (2011); semi-empirical line list gf4100.pos of 2017-…
a 6D1/2y 6F°3/2413.8256413.7089724.4416E12.244 measured3.600e+07 measured31Duquette, Den Hartog, Lawler, JQSRT 35, 281 (1986), as compiled in R. L. Kurucz gf4100ddl…
a 6D5/2z 6P°5/2414.0595413.9427724.0324E11.107 measured5.830e+06 measured25.7Duquette, Den Hartog, Lawler, JQSRT 35, 281 (1986), as compiled in R. L. Kurucz gf4100ddl…
a 6D9/2y 6F°9/2414.0869413.9701723.9844E12.777 measured2.200e+07 measured18Duquette, Den Hartog, Lawler, JQSRT 35, 281 (1986), as compiled in R. L. Kurucz gf4100ddl…
a 6D3/2z 6P°3/2414.4370414.3201723.3728E10.937 measured6.250e+06 measured29.2Duquette, Den Hartog, Lawler, JQSRT 35, 281 (1986), as compiled in R. L. Kurucz gf4100ddl…
a 6D7/2y 6F°7/2415.3747415.2576721.7399E13.258 measured3.750e+07 measured31.9Duquette, Den Hartog, Lawler, JQSRT 35, 281 (1986), as compiled in R. L. Kurucz gf4100ddl…
a 6D3/2y 6F°3/2416.4829416.3655719.8194E13.045 measured6.500e+07 measured55.9Duquette, Den Hartog, Lawler, JQSRT 35, 281 (1986), as compiled in R. L. Kurucz gf4100ddl…
a 6D5/2y 6F°5/2416.5833416.4659719.6458E13.272 measured5.000e+07 measured44Duquette, Den Hartog, Lawler, JQSRT 35, 281 (1986), as compiled in R. L. Kurucz gf4100ddl…
a 6D1/2y 6F°1/2416.9299416.8124719.0477E12.552 measured9.100e+07 measured77.3Duquette, Den Hartog, Lawler, JQSRT 35, 281 (1986), as compiled in R. L. Kurucz gf4100ddl…
a 6D5/2z 6P°3/2418.5621418.4441716.2437E10.798 measured4.400e+06 measured20.5Duquette, Den Hartog, Lawler, JQSRT 35, 281 (1986), as compiled in R. L. Kurucz gf4100ddl…
a 6D9/2z 6P°7/2419.2067419.0886715.1423E11.868 measured1.200e+07 measured48.7Duquette, Den Hartog, Lawler, JQSRT 35, 281 (1986), as compiled in R. L. Kurucz gf4100ddl…
a 6D7/2z 6P°5/2419.3247419.2065714.9412E11.335 measured8.160e+06 measured35.9Duquette, Den Hartog, Lawler, JQSRT 35, 281 (1986), as compiled in R. L. Kurucz gf4100ddl…
a 6D3/2y 6F°1/2419.6271419.5089714.4258E11.390 measured2.650e+07 measured22.5Duquette, Den Hartog, Lawler, JQSRT 35, 281 (1986), as compiled in R. L. Kurucz gf4100ddl…
a 6D7/2y 6F°5/2421.9135421.7947710.5543E11.106 measured5.500e+06 measured4.84Duquette, Den Hartog, Lawler, JQSRT 35, 281 (1986), as compiled in R. L. Kurucz gf4100ddl…
a 6D9/2z 4F°9/2426.3254426.2055703.2010E1 (intercombination)1.527 measured6.100e+06 measured21.8Duquette, Den Hartog, Lawler, JQSRT 35, 281 (1986), as compiled in R. L. Kurucz gf4100ddl…
a 6D7/2z 4F°7/2428.8192428.6986699.1115E1 (intercombination)1.150 measured4.250e+06 measured16.4Duquette, Den Hartog, Lawler, JQSRT 35, 281 (1986), as compiled in R. L. Kurucz gf4100ddl…
