Atomic energy level diagrams

Sulfur energy level diagram

Energy levels and transitions of neutral sulfur (S I): the 81 strongest classified lines below 2 µm from the NIST Atomic Spectra Database and the 47 levels they connect, each line with its vacuum wavelength, frequency and, for 74 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.

Sulfur energy level diagram with transition wavelengths and dipole matrix elements

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

Key transitions of sulfur

Transitionλ vac (nm)λ air (nm)ν (THz)|⟨J‖er‖J′⟩| (ea₀)A (s⁻¹)Γ/2π up. (MHz)branch (%)Use
3s23p4 3P2 – 3s23p34s 3P°2129.5653–2313.83211.3623.457e+0874.1674.2129.6 nm ground-state lines of the 1299 A multiplet used…
3s23p4 3P2 – 3s23p34s 3P°1129.6174–2312.90330.6851.456e+0878.2529.6129.6 nm ground-state lines of the 1299 A multiplet used…
3s23p4 3P2 – 3s23p34p 3P2154.1009–1945.429689(27)––3.452–Doppler-free two-photon excitation
3s23p4 3P2 – 3s23p34p 3P0154.1037–1945.393840(27)––3.452–Doppler-free two-photon excitation
3s23p4 3P2 – 3s23p34p 3P1154.1095–1945.321233(27)––3.452–Doppler-free two-photon excitation
3s23p4 3P1 – 3s23p34p 3P2155.0472–1933.55618(7)––3.452–Doppler-free two-photon excitation
3s23p4 3P1 – 3s23p34p 3P1155.0559–1933.447755(27)––3.452–Doppler-free two-photon excitation
3s23p4 3P0 – 3s23p34p 3P2155.4752–1928.233794(27)––3.452–Doppler-free two-photon excitation
3s23p4 3P0 – 3s23p34p 3P0155.4781–1928.197819(27)––3.452–Doppler-free two-photon excitation
3s23p4 3P2 – 3s23p34s 3S°1180.7312–1658.77491.6893.264e+0884.8861.2180.731 nm
3s23p34s 3S°1 – 3s23p34p 3P21045.83081045.5443286.65487.8722.195e+073.4521001045.5-1045.9 nm near-infrared triplet
3s23p34s 3S°1 – 3s23p34p 3P01045.96181045.6753286.61893.5212.195e+073.4521001045.5-1045.9 nm near-infrared triplet
3s23p34s 3S°1 – 3s23p34p 3P11046.22671045.9401286.54646.0992.194e+073.4521001045.5-1045.9 nm near-infrared triplet

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).

33S hyperfine structure (I = 3/2)

LevelA (MHz)B (MHz)Shift of each F level from the centre of gravity (MHz)
3s23p4 3P2130.090-31.600F=1/2: -613.05 F=3/2: -390.27 F=5/2: -45.30 F=7/2: +382.37
3s23p4 3P1-4.62015.800F=1/2: +31.30 F=3/2: -11.18 F=5/2: -2.98

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

Isotope shifts

Transitionλ vac (nm)IsotopesShift (MHz)
3s23p4 3P2 – 3s23p34p 3P2154.10134-32537(12)

