Atomic energy level diagrams

Antimony energy level diagram

Energy levels and transitions of neutral antimony (Sb I): the 82 strongest classified lines below 2 µm from the NIST Atomic Spectra Database and the 42 levels they connect, each line with its vacuum wavelength, frequency and, for 76 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.

Antimony energy level diagram with transition wavelengths and dipole matrix elements

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

Key transitions of antimony

Transitionλ vac (nm)λ air (nm)ν (THz)|⟨J‖er‖J′⟩| (ea₀)A (s⁻¹)Γ/2π up. (MHz)branch (%)Use
5p3 4S°3/2 – 5p26s 4P5/2206.9004206.83441448.96962.1791.810e+0834.690.4laser pumping line
5p3 4S°3/2 – 5p26s 4P3/2217.6499217.58181377.40661.8871.750e+0830.0388.9ground-state line used for collinear laser spectroscopy o…
5p3 4S°3/2 – 5p26s 4P1/2231.2174231.14631296.58251.4361.690e+0830.0382.5laser pumping 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).

121Sb hyperfine structure (I = 5/2)

LevelA (MHz)B (MHz)Shift of each F level from the centre of gravity (MHz)
5p3 4S°3/2-299.034(4)-3.680(20)F=1: +1567.35 F=2: +972.23 F=3: +76.78 F=4: -1122.30
5p3 2D°3/2565(7)-561(6)F=1: -3358.95 F=2: -1780.15 F=3: +167.30 F=4: +1978.50
5p3 2D°5/21468.980–F=0: -12853.58 F=1: -11384.59 F=2: -8446.64 F=3: -4039.70 F=4: +1836.22 F=5: +9181.12
5p3 2P°1/24907.600–F=2: -8588.30 F=3: +6134.50
5p3 2P°3/2680.0(10)438(30)F=1: -3263.40 F=2: -2253.80 F=3: -410.90 F=4: +2659.50
5p26s 4P3/2523.8(5)-471.0(20)F=1: -3079.65 F=2: -1655.25 F=3: +128.10 F=4: +1846.50

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

Closed and nearly closed transitions of antimony

Transitionλ vacuum (nm)Lower levelA (s⁻¹)Leak per scattered photonPhotons before a leakWhere the leak goes
5p3 2D°5/2 → 5p25d 2F7/2195.0393metastable2.600e+08 theory0.3 % from theory3335p26p (2,1/2)°5/2 ≈ 0.502 %; 5p26p (1,3/2)°5/2 ≈ 0.184 %; 5p26p (2,3/2)°5/2 ≈ 0.17 %; 1 weaker lines; the listed lines add up to ≈ 0.885 %
5p3 2D°5/2 → 5p25d 4F7/2214.2515metastable1.630e+07 theory0.6 % from theory1675p26p (1,3/2)°5/2 ≈ 0.5 %
5p3 2D°3/2 → 5p25d 2F5/2205.0234metastable9.930e+07 theory1.9 % from theory535p26p (0,3/2)°3/2 ≈ 1.36 %; 5p3 4S°3/2 1.07 %* (long-lived); 5p26p (1,3/2)°3/2 ≈ 9.76 × 10−4
5p3 2D°5/2 → 5p26s 2D5/2217.9872metastable2.390e+08 NIST7.3 % from theory145p3 4S°3/2 ≈ 7.93 % (long-lived); 5p3 2D°3/2 6.68 %* (long-lived); 5p3 2P°3/2 ≈ 6.27 % (long-lived); 2 weaker lines; the listed lines add up to ≈ 20.9 %
5p3 4S°3/2 → 5p25d 4P5/2187.1154ground1.500e+08 theory8.4 % from theory125p3 2D°3/2 5.9 %* (long-lived); 5p3 2D°5/2 1.42 %* (long-lived); 5p26p (0,3/2)°3/2 ≈ 1.86 × 10−4
5p3 4S°3/2 → 5p26s 4P5/2206.9004ground1.810e+08 NIST9.6 % from theory105p3 2D°5/2 9.29 %* (long-lived)