a 4F3/2z 4F°3/2452.4674452.3405662.5725E11.530 measured1.280e+07 measured56.8Duquette, Den Hartog, Lawler, JQSRT 35, 281 (1986), as compiled in R. L. Kurucz gf4100ddl…
a 4F5/2z 4F°5/2454.8093454.6818659.1609E11.626 measured9.490e+06 measured42.2Duquette, Den Hartog, Lawler, JQSRT 35, 281 (1986), as compiled in R. L. Kurucz gf4100ddl…
a 4F7/2z 4F°7/2457.4358457.3077655.3760E12.121 measured1.190e+07 measured45.9Duquette, Den Hartog, Lawler, JQSRT 35, 281 (1986), as compiled in R. L. Kurucz gf4100ddl…
a 4F9/2z 4F°9/2460.8046460.6756650.5847E12.506 measured1.300e+07 measured46.5Duquette, Den Hartog, Lawler, JQSRT 35, 281 (1986), as compiled in R. L. Kurucz gf4100ddl…
a 4H13/2z 4I°15/2463.1405463.0108647.3035E15.696 semi-empirical4.136e+07 semi-empirical–Kurucz, R. L., Can. J. Phys. 89, 417 (2011); semi-empirical line list gf4100.pos of 2017-…
a 4F3/2z 4G°5/2465.0248464.8946644.6806E11.337 measured6.000e+06 measured87.6Duquette, Den Hartog, Lawler, JQSRT 35, 281 (1986), as compiled in R. L. Kurucz gf4100ddl…
a 4F5/2z 4G°7/2466.5134466.3829642.6234E11.645 measured6.750e+06 measured89.1Duquette, Den Hartog, Lawler, JQSRT 35, 281 (1986), as compiled in R. L. Kurucz gf4100ddl…
a 4F9/2z 4G°11/2467.3404467.2096641.4863E12.095 measured7.260e+06 measured–Duquette, Den Hartog, Lawler, JQSRT 35, 281 (1986), as compiled in R. L. Kurucz gf4100ddl…
a 4F7/2z 4G°9/2467.6678467.5369641.0372E11.880 measured7.000e+06 measured89.6Duquette, Den Hartog, Lawler, JQSRT 35, 281 (1986), as compiled in R. L. Kurucz gf4100ddl…
a 6D9/2z 6D°9/2508.0371507.8956590.0995E11.817 measured5.100e+06 measured78.5Duquette, Den Hartog, Lawler, JQSRT 35, 281 (1986), as compiled in R. L. Kurucz gf4100ddl…
a 6D3/2z 6D°1/2513.6178513.4747583.6878E10.826 measured5.100e+06 measured80.6Duquette, Den Hartog, Lawler, JQSRT 35, 281 (1986), as compiled in R. L. Kurucz gf4100ddl…
a 4F3/2z 4D°1/2527.2991527.1523568.5435E11.031 measured7.350e+06 measured77.9Duquette, Den Hartog, Lawler, JQSRT 35, 281 (1986), as compiled in R. L. Kurucz gf4100ddl…
a 4F5/2z 4D°3/2532.0074531.8595563.5118E11.199 measured4.840e+06 measured49.4Duquette, Den Hartog, Lawler, JQSRT 35, 281 (1986), as compiled in R. L. Kurucz gf4100ddl…
a 4F9/2z 4D°7/2534.5647534.4160560.8161E12.055 measured7.000e+06 measured59.7Duquette, Den Hartog, Lawler, JQSRT 35, 281 (1986), as compiled in R. L. Kurucz gf4100ddl…