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

Closed and nearly closed transitions of sulfur

Transitionλ vacuum (nm)Lower levelA (s⁻¹)Leak per scattered photonPhotons before a leakWhere the leak goes
3s23p4 3P1 → 3s23p34s 3P°0130.3110metastable4.830e+08 NIST5.65 × 10−4 from semi-empirical calc.1,7703s23p34p 3P1 ≈ 5.45 × 10−4; 3s23p35p 3P1 ≈ 1.93 × 10−5; 3s23p34p 5P1 ≈ 6.3 × 10−7; 2 weaker lines
3s23p4 1D2 → 3s23p34s 1D°2166.6687metastable4.580e+08 NIST0.406 % from semi-empirical calc.2463s23p4 3P2 0.388 % (long-lived); 3s23p4 3P1 ≈ 1.67 × 10−4 (long-lived); 3s23p34p 3P1 ≈ 5.66 × 10−6; 4 weaker lines
3s23p4 3P2 → 3s23p34s 3D°3147.3995ground1.960e+08 NIST0.454 % from theory2203s23p34p 5P2 0.227 %*; 3s23p34p 5P3 0.11 %*; 3s23p4 1D2 9.23 × 10−4* (long-lived); 1 weaker lines
3s23p4 3P2 → 3s23p33d 3D°3142.5031ground3.790e+08 NIST1.62 % from semi-empirical calc.623s23p34p 3P2 1.59 %; 3s23p4 1D2 ≈ 2.11 × 10−4 (long-lived); 3s23p34p 5P2 ≈ 1.24 × 10−5; 1 weaker lines
3s23p4 3P2 → 3s23p34d 3D°3131.6545ground7.890e+07 NIST4.02 % from semi-empirical calc.253s23p34p 3P2 2.76 %; 3s23p35p 3P2 1.41 %; 3s23p4 1D2 1.95 × 10−4 (long-lived); 4 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 S 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
3s23p4 3P23s23p312d 3D°3120.8850–2479.9806E10.163 NIST4.330e+06 NIST–NIST ASD (accuracy E)
3s23p4 3P23s23p38s 3S°1124.1905–2413.9726E10.186 NIST1.220e+07 NIST48.8NIST ASD (accuracy D+)
3s23p4 3P23s23p36d 3D°1124.7108–2403.9011E10.0536 semi-empirical1.000e+06 semi-empirical7.5Kurucz, R. L., Can. J. Phys. 89, 417 (2011); semi-empirical line list gf1600.pos of 2011-…
3s23p4 3P23s23p36d 3D°2124.7136–2403.8472E10.116 NIST2.820e+06 NIST21.1NIST ASD (accuracy D+)
3s23p4 3P23s23p36d 3D°3124.7160–2403.8013E10.302 NIST1.360e+07 NIST100NIST ASD (accuracy D+)
3s23p4 3P13s23p38s 3S°1124.8044–2402.0992E10.147 measured7.464e+06 measured29.9Biemont, Garnir, Federman, Li, Svanberg, Astrophys. J. 502, 1010 (1998), Table 2, column …
3s23p4 3P03s23p38s 3S°1125.0815–2396.7767E10.0878 NIST2.660e+06 NIST10.6NIST ASD (accuracy D)
3s23p4 3P13s23p36d 3D°1125.3298–2392.0276E10.124 NIST5.290e+06 NIST39.7NIST ASD (accuracy D+)
3s23p4 3P13s23p36d 3D°2125.3327–2391.9737E10.228 NIST1.070e+07 NIST80.2NIST ASD (accuracy D+)
3s23p4 3P03s23p36d 3D°1125.6093–2386.7051E10.153 NIST7.980e+06 NIST59.9NIST ASD (accuracy D+)
3s23p4 3P23s23p37s 3S°1126.2860–2373.9171E10.210 NIST1.480e+07 NIST52.7NIST ASD (accuracy D+)
3s23p4 3P13s23p37s 3S°1126.9208–2362.0436E10.157 NIST8.180e+06 NIST29.1NIST ASD (accuracy D+)
3s23p4 3P23s23p35d 3D°1127.0768–2359.1435E10.0481 NIST7.600e+05 NIST3.14NIST ASD (accuracy D)
3s23p4 3P23s23p35d 3D°3127.0780–2359.1221E10.424 NIST2.540e+07 NIST100NIST ASD (accuracy C)
3s23p4 3P23s23p35d 3D°2127.0786–2359.1097E10.184 NIST6.700e+06 NIST–NIST ASD (accuracy D+)
3s23p4 3P03s23p37s 3S°1127.2074–2356.7211E10.0894 NIST2.620e+06 NIST9.33NIST ASD (accuracy D)
3s23p4 3P13s23p35d 3D°1127.7196–2347.2700E10.180 NIST1.050e+07 NIST43.4NIST ASD (accuracy D+)
3s23p4 3P13s23p35d 3D°2127.7215–2347.2362E10.308 NIST1.840e+07 NIST–NIST ASD (accuracy D+)
3s23p4 3P03s23p35d 3D°1128.0099–2341.9475E10.205 NIST1.350e+07 NIST55.8NIST ASD (accuracy D+)
