Atomic energy level diagrams

Bromine energy level diagram

Energy levels and transitions of neutral bromine (Br I): the 47 strongest classified lines below 2 µm from the NIST Atomic Spectra Database and the 33 levels they connect, each line with its vacuum wavelength, frequency and, for 45 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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Bromine energy level diagram with transition wavelengths and dipole matrix elements

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

Key transitions of bromine

Transitionλ vac (nm)λ air (nm)ν (THz)|⟨J‖er‖J′⟩| (ea₀)A (s⁻¹)Γ/2π up. (MHz)branch (%)Use
2P°3/2 – 2[1]°3/2126.2972–2373.7066––5.151–TALIF detection of ground-state Br: 2 x 252.594 nm, fluor…
2P°3/2 – 2[1]°3/2130.3049–2300.6997––––two-photon LIF scheme near 260.6 nm with fluorescence 5p…
2P°3/2 – 2[1]3/2148.8459–2014.11311.1412.000e+08––148.8 nm resonance line
2P°3/2 – 2[2]3/2154.0661–1945.86861.2602.200e+08––154.1 nm resonance line
2P°1/2 – 2[1]3/2157.4844–1903.63230.3932.000e+07––157.5 nm line to the metastable 2P°1/2 level
2P°3/2 – 2[2]5/2157.6381–1901.77690.2575.700e+06––157.6 nm resonance line
2P°1/2 – 2[2]3/2163.3401–1835.38790.4452.300e+07––163.3 nm line to the metastable 2P°1/2 level
2[2]5/2 – 2[1]°3/2635.2481635.0725471.92971.0552.200e+065.1516.8635.25 nm fluorescence line used to detect Br atoms after…

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).

79Br hyperfine structure (I = 3/2)

LevelA (MHz)B (MHz)Shift of each F level from the centre of gravity (MHz)
2P°3/2884.80977(6)-384.88284(20)F=0: -3799.14 F=1: -2529.45 F=2: -374.94 F=3: +1894.60
2P°1/25332.55(4)–F=1: -6665.69 F=2: +3999.41