a 4F7/2z 4D°5/2535.2216535.0728560.1277E11.556 measured5.330e+06 measured49.4Duquette, Den Hartog, Lawler, JQSRT 35, 281 (1986), as compiled in R. L. Kurucz gf4100ddl…
a 4P5/2z 4P°5/2564.3678564.2112531.2005E11.603 measured4.830e+06 measured22.5Duquette, Den Hartog, Lawler, JQSRT 35, 281 (1986), as compiled in R. L. Kurucz gf4100ddl…
a 4D1/2y 4F°3/2570.8053570.6469525.2097E11.355 measured5.000e+06 measured23.8Duquette, Den Hartog, Lawler, JQSRT 35, 281 (1986), as compiled in R. L. Kurucz gf4100ddl…
a 4D3/2y 4F°5/2576.1929576.0331520.2988E11.597 measured4.500e+06 measured18.7Duquette, Den Hartog, Lawler, JQSRT 35, 281 (1986), as compiled in R. L. Kurucz gf4100ddl…
a 4D5/2y 4F°7/2584.0235583.8616513.3226E11.908 measured4.630e+06 measured17.5Duquette, Den Hartog, Lawler, JQSRT 35, 281 (1986), as compiled in R. L. Kurucz gf4100ddl…
a 4D7/2y 4F°9/2590.2223590.0587507.9315E12.089 measured4.300e+06 measured15.3Duquette, Den Hartog, Lawler, JQSRT 35, 281 (1986), as compiled in R. L. Kurucz gf4100ddl…
a 4P3/2z 4P°1/2598.4870598.3213500.9172E11.113 measured5.850e+06 measured31.5Duquette, Den Hartog, Lawler, JQSRT 35, 281 (1986), as compiled in R. L. Kurucz gf4100ddl…
a 4D7/2z 4F°9/2666.2678666.0839449.9579E12.755 measured5.200e+06 measured18.6Duquette, Den Hartog, Lawler, JQSRT 35, 281 (1986), as compiled in R. L. Kurucz gf4100ddl…
a 4D7/2z 4P°5/2704.8771704.6828425.3117E12.596 measured6.500e+06 measured30.3Duquette, Den Hartog, Lawler, JQSRT 35, 281 (1986), as compiled in R. L. Kurucz gf4100ddl…
b 4F5/2x 6D°3/2713.2057713.0092420.3450E1 (intercombination)2.029 measured5.750e+06 measured4.2Duquette, Den Hartog, Lawler, JQSRT 35, 281 (1986), as compiled in R. L. Kurucz gf4100ddl…
a 4D5/2z 4P°3/2716.1436715.9462418.6206E11.741 measured4.180e+06 measured21.7Duquette, Den Hartog, Lawler, JQSRT 35, 281 (1986), as compiled in R. L. Kurucz gf4100ddl…
a 6S5/2z 6P°7/2737.4544737.2513406.5234E13.146 measured6.250e+06 measured25.4Duquette, Den Hartog, Lawler, JQSRT 35, 281 (1986), as compiled in R. L. Kurucz gf4100ddl…
a 6S5/2z 6P°5/2757.6670757.4585395.6784E12.740 measured5.830e+06 measured25.7Duquette, Den Hartog, Lawler, JQSRT 35, 281 (1986), as compiled in R. L. Kurucz gf4100ddl…
a 6S5/2z 6P°3/2772.8805772.6679387.8898E12.289 measured5.750e+06 measured26.9Duquette, Den Hartog, Lawler, JQSRT 35, 281 (1986), as compiled in R. L. Kurucz gf4100ddl…

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, a semi-empirical calculation (Kurucz line list, used only where no measurement or NIST value exists; typically within a factor 2), or a model calculation.

