Atomic energy level diagrams

Cadmium-114 energy level diagram

Energy levels and transitions of neutral 114Cd (Cd I, nuclear spin I = 0): the 21 strongest classified lines below 2 µm from the NIST Atomic Spectra Database and the 15 levels they connect, each line with its vacuum wavelength, frequency and, for 19 of them, the reduced dipole matrix element. Level energies come from NIST and refer to the natural isotope mixture; transition rates are 16 NIST, 2 measured, 1 theory. Hyperfine constants and measured frequencies are those of this isotope.

Hover a line or a level to isolate it, click to keep it selected. Scroll to zoom, drag to move.

Cadmium-114 energy level diagram with transition wavelengths and dipole matrix elements

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

Key transitions of 114Cd

Transitionλ vac (nm)λ air (nm)ν (THz)|⟨J‖er‖J′⟩| (ea₀)A (s⁻¹)Γ/2π up. (MHz)branch (%)Use
5s2 1S0 – 5s5p 1P°1228.8729228.80231309.864341(20)3.3316.250e+0899.47100228.9 nm resonance line: first-stage MOT / slowing / imag…
5s2 1S0 – 5s5p 3P°2314.1991314.1081954.1480––3.789e-09–314 nm ultra-narrow
5s2 1S0 – 5s5p 3P°1326.1995326.1055919.046234(21)0.1474.184e+050.06659100326.1 nm intercombination line: narrow-line MOT
5s2 1S0 – 5s5p 3P°0332.0716331.9761902.79462(6)––––332 nm optical lattice clock transition
5s5p 3P°2 – 5s5d 3D3361.1537361.0507830.096573(15)4.6001.300e+08––361.2 nm metastable MOT
5s5p 3P°2 – 5s5d 3D1361.5484361.4453829.19040.562*4.510e+06––361.5 nm
5s5p 3P°1 – 5s6s 3S1480.1254479.9912624.40452.5924.100e+07––480.0 nm optical pumping / repumping

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).

Isotope shifts

Transitionλ vac (nm)IsotopesShift (MHz)
5s2 1S0 – 5s5p 1P°1228.873106-1141818(4)
5s2 1S0 – 5s5p 1P°1228.873108-1141336(3)
5s2 1S0 – 5s5p 1P°1228.873110-114865(3)
5s2 1S0 – 5s5p 1P°1228.873112-114408(3)
5s2 1S0 – 5s5p 1P°1228.873116-114-316(3)
5s2 1S0 – 5s5p 1P°1228.873111-114805.0(3)
5s2 1S0 – 5s5p 1P°1228.873113-114344.9(5)
5s2 1S0 – 5s5p 3P°2314.199106-1141916(4)
5s2 1S0 – 5s5p 3P°2314.199108-1141404(3)
5s2 1S0 – 5s5p 3P°2314.199110-114913.7(21)
5s2 1S0 – 5s5p 3P°2314.199112-114429.7(16)
5s2 1S0 – 5s5p 3P°2314.199116-114-320.2(17)
5s2 1S0 – 5s5p 3P°1326.200106-1141913.0(10)
5s2 1S0 – 5s5p 3P°1326.200108-1141402.4(10)
5s2 1S0 – 5s5p 3P°1326.200110-114914.7(10)
5s2 1S0 – 5s5p 3P°1326.200112-114429.9(10)
5s2 1S0 – 5s5p 3P°1326.200116-114-321.5(10)
5s2 1S0 – 5s5p 3P°1326.200111-114861.6(10)
5s2 1S0 – 5s5p 3P°1326.200113-114370.8(10)
5s2 1S0 – 5s5p 3P°0332.072106-1141911(5)
5s2 1S0 – 5s5p 3P°0332.072108-1141404(4)
5s2 1S0 – 5s5p 3P°0332.072110-114914.1(21)

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

Closed and nearly closed transitions of 114Cd

Transitionλ vacuum (nm)Lower levelA (s⁻¹)Leak per scattered photonPhotons before a leakWhere the leak goes
5s2 1S0 → 5s5p 1P°1228.8729ground6.250e+08 measuredclosed–no other level can be reached by electric-dipole decay
5s2 1S0 → 5s5p 3P°1326.1995ground4.184e+05 measuredclosed–no other level can be reached by electric-dipole decay
5s5p 3P°2 → 5s5d 3D3361.1537metastable1.300e+08 NIST3.81 × 10−4 from this site's HFR fit2,6205s6p 3P°2 ≈ 3.81 × 10−4