3s23p4 3P23s23p34s 3P°2129.5653–2313.8321E11.362 measured3.457e+08 measured74.2Beideck, Schectman, Federman, Ellis, Astrophys. J. 428, 393 (1994), beam-foil spectroscop…
3s23p4 3P23s23p34s 3P°1129.6174–2312.9033E10.685 measured1.456e+08 measured29.6Beideck, Schectman, Federman, Ellis, Astrophys. J. 428, 393 (1994), beam-foil spectroscop…
3s23p4 3P13s23p34s 3P°2130.2336–2301.9586E10.810 measured1.203e+08 measured25.8Beideck, Schectman, Federman, Ellis, Astrophys. J. 428, 393 (1994), beam-foil spectroscop…
3s23p4 3P13s23p34s 3P°1130.2862–2301.0298E10.709 measured1.533e+08 measured31.2Beideck, Schectman, Federman, Ellis, Astrophys. J. 428, 393 (1994), beam-foil spectroscop…
3s23p4 3P13s23p34s 3P°0130.3110–2300.5921E10.726 NIST4.830e+08 NIST100NIST ASD (accuracy C)
3s23p4 3P23s23p36s 3S°1130.3429–2300.0283E10.311 NIST2.950e+07 NIST52.2NIST ASD (accuracy D+)
3s23p4 3P03s23p34s 3P°1130.5883–2295.7073E10.803 measured1.956e+08 measured39.8Beideck, Schectman, Federman, Ellis, Astrophys. J. 428, 393 (1994), beam-foil spectroscop…
3s23p4 3P13s23p36s 3S°1131.0193–2288.1548E10.238 NIST1.700e+07 NIST30.1NIST ASD (accuracy D+)
3s23p4 3P03s23p36s 3S°1131.3248–2282.8323E10.136 NIST5.540e+06 NIST9.81NIST ASD (accuracy D+)
3s23p4 3P23s23p34d 3D°3131.6545–2277.1159E10.789 NIST7.890e+07 NIST100NIST ASD (accuracy C)
3s23p4 3P23s23p34d 3D°2131.6616–2276.9925E10.344 NIST2.100e+07 NIST26.2NIST ASD (accuracy C)
3s23p4 3P23s23p34d 3D°1131.6625–2276.9771E10.0895 NIST2.370e+06 NIST2.99NIST ASD (accuracy D)
3s23p4 3P13s23p34d 3D°2132.3517–2265.1190E10.588 NIST6.040e+07 NIST75.5NIST ASD (accuracy C)
3s23p4 3P13s23p34d 3D°1132.3526–2265.1036E10.342 NIST3.400e+07 NIST42.8NIST ASD (accuracy C)
3s23p4 3P03s23p34d 3D°1132.6644–2259.7811E10.392 NIST4.440e+07 NIST55.9NIST ASD (accuracy C)
3s23p4 3P23s3p5 3P°1138.1553–2169.9669E10.046 NIST5.420e+05 NIST–NIST ASD (accuracy D)
3s23p4 3P23s3p5 3P°2138.8436–2159.2093E10.0605 NIST5.540e+05 NIST–NIST ASD (accuracy D)
3s23p4 3P13s3p5 3P°2139.6113–2147.3359E10.0621 NIST5.750e+05 NIST–NIST ASD (accuracy D)
3s23p4 3P23s23p35s 3S°1140.1515–2139.0601E10.552 NIST7.480e+07 NIST53.1NIST ASD (accuracy C)
3s23p4 3P13s23p35s 3S°1140.9338–2127.1866E10.425 NIST4.350e+07 NIST30.9NIST ASD (accuracy C)
3s23p4 3P03s23p35s 3S°1141.2873–2121.8641E10.243 NIST1.420e+07 NIST10.1NIST ASD (accuracy D+)
3s23p4 3P23s23p33d 3D°3142.5031–2103.7616E11.947 NIST3.790e+08 NIST79.6NIST ASD (accuracy C+)
3s23p4 3P23s23p33d 3D°2142.5189–2103.5283E10.823 NIST9.480e+07 NIST19.9NIST ASD (accuracy C)
3s23p4 3P23s23p33d 3D°1142.5220–2103.4821E10.212 NIST1.050e+07 NIST2.21NIST ASD (accuracy D+)
3s23p4 3P13s23p33d 3D°2143.3279–2091.6549E11.429 NIST2.810e+08 NIST59NIST ASD (accuracy C+)
3s23p4 3P13s23p33d 3D°1143.3310–2091.6086E10.825 NIST1.560e+08 NIST32.8NIST ASD (accuracy C)
3s23p4 3P03s23p33d 3D°1143.6967–2086.2861E10.954 NIST2.070e+08 NIST43.5NIST ASD (accuracy C)
3s23p4 3P23s23p34s 1D°2144.4296–2075.6992E1 (intercombination)0.139 NIST2.590e+06 NIST0.389NIST ASD (accuracy D+)
3s23p4 1D23s23p34s 1P°1144.8230–2070.0616E11.500 NIST5.000e+08 NIST80.2NIST ASD (accuracy D+)
3s23p4 1D23s23p34s 3P°2147.1832–2036.8655E1 (intercombination)0.140 NIST2.490e+06 NIST0.534NIST ASD (accuracy D+)