Nb energy levels

LevelEnergy (cm⁻¹)JParityLifetimegJHyperfine A (MHz)Hyperfine B (MHz)Lifetime sourceHyperfine source
a 6D1/20.0001/2evenstable3.3231868.22––Büttgenbach, Dicke, Gebauer, Herschel, Meisel, Z. Phys. A 275, 193 (1975) (atomic-beam ma…
a 6D3/2154.1903/2even–1.863852.543-64.572–Büttgenbach, Dicke, Gebauer, Herschel, Meisel, Z. Phys. A 275, 193 (1975) (atomic-beam ma…
a 6D5/2391.9905/2even–1.652719.476-47.605–Büttgenbach, Dicke, Gebauer, Herschel, Meisel, Z. Phys. A 275, 193 (1975) (atomic-beam ma…
a 6D7/2695.2507/2even–1.582690.19820.475–Büttgenbach, Dicke, Gebauer, Herschel, Meisel, Z. Phys. A 275, 193 (1975) (atomic-beam ma…
a 6D9/21050.2609/2even–1.549691.614132.754–Büttgenbach, Dicke, Gebauer, Herschel, Meisel, Z. Phys. A 275, 193 (1975) (atomic-beam ma…
a 4F3/21142.7903/2even–0.402644.1632.8–Büttgenbach, Dicke, Gebauer, Herschel, Meisel, Z. Phys. A 275, 193 (1975) (atomic-beam ma…
a 4F5/21586.9005/2even–1.029372.48533.341–Büttgenbach, Dicke, Gebauer, Herschel, Meisel, Z. Phys. A 275, 193 (1975) (atomic-beam ma…
a 4F7/22154.1107/2even–1.235292.20244.928–Büttgenbach, Dicke, Gebauer, Herschel, Meisel, Z. Phys. A 275, 193 (1975) (atomic-beam ma…
a 4F9/22805.3609/2even–1.33269.63264.315–Büttgenbach, Dicke, Gebauer, Herschel, Meisel, Z. Phys. A 275, 193 (1975) (atomic-beam ma…
a 4P3/25297.9203/2even–1.721497.75759.902–Fraenkel, Bengtsson, Hanstorp, Nyberg, Persson, Z. Phys. D 8, 171 (1988) (laser-rf double…
a 4P5/25965.4505/2even–1.596343.167-80.454–Fraenkel, Bengtsson, Hanstorp, Nyberg, Persson, Z. Phys. D 8, 171 (1988) (laser-rf double…
a 4D1/28410.9001/2even–0.061997––Fraenkel, Bengtsson, Hanstorp, Nyberg, Persson, Z. Phys. D 8, 171 (1988) (laser-rf double…
a 4D3/28705.3203/2even–1.197-143.322-10.761–Fraenkel, Bengtsson, Hanstorp, Nyberg, Persson, Z. Phys. D 8, 171 (1988) (laser-rf double…
a 4D5/29043.1405/2even–1.36-407.86135.06–Fraenkel, Bengtsson, Hanstorp, Nyberg, Persson, Z. Phys. D 8, 171 (1988) (laser-rf double…
a 4D7/29497.5207/2even–1.42-477.037126.899–Fraenkel, Bengtsson, Hanstorp, Nyberg, Persson, Z. Phys. D 8, 171 (1988) (laser-rf double…
a 6S5/211344.7005/2even–1.99-639.379-0.061–Fraenkel, Bengtsson, Hanstorp, Nyberg, Persson, Z. Phys. D 8, 171 (1988) (laser-rf double…
a 4H13/211524.65013/2even1.22 s theory1.22662–Eustice, Cassella, Stamper-Kurn, Phys. Rev. A 102, 053327 (2020). Note: derived, approxim…Kröger, Eur. Phys. J. D 41, 55 (2007) (laser-induced fluorescence), as tabulated in Kröge…
b 4F5/212692.1205/2even–0.852338.5––Kröger, Eur. Phys. J. D 41, 55 (2007), as compiled in R. L. Kurucz ab410093.dat
z 6D°1/219623.9601/2odd158 ns measured3.011713.5–Duquette & Lawler, Phys. Rev. A 26, 330 (1982), as compiled in R. L. Kurucz life4100.labKröger, Er, Öztürk, Başar, Jarmola, Ferber, Tamanis, Začs, Astron. Astrophys. 516, A70 (2…