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

Closed and nearly closed transitions of bromine

Transitionλ vacuum (nm)Lower levelA (s⁻¹)Leak per scattered photonPhotons before a leakWhere the leak goes
2P°3/2 → 2[2]5/2157.6381ground5.700e+06 measuredclosed–no other level can be reached by electric-dipole decay
2P°3/2 → 2[2]5/2131.7691ground1.000e+09 NIST≥ 6.81 × 10−7 from this site's HFR fit≤ 1.47 × 1062[2]°5/2 ≈ 3.93 × 10−7; 2[2]°3/2 ≈ 2.88 × 10−7; 2 more possible paths without a listed rate
2P°1/2 → 2[2]3/2138.4595metastable5.000e+08 NIST≥ 5.3 % from this site's HFR fit≤ 192P°3/2 5.3 % (long-lived); 2[2]°3/2 ≈ 7.47 × 10−7; 2[2]°5/2 ≈ 2.04 × 10−7; 2 more possible paths without a listed rate
2P°3/2 → 2[1]3/2148.8459ground2.000e+08 measured9.09 % from measured data112P°1/2 9.09 % (long-lived)
2P°3/2 → 2[2]3/2154.0661ground2.200e+08 measured9.47 % from measured data112P°1/2 9.47 % (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 Br 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
2P°3/22S1/2117.8889–2543.0075E10.0985 NIST6.000e+06 NIST–NIST ASD (accuracy E)
2P°3/22[1]°3/2126.2972–2373.7066two-photon––––
2P°3/22[1]°3/2130.3049–2300.6997two-photon––––
2P°3/22[2]3/2131.7375–2275.6805E10.355 NIST2.800e+07 NIST–NIST ASD (accuracy E)
2P°3/22[2]5/2131.7691–2275.1349E12.603 NIST1.000e+09 NIST–NIST ASD (accuracy E)
2P°1/22[2]3/2138.4595–2165.1998E11.619 NIST5.000e+08 NIST–NIST ASD (accuracy E)
2P°3/22[0]1/2144.9901–2067.6749E11.646 NIST9.000e+08 NIST–NIST ASD (accuracy E)
2P°3/22[1]3/2148.8459–2014.1131E11.141 measured2.000e+08 measured–Tellinghuisen & Clyne, J. Chem. Soc. Faraday Trans. 2 72, 783 (1976) (line-absorption osc…
2P°1/22[0]1/2153.1746–1957.1942E11.459 NIST6.000e+08 NIST–NIST ASD (accuracy E)
2P°3/22[2]3/2154.0661–1945.8686E11.260 measured2.200e+08 measured–Tellinghuisen & Clyne, J. Chem. Soc. Faraday Trans. 2 72, 783 (1976) (line-absorption osc…
2P°1/22[1]3/2157.4844–1903.6323E10.393 measured2.000e+07 measured–Tellinghuisen & Clyne, J. Chem. Soc. Faraday Trans. 2 72, 783 (1976) (line-absorption osc…
2P°3/22[2]5/2157.6381–1901.7769E10.257 measured5.700e+06 measured–Tellinghuisen & Clyne, J. Chem. Soc. Faraday Trans. 2 72, 783 (1976) (line-absorption osc…
2P°1/22[1]1/2158.2313–1894.6473E10.442 NIST5.000e+07 NIST–NIST ASD (accuracy E)
2P°1/22[2]3/2163.3401–1835.3879E10.445 measured2.300e+07 measured–Tellinghuisen & Clyne, J. Chem. Soc. Faraday Trans. 2 72, 783 (1976) (line-absorption osc…
2[1]1/22[1]°3/2436.6372436.5145686.5940E10.496 NIST1.500e+06 NIST–NIST ASD (accuracy D+)
2[2]3/22[1]°1/2442.6377442.5134677.2863E10.278 NIST9.000e+05 NIST–NIST ASD (accuracy D+)
2[2]5/22[1]°3/2444.2981444.1734674.7552E10.510 NIST1.500e+06 NIST–NIST ASD (accuracy C)
2[2]3/22[1]°3/2447.3853447.2597670.0991E10.624 NIST2.200e+06 NIST–NIST ASD (accuracy D)
2[2]5/22[3]°7/2447.8976447.7720669.3325E10.863 NIST2.100e+06 NIST–NIST ASD (accuracy C)
2[1]1/22[1]°1/2449.1671449.0411667.4408E10.378 NIST1.600e+06 NIST–NIST ASD (accuracy E)
2[2]5/22[2]°3/2451.4703451.3437664.0358E10.322 NIST5.700e+05 NIST–NIST ASD (accuracy D+)
2[2]5/22[2]°5/2452.6859452.5590662.2526E10.642 NIST1.500e+06 NIST–NIST ASD (accuracy D+)
2[1]3/22[1]°3/2498.1144497.9754601.8546E10.360 NIST5.300e+05 NIST–NIST ASD (accuracy D+)
2[1]3/22[3]°5/2536.5685536.4193558.7217E10.115 NIST2.900e+04 NIST–NIST ASD (accuracy E)
2[1]3/22[1]°1/2537.1836537.0342558.0820E10.0875 NIST5.000e+04 NIST–NIST ASD (accuracy E)
2[2]5/22[1]°3/2635.2481635.0725471.9297E11.055 NIST2.200e+06 NIST6.8NIST ASD (accuracy C)
2[2]5/22[2]°3/2656.1594655.9782456.8897E10.625 NIST7.000e+05 NIST–NIST ASD (accuracy C)
2[2]5/22[2]°5/2663.3433663.1602451.9416E10.778 NIST7.000e+05 NIST–NIST ASD (accuracy C)
2[2]3/22[1]°3/2700.7149700.5217427.8380E11.709 NIST4.300e+06 NIST13.3NIST ASD (accuracy C)
2[2]3/22[2]°3/2726.2449726.0448412.7980E10.651 NIST5.600e+05 NIST–NIST ASD (accuracy C)
2[2]3/22[2]°5/2735.0558734.8533407.8499E12.351 NIST4.700e+06 NIST–NIST ASD (accuracy C)
2[1]3/22[1]°3/2799.2129798.9932375.1096E11.768 NIST3.100e+06 NIST–NIST ASD (accuracy C)
2[1]1/22[1]°3/2813.3745813.1509368.5786E12.305 NIST5.000e+06 NIST15.4NIST ASD (accuracy C)
2[2]5/22[3]°7/2827.4686827.2413362.3007E18.849 NIST3.500e+07 NIST–NIST ASD (accuracy C+)
2[1]3/22[1]°3/2833.6981833.4690359.5936E14.129 NIST1.490e+07 NIST46NIST ASD (accuracy C+)
2[1]1/22[1]°1/2834.5957834.3663359.2068E14.285 NIST3.200e+07 NIST–NIST ASD (accuracy C+)
2[2]3/22[1]°3/2844.8879844.6558354.8311E15.774 NIST2.800e+07 NIST–NIST ASD (accuracy D)
2[1]1/22[2]°3/2847.9765847.7435353.5387E15.262 NIST2.300e+07 NIST–NIST ASD (accuracy C+)
2[2]5/22[2]°3/2864.1041863.8668346.9402E15.294 NIST2.200e+07 NIST–NIST ASD (accuracy C+)
2[1]3/22[2]°3/2870.0895869.8506344.5536E15.587 NIST2.400e+07 NIST–NIST ASD (accuracy C+)
2[2]5/22[3]°7/2882.2364881.9942339.8096E19.019 NIST3.000e+07 NIST–NIST ASD (accuracy C+)
2[1]3/22[2]°5/2882.7668882.5245339.6055E17.818 NIST3.000e+07 NIST–NIST ASD (accuracy C+)
2[2]5/22[2]°5/2890.0067889.7624336.8429E17.914 NIST3.000e+07 NIST–NIST ASD (accuracy C+)
2[1]1/22[0]°1/2893.4850893.2397335.5316E11.477 NIST3.100e+06 NIST–NIST ASD (accuracy D)
2[2]3/22[1]°1/2916.8584916.6068326.9779E14.856 NIST3.100e+07 NIST–NIST ASD (accuracy C+)
2[1]3/22[0]°1/2918.0696917.8177326.5465E14.625 NIST2.800e+07 NIST–NIST ASD (accuracy C+)
2[2]3/22[3]°5/2926.7961926.5418323.4719E17.522 NIST2.400e+07 NIST–NIST ASD (accuracy C+)