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 Sb 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
5p3 4S°3/25p25d 2D5/2153.2726–1955.9434E1 (intercombination)––––
5p3 4S°3/25p26d 4F5/2159.9956–1873.7547E10.667 HFR fit (this site)3.666e+07 HFR fit (this site)–This site: Cowan-code HFR calculation of Sb I with the parameters fitted to the NIST ener…
5p3 2D°3/25p28s 4P5/2166.2821–1802.9151E1 (intercombination)0.470 HFR fit (this site)1.621e+07 HFR fit (this site)–This site: Cowan-code HFR calculation of Sb I with the parameters fitted to the NIST ener…
5p3 2D°5/25p26d 2F7/2171.7455–1745.5619E11.905 HFR fit (this site)1.814e+08 HFR fit (this site)–This site: Cowan-code HFR calculation of Sb I with the parameters fitted to the NIST ener…
5p3 4S°3/25p25d 4D1/2173.6195–1726.7207E11.179 HFR fit (this site)2.690e+08 HFR fit (this site)100This site: Cowan-code HFR calculation of Sb I with the parameters fitted to the NIST ener…
5p3 4S°3/25p25d 2F5/2174.5595–1717.4226E1 (intercombination)0.130 theory1.080e+06 theory1.07Hartman, Nilsson, Engström, Lundberg, Palmeri, Quinet, Biémont, Phys. Rev. A 82, 052512 (…
5p3 4S°3/25p25d 2P3/2176.2638–1700.8174E1 (intercombination)0.446 theory1.840e+07 theory15.7Hartman, Nilsson, Engström, Lundberg, Palmeri, Quinet, Biémont, Phys. Rev. A 82, 052512 (…
5p3 4S°3/25p25d 4P3/2178.0887–1683.3887E10.701 theory4.400e+07 theory23.4Hartman, Nilsson, Engström, Lundberg, Palmeri, Quinet, Biémont, Phys. Rev. A 82, 052512 (…
5p3 2D°3/2(64432)3/2178.8260–1676.4475E1––––
5p3 2D°5/25p25d 2F7/2180.0187–1665.3405E13.626 HFR fit (this site)5.707e+08 HFR fit (this site)–This site: Cowan-code HFR calculation of Sb I with the parameters fitted to the NIST ener…
5p3 4S°3/25p26s 2D3/2181.0513–1655.8426E1 (intercombination)0.714 theory4.350e+07 theory35.7Hartman, Nilsson, Engström, Lundberg, Palmeri, Quinet, Biémont, Phys. Rev. A 82, 052512 (…
5p3 4S°3/25p25d 4F5/2181.4192–1652.4843E10.850 theory4.090e+07 theory39.2Hartman, Nilsson, Engström, Lundberg, Palmeri, Quinet, Biémont, Phys. Rev. A 82, 052512 (…
5p3 2D°5/25p26d 2F5/2182.9502–1638.6562E10.773 HFR fit (this site)3.296e+07 HFR fit (this site)–This site: Cowan-code HFR calculation of Sb I with the parameters fitted to the NIST ener…
5p3 2D°5/25p27s 2P3/2185.8893–1612.7468E10.908 HFR fit (this site)6.504e+07 HFR fit (this site)–This site: Cowan-code HFR calculation of Sb I with the parameters fitted to the NIST ener…
5p3 4S°3/25p25d 4F3/2186.8183–1604.7278E10.341 theory9.040e+06 theory21.1Hartman, Nilsson, Engström, Lundberg, Palmeri, Quinet, Biémont, Phys. Rev. A 82, 052512 (…
5p3 4S°3/25p25d 4P5/2187.1154–1602.1798E11.706 theory1.500e+08 theory91.6Hartman, Nilsson, Engström, Lundberg, Palmeri, Quinet, Biémont, Phys. Rev. A 82, 052512 (…