z 4D°1/220107.3601/2odd106 ns measured0.02-794.7–Duquette & Lawler, Phys. Rev. A 26, 330 (1982), as compiled in R. L. Kurucz life4100.labKröger, Er, Öztürk, Başar, Jarmola, Ferber, Tamanis, Začs, Astron. Astrophys. 516, A70 (2…
z 4D°3/220383.6203/2odd102 ns measured1.26597.4–Duquette & Lawler, Phys. Rev. A 26, 330 (1982), as compiled in R. L. Kurucz life4100.labKröger, Er, Öztürk, Başar, Jarmola, Ferber, Tamanis, Začs, Astron. Astrophys. 516, A70 (2…
z 6D°9/220733.8809/2odd154 ns measured1.54733.9–Duquette & Lawler, Phys. Rev. A 26, 330 (1982), as compiled in R. L. Kurucz life4100.labKröger, Er, Öztürk, Başar, Jarmola, Ferber, Tamanis, Začs, Astron. Astrophys. 516, A70 (2…
z 4D°5/220837.9805/2odd92.7 ns measured1.39809.8–Duquette & Lawler, Phys. Rev. A 26, 330 (1982), as compiled in R. L. Kurucz life4100.labKröger, Er, Öztürk, Başar, Jarmola, Ferber, Tamanis, Začs, Astron. Astrophys. 516, A70 (2…
z 4D°7/221512.1807/2odd85.3 ns measured1.44872.6–Duquette & Lawler, Phys. Rev. A 26, 330 (1982), as compiled in R. L. Kurucz life4100.labKröger, Er, Öztürk, Başar, Jarmola, Ferber, Tamanis, Začs, Astron. Astrophys. 516, A70 (2…
z 4P°1/222006.7401/2odd53.8 ns measured2.47-268–Duquette & Lawler, Phys. Rev. A 26, 330 (1982), as compiled in R. L. Kurucz life4100.labKröger, Er, Öztürk, Başar, Jarmola, Ferber, Tamanis, Začs, Astron. Astrophys. 516, A70 (2…
z 4G°5/222647.0305/2odd146 ns measured0.578-78.5–Duquette & Lawler, Phys. Rev. A 26, 330 (1982), as compiled in R. L. Kurucz life4100.labKröger, Er, Öztürk, Başar, Jarmola, Ferber, Tamanis, Začs, Astron. Astrophys. 516, A70 (2…
z 4P°3/223006.8603/2odd51.9 ns measured1.61-138.9–Duquette & Lawler, Phys. Rev. A 26, 330 (1982), as compiled in R. L. Kurucz life4100.labKröger, Er, Öztürk, Başar, Jarmola, Ferber, Tamanis, Začs, Astron. Astrophys. 516, A70 (2…
z 4G°7/223022.5607/2odd132 ns measured0.98430.3–Duquette & Lawler, Phys. Rev. A 26, 330 (1982), as compiled in R. L. Kurucz life4100.labKröger, Er, Öztürk, Başar, Jarmola, Ferber, Tamanis, Začs, Astron. Astrophys. 516, A70 (2…
z 4F°3/223243.8703/2odd44.4 ns measured0.416-16.6–Duquette & Lawler, Phys. Rev. A 26, 330 (1982), as compiled in R. L. Kurucz life4100.labKröger, Er, Öztürk, Başar, Jarmola, Ferber, Tamanis, Začs, Astron. Astrophys. 516, A70 (2…
z 4G°9/223536.7709/2odd128 ns measured1.15632.6–Duquette & Lawler, Phys. Rev. A 26, 330 (1982), as compiled in R. L. Kurucz life4100.labKröger, Er, Öztürk, Başar, Jarmola, Ferber, Tamanis, Začs, Astron. Astrophys. 516, A70 (2…
z 4F°5/223574.1405/2odd44.5 ns measured1.061514.7–Duquette & Lawler, Phys. Rev. A 26, 330 (1982), as compiled in R. L. Kurucz life4100.labKröger, Er, Öztürk, Başar, Jarmola, Ferber, Tamanis, Začs, Astron. Astrophys. 516, A70 (2…
z 4P°5/223684.4405/2odd46.6 ns measured1.477103.5–Duquette & Lawler, Phys. Rev. A 26, 330 (1982), as compiled in R. L. Kurucz life4100.labKröger, Er, Öztürk, Başar, Jarmola, Ferber, Tamanis, Začs, Astron. Astrophys. 516, A70 (2…