3s23p4 3P23s23p33d 5D°3147.2971–2035.2909E1 (intercombination)0.642 NIST3.730e+07 NIST100NIST ASD (accuracy D+)
3s23p4 3P23s23p34s 3D°3147.3995–2033.8773E11.473 NIST1.960e+08 NIST100NIST ASD (accuracy C+)
3s23p4 3P23s23p34s 3D°2147.4379–2033.3473E10.621 NIST4.880e+07 NIST34.3NIST ASD (accuracy C)
3s23p4 3P23s23p34s 3D°1147.4571–2033.0822E10.160 NIST5.390e+06 NIST3.67NIST ASD (accuracy D+)
3s23p4 3P13s23p33d 5D°2148.1663–2023.3510E1 (intercombination)0.236 NIST6.950e+06 NIST54.7NIST ASD (accuracy E)
3s23p4 3P13s23p34s 3D°2148.3039–2021.4739E11.077 NIST1.440e+08 NIST100NIST ASD (accuracy C+)
3s23p4 3P13s23p34s 3D°1148.3234–2021.2087E10.621 NIST7.990e+07 NIST54.3NIST ASD (accuracy C)
3s23p4 3P03s23p33d 5D°1148.5621–2017.9604E1 (intercombination)0.106 NIST2.320e+06 NIST35.7NIST ASD (accuracy D+)
3s23p4 3P03s23p34s 3D°1148.7150–2015.8862E10.719 NIST1.060e+08 NIST72.1NIST ASD (accuracy C)
3s23p4 3P23s23p34p 3P2154.1009–1945.4297two-photon––––
3s23p4 3P23s23p34p 3P0154.1037–1945.3938two-photon––––
3s23p4 3P23s23p34p 3P1154.1095–1945.3212two-photon––––
3s23p4 3P13s23p34p 3P2155.0472–1933.5562two-photon––––
3s23p4 3P13s23p34p 3P1155.0559–1933.4478two-photon––––
3s23p4 3P03s23p34p 3P2155.4752–1928.2338two-photon––––
3s23p4 3P03s23p34p 3P0155.4781–1928.1978two-photon––––
3s23p4 1D23s23p33d 3D°2164.1294–1826.5618E1 (intercombination)0.0885 NIST7.180e+05 NIST0.151NIST ASD (accuracy D+)
3s23p4 1D23s23p34s 1D°2166.6687–1798.7326E12.288 NIST4.580e+08 NIST68.7NIST ASD (accuracy C+)
3s23p4 1S03s23p33d 1P°1168.7530–1776.5165E10.701 NIST6.900e+07 NIST100NIST ASD (accuracy D)
3s23p4 1S03s23p34s 1P°1178.2262–1682.0898E10.986 NIST1.160e+08 NIST18.6NIST ASD (accuracy D)
3s23p4 3P23s23p34s 3S°1180.7312–1658.7749E11.689 measured3.264e+08 measured61.2Beideck, Schectman, Federman, Ellis, Astrophys. J. 428, 393 (1994), beam-foil spectroscop…
3s23p4 3P13s23p34s 3S°1182.0342–1646.9014E11.233 measured1.701e+08 measured31.9Beideck, Schectman, Federman, Ellis, Astrophys. J. 428, 393 (1994), beam-foil spectroscop…
3s23p4 3P03s23p34s 3S°1182.6245–1641.5789E10.713 NIST5.640e+07 NIST6.9NIST ASD (accuracy C)
3s23p34s 5S°23s23p35p 5P3469.5422469.4108638.4782E10.547 NIST8.370e+05 NIST51.5NIST ASD (accuracy D)
3s23p34s 5S°23s23p35p 5P2469.6753469.5439638.2973E10.456 NIST8.140e+05 NIST12.9NIST ASD (accuracy D)
3s23p34s 5S°23s23p35p 5P1469.7563469.6249638.1872E10.351 NIST8.010e+05 NIST12.8NIST ASD (accuracy D)
3s23p34s 5S°23s23p34p 5P3921.5382921.2854325.3175E18.685 NIST2.790e+07 NIST100NIST ASD (accuracy C)
3s23p34s 5S°23s23p34p 5P2923.0617922.8085324.7805E17.332 NIST2.770e+07 NIST100NIST ASD (accuracy C)
3s23p34s 5S°23s23p34p 5P1924.0066923.7531324.4484E15.688 NIST2.770e+07 NIST100NIST ASD (accuracy C)
3s23p34s 3S°13s23p34p 3P21045.83081045.5443286.6548E17.872 measured2.195e+07 measured100Zerne, Luo Caiyan, Berzinsh, Svanberg, Phys. Scr. 56, 459 (1997), two-photon UV excitatio…
3s23p34s 3S°13s23p34p 3P01045.96181045.6753286.6189E13.521 measured2.195e+07 measured100Zerne, Luo Caiyan, Berzinsh, Svanberg, Phys. Scr. 56, 459 (1997), two-photon UV excitatio…
3s23p34s 3S°13s23p34p 3P11046.22671045.9401286.5464E16.099 measured2.194e+07 measured100Zerne, Luo Caiyan, Berzinsh, Svanberg, Phys. Scr. 56, 459 (1997), two-photon UV excitatio…