5p3 2D°3/25p25d 2D5/2188.2568–1592.4658E11.612 HFR fit (this site)1.315e+08 HFR fit (this site)–This site: Cowan-code HFR calculation of Sb I with the parameters fitted to the NIST ener…
5p3 2D°3/25p27s 2P1/2189.1275–1585.1342E10.705 HFR fit (this site)7.435e+07 HFR fit (this site)–This site: Cowan-code HFR calculation of Sb I with the parameters fitted to the NIST ener…
5p3 2D°5/25p26d 4F5/2189.9418–1578.3386E1 (intercombination)0.498 HFR fit (this site)1.220e+07 HFR fit (this site)–This site: Cowan-code HFR calculation of Sb I with the parameters fitted to the NIST ener…
5p3 2D°3/2(60404)5/2192.7066–1555.6935E1––––
5p3 2D°5/25p25d 2F7/2195.0393–1537.0876E12.760 theory2.600e+08 theory99.7Hartman, Nilsson, Engström, Lundberg, Palmeri, Quinet, Biémont, Phys. Rev. A 82, 052512 (…
5p3 4S°3/25p26s 2P3/2202.4655202.40031480.7089E1 (intercombination)0.132 theory1.060e+06 theory0.413Hartman, Nilsson, Engström, Lundberg, Palmeri, Quinet, Biémont, Phys. Rev. A 82, 052512 (…
5p3 2D°5/25p25d 4D5/2204.0447203.97921469.2490E1 (intercombination)0.767 HFR fit (this site)2.339e+07 HFR fit (this site)24.3This site: Cowan-code HFR calculation of Sb I with the parameters fitted to the NIST ener…
5p3 2D°3/25p25d 2F5/2205.0234204.95771462.2355E11.592 theory9.930e+07 theory98.1Hartman, Nilsson, Engström, Lundberg, Palmeri, Quinet, Biémont, Phys. Rev. A 82, 052512 (…
5p3 4S°3/25p26s 4P5/2206.9004206.83441448.9696E12.179 NIST1.810e+08 NIST90.4NIST ASD (accuracy n/a)
5p3 2D°3/25p25d 2P3/2207.3784207.31231445.6303E10.185 theory1.940e+06 theory1.65Hartman, Nilsson, Engström, Lundberg, Palmeri, Quinet, Biémont, Phys. Rev. A 82, 052512 (…
5p3 2D°3/25p25d 4P3/2209.9091209.84251428.2016E1 (intercombination)1.424 theory1.110e+08 theory59Hartman, Nilsson, Engström, Lundberg, Palmeri, Quinet, Biémont, Phys. Rev. A 82, 052512 (…
5p3 2D°3/25p26s 2D5/2211.7920211.72501415.5042E10.583 theory1.210e+07 theory6.68Hartman, Nilsson, Engström, Lundberg, Palmeri, Quinet, Biémont, Phys. Rev. A 82, 052512 (…
5p3 4S°3/25p26s 2P1/2212.8064212.73931408.7565E1 (intercombination)0.191 theory3.820e+06 theory1.21Hartman, Nilsson, Engström, Lundberg, Palmeri, Quinet, Biémont, Phys. Rev. A 82, 052512 (…
5p3 2D°3/25p26s 2D3/2214.0373213.96981400.6555E11.835 NIST1.740e+08 NIST58.2NIST ASD (accuracy n/a)
5p3 2D°5/25p25d 4F7/2214.2515214.18401399.2547E1 (intercombination)0.796 theory1.630e+07 theory99.4Hartman, Nilsson, Engström, Lundberg, Palmeri, Quinet, Biémont, Phys. Rev. A 82, 052512 (…
5p3 2D°3/25p25d 4F5/2214.5517214.48411397.2972E1 (intercombination)0.940 theory3.020e+07 theory29Hartman, Nilsson, Engström, Lundberg, Palmeri, Quinet, Biémont, Phys. Rev. A 82, 052512 (…
5p3 2D°5/25p25d 4P3/2215.9931215.92521387.9726E1 (intercombination)0.318 theory5.080e+06 theory2.7Hartman, Nilsson, Engström, Lundberg, Palmeri, Quinet, Biémont, Phys. Rev. A 82, 052512 (…