y 6F°1/223984.8701/2odd8.5 ns measured0.6011474.3–Duquette & Lawler, Phys. Rev. A 26, 330 (1982), as compiled in R. L. Kurucz life4100.labKröger, Er, Öztürk, Başar, Jarmola, Ferber, Tamanis, Začs, Astron. Astrophys. 516, A70 (2…
z 4F°7/224015.1107/2odd38.6 ns measured1.243592.2–Duquette & Lawler, Phys. Rev. A 26, 330 (1982), as compiled in R. L. Kurucz life4100.labKröger, Er, Öztürk, Başar, Jarmola, Ferber, Tamanis, Začs, Astron. Astrophys. 516, A70 (2…
y 6F°3/224164.7903/2odd8.6 ns measured1.06266.9–Duquette & Lawler, Phys. Rev. A 26, 330 (1982), as compiled in R. L. Kurucz life4100.labKröger, Er, Öztürk, Başar, Jarmola, Ferber, Tamanis, Začs, Astron. Astrophys. 516, A70 (2…
z 4G°11/224203.05011/2odd–1.25752.3––Kröger, Er, Öztürk, Başar, Jarmola, Ferber, Tamanis, Začs, Astron. Astrophys. 516, A70 (2…
z 6P°3/224283.3403/2odd46.7 ns measured2.38290.9–Duquette & Lawler, Phys. Rev. A 26, 330 (1982), as compiled in R. L. Kurucz life4100.labKröger, Er, Öztürk, Başar, Jarmola, Ferber, Tamanis, Začs, Astron. Astrophys. 516, A70 (2…
y 6F°5/224396.8005/2odd8.8 ns measured1.306227.5–Duquette & Lawler, Phys. Rev. A 26, 330 (1982), as compiled in R. L. Kurucz life4100.labKröger, Er, Öztürk, Başar, Jarmola, Ferber, Tamanis, Začs, Astron. Astrophys. 516, A70 (2…
z 4F°9/224506.5309/2odd35.8 ns measured1.336593.8–Gao, Geng, Quinet, Wang, Yu, Dai, Astrophys. J. Suppl. 242, 23 (2019), Table 1Kröger, Er, Öztürk, Başar, Jarmola, Ferber, Tamanis, Začs, Astron. Astrophys. 516, A70 (2…
z 6P°5/224543.1305/2odd44 ns measured1.874136.8–Duquette & Lawler, Phys. Rev. A 26, 330 (1982), as compiled in R. L. Kurucz life4100.labKröger, Er, Öztürk, Başar, Jarmola, Ferber, Tamanis, Začs, Astron. Astrophys. 516, A70 (2…
y 6F°7/224769.9107/2odd8.5 ns measured1.38138.6–Duquette & Lawler, Phys. Rev. A 26, 330 (1982), as compiled in R. L. Kurucz life4100.labKröger, Er, Öztürk, Başar, Jarmola, Ferber, Tamanis, Začs, Astron. Astrophys. 516, A70 (2…
z 6P°7/224904.8607/2odd40.6 ns measured1.703194.7–Duquette & Lawler, Phys. Rev. A 26, 330 (1982), as compiled in R. L. Kurucz life4100.labKröger, Er, Öztürk, Başar, Jarmola, Ferber, Tamanis, Začs, Astron. Astrophys. 516, A70 (2…
y 6F°9/225199.8109/2odd8.2 ns measured1.427112.4–Duquette & Lawler, Phys. Rev. A 26, 330 (1982), as compiled in R. L. Kurucz life4100.labKröger, Er, Öztürk, Başar, Jarmola, Ferber, Tamanis, Začs, Astron. Astrophys. 516, A70 (2…
y 6F°11/225680.36011/2odd7.5 ns measured1.4544.9–Rudolph & Helbig, Phys. Lett. 89A, 339 (1982), as compiled in R. L. Kurucz life4100.labKröger, Er, Öztürk, Başar, Jarmola, Ferber, Tamanis, Začs, Astron. Astrophys. 516, A70 (2…