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.

S energy levels

LevelEnergy (cm⁻¹)JParityLifetimegJHyperfine A (MHz)Hyperfine B (MHz)Lifetime sourceHyperfine source
3s23p4 3P20.0002evenstable1.5005130.09-31.6–Carette & Godefroid, J. Phys. B 44, 105001 (2011), arXiv:1101.5645, MCHF/CI with relativi…
3s23p4 3P1396.0561even–1.501-4.6215.8–Carette & Godefroid, J. Phys. B 44, 105001 (2011), arXiv:1101.5645, MCHF/CI with relativi…
3s23p4 3P0573.5960even––––––
3s23p4 1D29238.6092even36.47 s theory–––NIST ASD S I lines table (tp_ref T8595,T7942c84), local cache data/nist/S_I_lines_from1nm…–
3s23p4 1S022179.9540even594.2 ms theory–––NIST ASD S I lines table (tp_ref T8595,T7942c84), local cache data/nist/S_I_lines_from1nm…–
3s23p34s 5S°252623.6052odd17.61 µs theory–––Zatsarinny & Bartschat, J. Phys. B 39, 2861 (2006), B-spline R-matrix calculation; level-…–
3s23p34s 3S°155330.7751odd1.875 ns measured–––Beideck, Schectman, Federman, Ellis, Astrophys. J. 428, 393 (1994), beam-foil spectroscop…–
3s23p34p 5P163446.0381even36.92 ns theory–––Zatsarinny & Bartschat, J. Phys. B 39, 2861 (2006), B-spline R-matrix calculation; level-…–
3s23p34p 5P263457.1172even36.83 ns theory–––Zatsarinny & Bartschat, J. Phys. B 39, 2861 (2006), B-spline R-matrix calculation; level-…–
3s23p34p 5P363475.0273even36.68 ns theory–––Zatsarinny & Bartschat, J. Phys. B 39, 2861 (2006), B-spline R-matrix calculation; level-…–
3s23p34p 3P164888.9331even46.1 ns measured–––Zerne, Luo Caiyan, Berzinsh, Svanberg, Phys. Scr. 56, 459 (1997), two-photon UV excitatio…–
3s23p34p 3P064891.3540even46.1 ns measured–––Zerne, Luo Caiyan, Berzinsh, Svanberg, Phys. Scr. 56, 459 (1997), two-photon UV excitatio…–
3s23p34p 3P264892.5512even46.1 ns measured–––Zerne, Luo Caiyan, Berzinsh, Svanberg, Phys. Scr. 56, 459 (1997), two-photon UV excitatio…–
3s23p34s 3D°167816.3211odd6.801 ns theory–––Zatsarinny & Bartschat, J. Phys. B 39, 2861 (2006), B-spline R-matrix calculation; level-…–
3s23p34s 3D°267825.1662odd7.024 ns theory–––Zatsarinny & Bartschat, J. Phys. B 39, 2861 (2006), B-spline R-matrix calculation; level-…–
3s23p34s 3D°367842.8463odd7.503 ns theory–––Zatsarinny & Bartschat, J. Phys. B 39, 2861 (2006), B-spline R-matrix calculation; level-…–
3s23p33d 5D°167885.5081odd153.8 ns theory–––Zatsarinny & Bartschat, J. Phys. B 39, 2861 (2006), B-spline R-matrix calculation; level-…–
3s23p33d 5D°267887.7822odd78.65 ns theory–––Zatsarinny & Bartschat, J. Phys. B 39, 2861 (2006), B-spline R-matrix calculation; level-…–
3s23p33d 5D°367889.9983odd41.51 ns theory–––Zatsarinny & Bartschat, J. Phys. B 39, 2861 (2006), B-spline R-matrix calculation; level-…–
3s23p34s 1D°269237.8722odd1.5 ns measured–––Savage & Lawrence, Astrophys. J. 146, 940 (1966), phase-shift method, Table 1 (3p4 1D - 4…–
3s23p33d 3D°170164.6101odd2.1 ns measured–––Savage & Lawrence, Astrophys. J. 146, 940 (1966), phase-shift method, Table 1; lifetime o…–
3s23p33d 3D°270166.1532odd2.1 ns measured–––Savage & Lawrence, Astrophys. J. 146, 940 (1966), phase-shift method, Table 1; lifetime o…–