5p3 4S°3/25p26s 4P3/2217.6499217.58181377.4066E11.887 NIST1.750e+08 NIST88.9NIST ASD (accuracy n/a)
5p3 2D°5/25p26s 2D5/2217.9872217.91901375.2753E12.708 NIST2.390e+08 NIST92.7NIST ASD (accuracy n/a)
5p3 2P°1/25p25d 2D3/2220.1996220.13091361.4577E11.776 HFR fit (this site)1.497e+08 HFR fit (this site)–This site: Cowan-code HFR calculation of Sb I with the parameters fitted to the NIST ener…
5p3 2D°5/25p25d 4F5/2220.9118220.84301357.0683E1 (intercombination)0.850 HFR fit (this site)2.262e+07 HFR fit (this site)17.6This site: Cowan-code HFR calculation of Sb I with the parameters fitted to the NIST ener…
5p3 2D°3/25p25d 4F3/2222.1441222.07491349.5407E1 (intercombination)0.434 theory8.720e+06 theory20.4Hartman, Nilsson, Engström, Lundberg, Palmeri, Quinet, Biémont, Phys. Rev. A 82, 052512 (…
5p3 2P°1/25p27s 2P1/2222.2659222.19681348.8007E10.825 HFR fit (this site)6.279e+07 HFR fit (this site)–This site: Cowan-code HFR calculation of Sb I with the parameters fitted to the NIST ener…
5p3 2D°3/25p25d 4P5/2222.5643222.49511346.9928E1 (intercombination)0.561 theory9.640e+06 theory5.9Hartman, Nilsson, Engström, Lundberg, Palmeri, Quinet, Biémont, Phys. Rev. A 82, 052512 (…
5p3 2P°1/25p26d 2D3/2226.3184226.24841324.6492E11.250 HFR fit (this site)6.827e+07 HFR fit (this site)–This site: Cowan-code HFR calculation of Sb I with the parameters fitted to the NIST ener…
5p3 2D°5/25p25d 4F3/2228.9695228.89891309.3117E1 (intercombination)0.416 theory7.310e+06 theory17.1Hartman, Nilsson, Engström, Lundberg, Palmeri, Quinet, Biémont, Phys. Rev. A 82, 052512 (…
5p3 2D°5/25p25d 4P5/2229.4159229.34531306.7638E1 (intercombination)0.289 theory2.330e+06 theory1.42Hartman, Nilsson, Engström, Lundberg, Palmeri, Quinet, Biémont, Phys. Rev. A 82, 052512 (…
5p3 2P°3/25p25d 2D3/2230.7098230.63881299.4353E11.610 HFR fit (this site)1.069e+08 HFR fit (this site)–This site: Cowan-code HFR calculation of Sb I with the parameters fitted to the NIST ener…
5p3 2P°1/25p25d 2P1/2230.7217230.65071299.3684E11.288 HFR fit (this site)1.369e+08 HFR fit (this site)–This site: Cowan-code HFR calculation of Sb I with the parameters fitted to the NIST ener…
5p3 4S°3/25p26s 4P1/2231.2174231.14631296.5825E11.436 NIST1.690e+08 NIST82.5NIST ASD (accuracy n/a)
5p3 2P°3/25p25d 2D5/2231.6592231.58801294.1100E11.492 HFR fit (this site)6.047e+07 HFR fit (this site)–This site: Cowan-code HFR calculation of Sb I with the parameters fitted to the NIST ener…
5p3 2P°3/25p26d 2D3/2237.4355237.36311262.6268E1––––
5p3 2P°3/2(60404)5/2238.4343238.36161257.3377E13.501 HFR fit (this site)3.053e+08 HFR fit (this site)–This site: Cowan-code HFR calculation of Sb I with the parameters fitted to the NIST ener…