y 6D°1/225879.8101/2odd62.7 ns measured3.221537.9–Duquette & Lawler, Phys. Rev. A 26, 330 (1982), as compiled in R. L. Kurucz life4100.labBouzed, Kröger, Zimmermann, Kronfeldt, Guthöhrlein, Eur. Phys. J. D 23, 57 (2003), as com…
y 4F°3/225930.0103/2odd47.6 ns measured0.467559.7–Duquette & Lawler, Phys. Rev. A 26, 330 (1982), as compiled in R. L. Kurucz life4100.labKröger, Er, Öztürk, Başar, Jarmola, Ferber, Tamanis, Začs, Astron. Astrophys. 516, A70 (2…
y 4F°5/226060.6505/2odd41.5 ns measured1.085265.9–Duquette & Lawler, Phys. Rev. A 26, 330 (1982), as compiled in R. L. Kurucz life4100.labKröger, Er, Öztürk, Başar, Jarmola, Ferber, Tamanis, Začs, Astron. Astrophys. 516, A70 (2…
y 6D°3/226067.0603/2odd54.8 ns measured1.82933.2–Duquette & Lawler, Phys. Rev. A 26, 330 (1982), as compiled in R. L. Kurucz life4100.labKröger, Er, Öztürk, Başar, Jarmola, Ferber, Tamanis, Začs, Astron. Astrophys. 516, A70 (2…
y 4F°7/226165.7907/2odd37.9 ns measured1.245297.6–Duquette & Lawler, Phys. Rev. A 26, 330 (1982), as compiled in R. L. Kurucz life4100.labKröger, Er, Öztürk, Başar, Jarmola, Ferber, Tamanis, Začs, Astron. Astrophys. 516, A70 (2…
y 6D°5/226386.3605/2odd38.9 ns measured1.61804.1–Duquette & Lawler, Phys. Rev. A 26, 330 (1982), as compiled in R. L. Kurucz life4100.labKröger, Er, Öztürk, Başar, Jarmola, Ferber, Tamanis, Začs, Astron. Astrophys. 516, A70 (2…
y 4F°9/226440.3309/2odd35.6 ns measured1.334337.4–Duquette & Lawler, Phys. Rev. A 26, 330 (1982), as compiled in R. L. Kurucz life4100.labKröger, Er, Öztürk, Başar, Jarmola, Ferber, Tamanis, Začs, Astron. Astrophys. 516, A70 (2…
x 6D°1/226552.4001/2odd8 ns measured2.441430.3–Duquette & Lawler, Phys. Rev. A 26, 330 (1982), as compiled in R. L. Kurucz life4100.labBaşar, Başar, Öztürk, Er, Güzelçimen, Kröger, Astron. Astrophys. 556, A103 (2013), as com…
x 6D°3/226713.3203/2odd7.3 ns measured1.45103.6–Duquette & Lawler, Phys. Rev. A 26, 330 (1982), as compiled in R. L. Kurucz life4100.labKröger, Er, Öztürk, Başar, Jarmola, Ferber, Tamanis, Začs, Astron. Astrophys. 516, A70 (2…
y 4D°1/226717.7301/2odd14.9 ns measured1.141506–Duquette & Lawler, Phys. Rev. A 26, 330 (1982), as compiled in R. L. Kurucz life4100.labKröger, Er, Öztürk, Başar, Jarmola, Ferber, Tamanis, Začs, Astron. Astrophys. 516, A70 (2…
y 6D°7/226832.4307/2odd25.8 ns measured1.248378.4–Duquette & Lawler, Phys. Rev. A 26, 330 (1982), as compiled in R. L. Kurucz life4100.labBouzed, Kröger, Zimmermann, Kronfeldt, Guthöhrlein, Eur. Phys. J. D 23, 57 (2003), as com…
z 2G°7/226896.6807/2odd56.2 ns measured1.013181.3-21Duquette & Lawler, Phys. Rev. A 26, 330 (1982), as compiled in R. L. Kurucz life4100.labBaşar, Başar, Öztürk, Er, Güzelçimen, Kröger, Astron. Astrophys. 556, A103 (2013), as com…
y 4D°3/226936.8603/2odd23 ns measured1.29239.9–Gao, Geng, Quinet, Wang, Yu, Dai, Astrophys. J. Suppl. 242, 23 (2019), Table 1Kröger, Er, Öztürk, Başar, Jarmola, Ferber, Tamanis, Začs, Astron. Astrophys. 516, A70 (2…