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.

Br energy levels

LevelEnergy (cm⁻¹)JParityLifetimegJHyperfine A (MHz)Hyperfine B (MHz)Lifetime sourceHyperfine source
2P°3/20.0003/2oddstable1.3339884.81-384.883–atomic-beam magnetic resonance: Brown & King, Phys. Rev. 142, 53 (1966); King & Jaccarino…
2P°1/23685.2401/2odd960 ms measured0.66555332.55–He, Seth, Tokue, Macdonald, J. Chem. Phys. 110, 7821 (1999) (colour-centre-laser absorpti…Davies, Thrush, Stone, Wayne, Chem. Phys. Lett. 17, 19 (1972) (EPR) and Bessis, Picart, D…
2[2]5/263436.4505/2even–1.595––––
2[2]3/264907.1903/2even–1.532––––
2[1]1/266883.8701/2even–2.608––––
2[1]3/267183.5803/2even–1.522––––
2[0]1/268970.2101/2even–0.734––––
2[2]°5/274672.3205/2odd––––––
2[2]°3/275009.1303/2odd–0.826––––
2[3]°7/275521.5007/2odd––––––
2[3]°5/275697.0505/2odd––––––
2[1]°1/275814.0001/2odd––––––
2[2]5/275890.3305/2even–1.21––––
2[2]3/275908.5303/2even––––––
2[1]°3/276743.0803/2odd––––––
2[0]°1/278076.0001/2odd––––––
2[2]°5/278511.6005/2odd––––––
2[2]°3/278676.6503/2odd––––––
2[1]°1/278865.7201/2odd––––––
2[1]°3/279178.3303/2odd30.9 ns measured–––Sirse, Foucher, Chabert, Booth, Plasma Sources Sci. Technol. 23, 062003 (2014), abstract–
2[1]°3/279695.8903/2odd––––––
2S1/284825.6001/2even––––––
2[2]°5/285526.8205/2odd–1.46––––
2[2]°3/285586.3003/2odd–1.54––––
2[3]°7/285762.9807/2odd–1.43––––
2[1]°1/285799.1901/2odd––––––
2[3]°5/285820.5305/2odd–1.23––––
2[1]°3/285943.8603/2odd–1.62––––
2[3]°7/287225.1607/2odd––––––
2[1]°3/287259.2903/2odd––––––
2[1]°1/287499.0301/2odd––––––
2[1]°1/289147.3001/2odd–2.26––––
2[1]°3/289786.1803/2odd––––––

Br⁺ ionisation limit 95284.80 cm⁻¹ = 11.81381 eV (104.949 nm)

Sources

Literature search was limited: the session's web-search quota was exhausted, so sources were located through Crossref, HAL, OSTI, arXiv and NASA ADS queries and only open copies could be read. Ground-term hyperfine constants are second-hand from Chichinin's JPCRD review (method 'compilation'); the King & Jaccarino 1954 numbers were read on the APS abstract page. B < 0 for both isotopes as printed. The M1 A value is the calculated one adopted by NIST. Two-photon entries: wavelength_vac_nm is the laser wavelength. Second pass (2026-10-01): the measured lifetime of the TALIF upper level was found in the abstract reproduced by OSTI/INIS (ETDEWEB record 22362940). Third pass (2026-10-02): added the five 4p5 2P - 5s vacuum-ultraviolet resonance lines with measured A values. NIST's transition-probability reference T3064 for these lines was checked to be Tellinghuisen & Clyne 1976, the hyperfine-corrected re-analysis of the Clyne & Townsend 1974 absorption measurements; the uncorrected 1974 oscillator strengths (read in the abstract on the archived RSC page) are kept as alternatives, converted to A (derived). Morton 2000 (saved as pdf/Br_Morton_2000.pdf) states that the 1976 paper corrected the 1974 one.

Atoms with measured data

All elements: periodic table