5p3 2P°1/25p27s 4P1/2239.5939239.52091251.2527E1 (intercombination)0.294 HFR fit (this site)6.383e+06 HFR fit (this site)–This site: Cowan-code HFR calculation of Sb I with the parameters fitted to the NIST ener…
5p3 2P°3/25p25d 2P1/2242.2867242.21311237.3461E10.772 HFR fit (this site)4.250e+07 HFR fit (this site)–This site: Cowan-code HFR calculation of Sb I with the parameters fitted to the NIST ener…
5p3 2P°1/25p25d 4D1/2242.7076242.63391235.2002E1 (intercombination)0.534 HFR fit (this site)2.023e+07 HFR fit (this site)23.7This site: Cowan-code HFR calculation of Sb I with the parameters fitted to the NIST ener…
5p3 2D°3/25p26s 2P3/2244.6243244.55021225.5218E10.473 theory7.750e+06 theory3.03Hartman, Nilsson, Engström, Lundberg, Palmeri, Quinet, Biémont, Phys. Rev. A 82, 052512 (…
5p3 2P°1/25p25d 2P3/2247.9064247.83151209.2969E10.862 theory2.470e+07 theory21Hartman, Nilsson, Engström, Lundberg, Palmeri, Quinet, Biémont, Phys. Rev. A 82, 052512 (…
5p3 2P°1/25p25d 4P1/2248.1190248.04401208.2610E1 (intercombination)0.325 HFR fit (this site)6.985e+06 HFR fit (this site)7.2This site: Cowan-code HFR calculation of Sb I with the parameters fitted to the NIST ener…
5p3 2D°3/25p26s 4P5/2251.1282251.05261193.7825E1 (intercombination)––––
5p3 2P°1/25p25d 4P3/2251.5316251.45591191.8682E1 (intercombination)0.387 theory4.760e+06 theory2.53Hartman, Nilsson, Engström, Lundberg, Palmeri, Quinet, Biémont, Phys. Rev. A 82, 052512 (…
5p3 2D°5/25p26s 2P3/2252.9269252.85091185.2929E12.378 NIST1.770e+08 NIST85.5NIST ASD (accuracy n/a)
5p3 2P°1/25p26s 2D3/2257.4824257.40531164.3221E10.470 theory6.550e+06 theory5.36Hartman, Nilsson, Engström, Lundberg, Palmeri, Quinet, Biémont, Phys. Rev. A 82, 052512 (…
5p3 2D°3/25p26s 2P1/2259.8825259.80481153.5694E10.603 NIST2.100e+07 NIST89.7NIST ASD (accuracy n/a)
5p3 2D°5/25p26s 4P5/2259.8860259.80841153.5536E1 (intercombination)1.027 theory2.030e+07 theory9.29Hartman, Nilsson, Engström, Lundberg, Palmeri, Quinet, Biémont, Phys. Rev. A 82, 052512 (…
5p3 2P°3/25p25d 2P3/2261.3084261.23041147.2746E11.580 theory7.090e+07 theory60.4Hartman, Nilsson, Engström, Lundberg, Palmeri, Quinet, Biémont, Phys. Rev. A 82, 052512 (…
5p3 2P°3/25p25d 4P3/2265.3393265.26031129.8458E1 (intercombination)0.927 theory2.330e+07 theory12.4Hartman, Nilsson, Engström, Lundberg, Palmeri, Quinet, Biémont, Phys. Rev. A 82, 052512 (…
5p3 2D°3/25p26s 4P3/2267.1424267.06301122.2196E1 (intercombination)0.496 theory6.550e+06 theory3.67Hartman, Nilsson, Engström, Lundberg, Palmeri, Quinet, Biémont, Phys. Rev. A 82, 052512 (…
5p3 2P°3/25p26s 2D5/2268.3551268.27541117.1485E10.972 HFR fit (this site)1.651e+07 HFR fit (this site)6.27This site: Cowan-code HFR calculation of Sb I with the parameters fitted to the NIST ener…
5p3 2P°1/25p25d 4F3/2269.3052269.22521113.2072E1 (intercombination)0.415 theory4.460e+06 theory10.4Hartman, Nilsson, Engström, Lundberg, Palmeri, Quinet, Biémont, Phys. Rev. A 82, 052512 (…