x 6D°5/226983.3405/2odd7 ns measured1.618196.4–Duquette & Lawler, Phys. Rev. A 26, 330 (1982), as compiled in R. L. Kurucz life4100.labKröger, Er, Öztürk, Başar, Jarmola, Ferber, Tamanis, Začs, Astron. Astrophys. 516, A70 (2…
z 2G°9/227331.8009/2odd56.7 ns measured1.078––Duquette & Lawler, Phys. Rev. A 26, 330 (1982), as compiled in R. L. Kurucz life4100.lab–
y 6D°9/227419.6209/2odd15.1 ns measured1.422405.747Duquette & Lawler, Phys. Rev. A 26, 330 (1982), as compiled in R. L. Kurucz life4100.labBaşar, Başar, Öztürk, Er, Güzelçimen, Kröger, Astron. Astrophys. 556, A103 (2013), as com…
x 6D°7/227427.0707/2odd7.5 ns measured1.567384.7–Gao, Geng, Quinet, Wang, Yu, Dai, Astrophys. J. Suppl. 242, 23 (2019), Table 1Kröger, Er, Öztürk, Başar, Jarmola, Ferber, Tamanis, Začs, Astron. Astrophys. 516, A70 (2…
y 4D°7/227596.7407/2odd29.1 ns measured1.422-144–Gao, Geng, Quinet, Wang, Yu, Dai, Astrophys. J. Suppl. 242, 23 (2019), Table 1Kröger, Er, Öztürk, Başar, Jarmola, Ferber, Tamanis, Začs, Astron. Astrophys. 516, A70 (2…
x 6D°9/227974.8709/2odd11.4 ns measured1.542525.1–Gao, Geng, Quinet, Wang, Yu, Dai, Astrophys. J. Suppl. 242, 23 (2019), Table 1Kröger, Er, Öztürk, Başar, Jarmola, Ferber, Tamanis, Začs, Astron. Astrophys. 516, A70 (2…
z 4I°15/233116.36015/2odd–1.19627.1––Kröger, Er, Öztürk, Başar, Jarmola, Ferber, Tamanis, Začs, Astron. Astrophys. 516, A70 (2…
4I°15/235731.34015/2odd18.7 ns measured1.24298.8–Mukund, Bhattacharyya, Yarlagadda, Nakhate, JQSRT 166, 68 (2015), as compiled in R. L. Ku…Kröger, Er, Öztürk, Başar, Jarmola, Ferber, Tamanis, Začs, Astron. Astrophys. 516, A70 (2…

Nb⁺ ionisation limit 54513.80 cm⁻¹ = 6.75885 eV (183.440 nm)

Sources

Transitions: classified Nb I lines with log gf of Duquette, Den Hartog & Lawler 1986 as transcribed by Kurucz (gf4100ddl.lab; lower/upper energies and J matched to the NIST levels file within 0.06 cm^-1); A_s is derived from log gf with A = 0.667025 sigma^2 gf / g_upper (sigma from NIST energies). Where the line is in Table 1 of Kröger et al. 2010 the measured hyperfine centre-of-gravity wavenumber is given as frequency_THz (isotope 93, the only stable one). Level lifetimes: Gao et al. 2019 (first-hand) preferred, older measurements under alternatives. Hyperfine: even levels from Table 2 of Kröger et al. 2010 (literature compilation with uncertainties) plus Kurucz ab410093.dat for levels missing there; odd levels from Table 3 of Kröger et al. 2010 (A only). The Kurucz hyperfine file has transcription errors (three found against Kröger 2010, listed under conflicts) and omits uncertainties, so its entries should be treated with care; entries flagged COMPUTED in that file (code KOAB) were skipped. Sign convention: A, B in MHz as printed. Lines without frequency_THz: 188.

Atoms with measured data

All elements: periodic table