3s23p33d 3D°370173.9333odd2.1 ns measured–––Savage & Lawrence, Astrophys. J. 146, 940 (1966), phase-shift method, Table 1; lifetime o…–
3s23p35s 3S°171351.3641odd7.1 ns measured–––Berzinsh, Luo Caiyan, Zerne, Svanberg, Biemont, Phys. Rev. A 55, 1836 (1997), time-resolv…–
3s3p5 3P°272023.4712odd––––––
3s3p5 3P°172382.3051odd––––––
3s23p35p 5P173911.2381even159.3 ns theory–––Zatsarinny & Bartschat, J. Phys. B 39, 2861 (2006), B-spline R-matrix calculation; level-…–
3s23p35p 5P273914.9102even158.9 ns theory–––Zatsarinny & Bartschat, J. Phys. B 39, 2861 (2006), B-spline R-matrix calculation; level-…–
3s23p35p 5P373920.9453even615 ns measured–––Delalic, Erman, Kallne, Phys. Scr. 42, 540 (1990), high-frequency deflection technique; v…–
3s23p34d 3D°175951.7801odd12.6 ns measured–––Berzinsh, Luo Caiyan, Zerne, Svanberg, Biemont, Phys. Rev. A 55, 1836 (1997), time-resolv…–
3s23p34d 3D°275952.2932odd12.5 ns measured–––Berzinsh, Luo Caiyan, Zerne, Svanberg, Biemont, Phys. Rev. A 55, 1836 (1997), time-resolv…–
3s23p34d 3D°375956.4113odd12.9 ns measured–––Berzinsh, Luo Caiyan, Zerne, Svanberg, Biemont, Phys. Rev. A 55, 1836 (1997), time-resolv…–
3s23p36s 3S°176720.6851odd17.7 ns measured–––Berzinsh, Luo Caiyan, Zerne, Svanberg, Biemont, Phys. Rev. A 55, 1836 (1997), time-resolv…–
3s23p34s 3P°077135.5500odd3 ns theory–––relativistic Hartree-Fock, Biemont, Garnir, Federman, Li, Svanberg, Astrophys. J. 502, 10…–
3s23p34s 3P°177150.1501odd2.034 ns measured–––Beideck, Schectman, Federman, Ellis, Astrophys. J. 428, 393 (1994), beam-foil spectroscop…–
3s23p34s 3P°277181.1302odd2.146 ns measured–––Beideck, Schectman, Federman, Ellis, Astrophys. J. 428, 393 (1994), beam-foil spectroscop…–
3s23p34s 1P°178288.4301odd1.605 ns theory–––Zatsarinny & Bartschat, J. Phys. B 39, 2861 (2006), B-spline R-matrix calculation; level-…–
3s23p35d 3D°278691.4302odd––––––
3s23p35d 3D°378691.8433odd40 ns measured–––Berzinsh, Luo Caiyan, Zerne, Svanberg, Biemont, Phys. Rev. A 55, 1836 (1997), time-resolv…–
3s23p35d 3D°178692.5571odd41.3 ns measured–––Berzinsh, Luo Caiyan, Zerne, Svanberg, Biemont, Phys. Rev. A 55, 1836 (1997), time-resolv…–
3s23p37s 3S°179185.3501odd35.6 ns measured–––Berzinsh, Luo Caiyan, Zerne, Svanberg, Biemont, Phys. Rev. A 55, 1836 (1997), time-resolv…–
3s23p36d 3D°380182.1803odd75 ns measured–––Biemont, Garnir, Federman, Li, Svanberg, Astrophys. J. 502, 1010 (1998), Table 1 (entries…–
3s23p36d 3D°280183.7102odd75 ns measured–––Biemont, Garnir, Federman, Li, Svanberg, Astrophys. J. 502, 1010 (1998), Table 1 (entries…–
3s23p36d 3D°180185.5101odd75 ns measured–––Biemont, Garnir, Federman, Li, Svanberg, Astrophys. J. 502, 1010 (1998), Table 1 (entries…–
3s23p38s 3S°180521.4601odd40 ns measured–––Biemont, Garnir, Federman, Li, Svanberg, Astrophys. J. 502, 1010 (1998), Table 1 (entries…–
3s23p33d 1P°181438.1671odd17 ns measured–––Savage & Lawrence, Astrophys. J. 146, 940 (1966), phase-shift method, Table 1: line 1687.…–
3s23p312d 3D°382723.2503odd––––––