5p3 2P°3/25p26s 2D3/2271.9700271.88941102.2997E11.586 HFR fit (this site)6.335e+07 HFR fit (this site)23.4This site: Cowan-code HFR calculation of Sb I with the parameters fitted to the NIST ener…
5p3 2P°3/25p25d 4F5/2272.8011272.72041098.9415E1 (intercombination)0.908 theory1.370e+07 theory13.1Hartman, Nilsson, Engström, Lundberg, Palmeri, Quinet, Biémont, Phys. Rev. A 82, 052512 (…
5p3 2D°5/25p26s 4P3/2277.0749276.99311081.9906E1 (intercombination)0.707 theory1.190e+07 theory6.66Hartman, Nilsson, Engström, Lundberg, Palmeri, Quinet, Biémont, Phys. Rev. A 82, 052512 (…
5p3 2P°3/25p25d 4F3/2285.1948285.11101051.1849E1 (intercombination)0.772 theory1.300e+07 theory30.3Hartman, Nilsson, Engström, Lundberg, Palmeri, Quinet, Biémont, Phys. Rev. A 82, 052512 (…
5p3 2D°3/25p26s 4P1/2287.8757287.79131041.3954E1 (intercombination)0.999 NIST4.240e+07 NIST16.6NIST ASD (accuracy n/a)
5p3 2P°1/25p26s 2P3/2303.0691302.9809989.1884E10.997 theory1.810e+07 theory7.05Hartman, Nilsson, Engström, Lundberg, Palmeri, Quinet, Biémont, Phys. Rev. A 82, 052512 (…
5p3 2P°3/25p26s 2P3/2323.3428323.2495927.1661E11.431 NIST3.070e+07 NIST4.03NIST ASD (accuracy n/a)
5p3 2P°1/25p26s 2P1/2326.8433326.7491917.2360E11.306 NIST4.950e+07 NIST9NIST ASD (accuracy n/a)
5p3 2P°1/25p26s 4P3/2338.4097338.3125885.8861E1 (intercombination)0.186 HFR fit (this site)4.525e+05 HFR fit (this site)0.24This site: Cowan-code HFR calculation of Sb I with the parameters fitted to the NIST ener…
5p3 2P°3/25p26s 4P3/2363.8859363.7823823.8638E1 (intercombination)0.339 HFR fit (this site)1.205e+06 HFR fit (this site)0.639This site: Cowan-code HFR calculation of Sb I with the parameters fitted to the NIST ener…
5p3 2P°1/25p26s 4P1/2372.3843372.2784805.0620E1 (intercombination)0.263 HFR fit (this site)1.356e+06 HFR fit (this site)0.719This site: Cowan-code HFR calculation of Sb I with the parameters fitted to the NIST ener…
5p3 2P°3/25p26s 4P1/2403.4676403.3537743.0397E1 (intercombination)0.309 theory1.470e+06 theory0.759Hartman, Nilsson, Engström, Lundberg, Palmeri, Quinet, Biémont, Phys. Rev. A 82, 052512 (…
5p26s 4P1/25p27p (0,3/2)°3/2563.3498563.1935532.1604E10.700 HFR fit (this site)1.388e+06 HFR fit (this site)–This site: Cowan-code HFR calculation of Sb I with the parameters fitted to the NIST ener…
5p26s 4P1/25p26p (1,3/2)°1/2784.6509784.4351382.0711E10.913 HFR fit (this site)1.747e+06 HFR fit (this site)–This site: Cowan-code HFR calculation of Sb I with the parameters fitted to the NIST ener…
5p26s 4P1/25p26p (1,3/2)°3/2792.6762792.4582378.2029E1––––
5p26s 4P1/25p26p (0,3/2)°3/21068.01711067.7246280.7001E17.749 HFR fit (this site)2.497e+07 HFR fit (this site)–This site: Cowan-code HFR calculation of Sb I with the parameters fitted to the NIST ener…