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 114Cd 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
5s2 1S05s5p 1P°1228.8729228.80231309.8643E13.331 measured6.250e+08 measured100Hofsaess, Padilla-Castillo, Wright, Kray, Thomas, Sartakov, Ohayon, Meijer, Truppe, 'High…
5s5p 3P°05s6d 3D1283.7734283.69001056.4501E10.973 NIST2.800e+07 NIST–NIST ASD (accuracy D)
5s5p 3P°15s6d 3D2288.1612288.07671040.3636E11.575 NIST4.200e+07 NIST–NIST ASD (accuracy D)
5s5p 3P°15s6d 3D1288.2070288.12251040.1984E10.922 NIST2.400e+07 NIST–NIST ASD (accuracy D)
5s5p 3P°25s6d 3D3298.1490298.06201005.5122E12.324 NIST5.900e+07 NIST–NIST ASD (accuracy D)
5s5p 3P°25s6d 3D2298.2232298.13621005.2619E10.991 NIST1.500e+07 NIST–NIST ASD (accuracy D)
5s2 1S05s5p 3P°2314.1991314.1081954.1480M2––––
5s2 1S05s5p 3P°1326.1995326.1055919.0462E1 (intercombination)0.147 measured4.184e+05 measured100Hofsaess, Padilla-Castillo, Wright, Kray, Thomas, Sartakov, Ohayon, Meijer, Truppe, 'High…
5s2 1S05s5p 3P°0332.0716331.9761902.7946clock––––
5s5p 3P°05s5d 3D1340.4629340.3652880.5438E12.121 NIST7.700e+07 NIST–NIST ASD (accuracy C)
5s5p 3P°15s5d 3D2346.7192346.6200864.6548E13.513 NIST1.200e+08 NIST–NIST ASD (accuracy D)
5s5p 3P°15s5d 3D1346.8647346.7654864.2921E12.035 NIST6.700e+07 NIST–NIST ASD (accuracy D)
5s5p 3P°25s5d 3D3361.1537361.0507830.0966E14.600 NIST1.300e+08 NIST–NIST ASD (accuracy D)
5s5p 3P°25s5d 3D2361.3903361.2872829.5532E12.019 NIST3.500e+07 NIST–NIST ASD (accuracy D)
5s5p 3P°25s5d 3D1361.5484361.4453829.1904E10.562 theory4.510e+06 theory–Robert, Manzoor, Chiarotti, Poli, 'Multipole transition amplitudes and radiative decay ra…
5s5p 1P°15s7d 1D2414.1470414.0302723.8794E10.908 NIST4.700e+06 NIST–NIST ASD (accuracy D)
5s5p 1P°15s6d 1D2466.3657466.2352642.8270E11.173 NIST5.500e+06 NIST–NIST ASD (accuracy C)
5s5p 3P°05s6s 3S1467.9459467.8150640.6562E11.404 NIST1.300e+07 NIST–NIST ASD (accuracy C)
5s5p 3P°15s6s 3S1480.1254479.9912624.4045E12.592 NIST4.100e+07 NIST–NIST ASD (accuracy C)
5s5p 3P°25s6s 3S1508.7239508.5821589.3029E13.304 NIST5.600e+07 NIST–NIST ASD (accuracy C)
5s5p 1P°15s5d 1D2644.0249643.8469465.4982E16.236 NIST5.900e+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.

114Cd energy levels

LevelEnergy (cm⁻¹)JParityLifetimegJHyperfine A (MHz)Hyperfine B (MHz)Lifetime sourceHyperfine source
5s2 1S00.0000evenstable–––––
5s5p 3P°030113.9900odd––––––
5s5p 3P°130656.0871odd2.39 µs measured–––Hofsaess, Padilla-Castillo, Wright, Kray, Thomas, Sartakov, Ohayon, Meijer, Truppe, 'High…–
5s5p 3P°231826.9522odd42 s theory–––Robert, Manzoor, Chiarotti, Poli, 'Multipole transition amplitudes and radiative decay ra…–
5s5p 1P°143692.3841odd1.6 ns measured–––Hofsaess, Padilla-Castillo, Wright, Kray, Thomas, Sartakov, Ohayon, Meijer, Truppe, 'High…–
5s6s 3S151483.9801even––––––
5s5d 1D259219.7342even––––––
5s5d 3D159485.7681even––––––
5s5d 3D259497.8682even––––––
5s5d 3D359515.9903even––––––
5s6d 1D265134.7832even––––––
5s6d 3D165353.3721even––––––
5s6d 3D265358.8812even––––––
5s6d 3D365367.2273even––––––
5s7d 1D267838.4012even––––––

Cd⁺ ionisation limit 72540.05 cm⁻¹ = 8.99382 eV (137.855 nm)

Sources

Conventions. (1) Isotope-shift keys 'a-b' mean nu(a) - nu(b); all Cd shifts are relative to 114Cd as printed. Fermion shifts are hyperfine centres of gravity. (2) Hyperfine entries carry the measured interval (interval_MHz) and a derived A_MHz; I = 1/2 so B = 0. (3) Fields beyond SCHEMA.md: natural_linewidth_*, interval_MHz, photoionization, magic_wavelength_nm, bbr_shift_Hz, type 'M2', top-level 'rydberg' (ionization limit) and 'conflicts'. (4) rme_J_ea0 values are derived here from measured lifetimes with the schema convention (branching to the ground state taken as 1); they are not printed in the sources. (5) The clock (332 nm) and 314 nm isotope shifts are King-plot derived values of Ohayon et al., not direct measurements.

Atoms with measured data

All elements: periodic table