S⁺ ionisation limit 83559.17 cm⁻¹ = 10.36002 eV (119.676 nm)

Sources

Level energies are the NIST ASD values (data/nist/S_I_levels.tsv). Uncertainties copied from Biemont et al. 1998 Table 1 are 2 sigma ('b represents a 2 sigma uncertainty'); Beideck et al. 1994 uncertainties are 1 sigma as printed in the original (Biemont et al. list them doubled). Lifetimes attributed to Berzinsh et al. 1997, Delalic et al. 1990, Bridges & Wiese, Smith 1978, Mueller 1968, Federman & Cardelli 1995 are second-hand (method 'compilation'). The Federman & Cardelli 'lifetimes' are inferred from interstellar absorption f-values, not laboratory lifetimes. Savage & Lawrence values are multiplet lifetimes attached to each fine-structure level. A-values of the 3P - ns 3S°, nd 3D° lines from Biemont et al. are semi-empirical (measured lifetime x calculated branching ratio); they are close to what NIST ASD already lists. 'f_abs' (absorption oscillator strength) is a non-schema field; type 'two-photon' is used for the Doppler-free two-photon lines (frequency = total energy of both photons). 32S and 34S have I = 0; 33S has I = 3/2. Lifetimes of 1D2 and 1S0 are derived from calculated A-values (theory).

Atoms with measured data

All elements: periodic table