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.

Sb energy levels

LevelEnergy (cm⁻¹)JParityLifetimegJHyperfine A (MHz)Hyperfine B (MHz)Lifetime sourceHyperfine source
5p3 4S°3/20.0003/2oddstable1.967-299.034-3.68–Fernando, Rochester, Spalding, Smith, Phil. Mag. 5, 1291 (1960) (atomic-beam magnetic res…
5p3 2D°3/28512.1253/2odd1.4 s theory0.889565-561Liu, Yu, Suo, Liu, Sahoo, "Investigating properties of heavy and superheavy atomic system…Hassini, Ben Ahmed, Robaux, Vergès, Wyart, J. Opt. Soc. Am. B 5, 2060 (1988) (Fourier-tra…
5p3 2D°5/29854.0185/2odd13 s theory1.2051468.98–Liu, Yu, Suo, Liu, Sahoo, "Investigating properties of heavy and superheavy atomic system…Hassini, Ben Ahmed, Robaux, Vergès, Wyart, J. Opt. Soc. Am. B 5, 2060 (1988) (Fourier-tra…
5p3 2P°1/216395.3591/2odd270 ms theory0.6884907.6–Liu, Yu, Suo, Liu, Sahoo, "Investigating properties of heavy and superheavy atomic system…Hassini, Ben Ahmed, Robaux, Vergès, Wyart, J. Opt. Soc. Am. B 5, 2060 (1988) (Fourier-tra…
5p3 2P°3/218464.2023/2odd100 ms theory1.277680438Liu, Yu, Suo, Liu, Sahoo, "Investigating properties of heavy and superheavy atomic system…Hassini, Ben Ahmed, Robaux, Vergès, Wyart, J. Opt. Soc. Am. B 5, 2060 (1988) (Fourier-tra…
5p26s 4P1/243249.3371/2even5.3 ns measured2.332––Hartman, Nilsson, Engström, Lundberg, Palmeri, Quinet, Biémont, Phys. Rev. A 82, 052512 (…–
5p26s 4P3/245945.3403/2even5.3 ns measured1.713523.8-471Hartman, Nilsson, Engström, Lundberg, Palmeri, Quinet, Biémont, Phys. Rev. A 82, 052512 (…Lechner et al., "Electromagnetic moments of the antimony isotopes 112-133Sb", arXiv:2311.…
5p26s 2P1/246991.0581/2even3.7 ns measured1.004––Hartman, Nilsson, Engström, Lundberg, Palmeri, Quinet, Biémont, Phys. Rev. A 82, 052512 (…–
5p26s 4P5/248332.4245/2even4.6 ns measured1.547––Hartman, Nilsson, Engström, Lundberg, Palmeri, Quinet, Biémont, Phys. Rev. A 82, 052512 (…–
5p26s 2P3/249391.1333/2even3.8 ns measured1.277––Hartman, Nilsson, Engström, Lundberg, Palmeri, Quinet, Biémont, Phys. Rev. A 82, 052512 (…–
5p26p (0,3/2)°3/252612.4833/2odd––––––
5p25d 4P5/253442.9675/2even7 ns measured–––Hartman, Nilsson, Engström, Lundberg, Palmeri, Quinet, Biémont, Phys. Rev. A 82, 052512 (…–
5p25d 4F3/253527.9563/2even19.5 ns measured–––Hartman, Nilsson, Engström, Lundberg, Palmeri, Quinet, Biémont, Phys. Rev. A 82, 052512 (…–
5p25d 4F5/255120.9435/2even7.8 ns measured–––Hartman, Nilsson, Engström, Lundberg, Palmeri, Quinet, Biémont, Phys. Rev. A 82, 052512 (…–
5p26s 2D3/255232.9633/2even3.7 ns measured0.991––Andersen, Worre Jørgensen, Sørensen, J. Opt. Soc. Am. 64, 891 (1974) (beam-foil), as quot…–
5p26s 2D5/255728.2645/2even3.8 ns measured1.277––Andersen, Worre Jørgensen, Sørensen, J. Opt. Soc. Am. 64, 891 (1974) (beam-foil), as quot…–
5p26p (1,3/2)°3/255864.8283/2odd––––––
5p26p (1,3/2)°1/255993.8581/2odd––––––
5p25d 4P3/256151.8023/2even6 ns measured1.302––Hartman, Nilsson, Engström, Lundberg, Palmeri, Quinet, Biémont, Phys. Rev. A 82, 052512 (…–
5p25d 4F7/256528.1327/2even54 ns measured–––Hartman, Nilsson, Engström, Lundberg, Palmeri, Quinet, Biémont, Phys. Rev. A 82, 052512 (…–
5p25d 4P1/256698.6081/2even10.3 ns measured–––Osherovich, Tezikov, Opt. Spectrosc. 43, 612 (1977) (delayed coincidence), as quoted in T…–
5p25d 2P3/256733.1623/2even3.5 ns measured1.311––Tezikov, Opt. Spectrosc. 44, 121 (1978) (delayed coincidence), as quoted in Table II of H…–
5p25d 2F5/257287.0525/2even9.5 ns measured–––Hartman, Nilsson, Engström, Lundberg, Palmeri, Quinet, Biémont, Phys. Rev. A 82, 052512 (…–
5p25d 4D1/257597.2031/2even11.7 ns measured–––Osherovich, Tezikov, Opt. Spectrosc. 43, 612 (1977) (delayed coincidence), as quoted in T…–
5p27s 4P1/258132.6561/2even––––––
5p25d 4D5/258862.8895/2even10.4 ns measured–––Osherovich, Tezikov, Opt. Spectrosc. 43, 612 (1977) (delayed coincidence), as quoted in T…–
5p25d 2P1/259737.6251/2even––––––
(60404)5/260404.4755/2even––––––
5p26d 2D3/260580.8993/2even––––––
5p27p (0,3/2)°3/261000.2963/2odd––––––
5p25d 2F7/261125.7417/2even3.8 ns measured–––Hartman, Nilsson, Engström, Lundberg, Palmeri, Quinet, Biémont, Phys. Rev. A 82, 052512 (…–
5p27s 2P1/261386.5091/2even––––––
5p25d 2D5/261631.0655/2even––––––
5p25d 2D3/261808.6983/2even––––––
5p26d 4F5/262501.7285/2even––––––
5p27s 2P3/263649.4623/2even––––––
(64432)3/264432.3953/2even––––––
5p26d 2F5/264513.7055/2even––––––
5p25d 2D5/265243.2505/2even––––––
5p25d 2F7/265403.7987/2even––––––
5p26d 2F7/268079.6967/2even––––––
5p28s 4P5/268650.9005/2even––––––

Sb⁺ ionisation limit 69431.34 cm⁻¹ = 8.60839 eV (144.027 nm)

Sources

All transition A_s and branching values are CALCULATED (MCDHF, Hartman et al. 2010, Table III) and marked method 'theory'; they are not measurements. Rows flagged in the paper as affected by convergence problems (upper levels 5d 4P1/2, 4D1/2, 4D5/2) were left out. Lifetimes with method 'experiment' are the laser measurements of Hartman et al.; those with method 'compilation' are older beam-foil / delayed-coincidence values read in Hartman's Table II (originals not opened). Hyperfine constants of the 5p3 2D, 2P levels are for 121Sb and are second-hand (read in Liu et al. 2023, units MHz as printed there). Wavelengths in labels are those printed by Hartman et al. (air above 200 nm, vacuum below). Lechner et al. give A and B for both hyperfine-split levels of the 217.6 nm line for 112-133Sb; only the stable isotopes are recorded here.

Atoms with measured data

All elements: periodic table