Xenon energy level diagram
Energy levels and transitions of neutral xenon (Xe I): the 72 strongest classified lines below 2 µm from the NIST Atomic Spectra Database and the 51 levels they connect, each line with its vacuum wavelength, frequency and, for 70 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.

Download: diagram (PDF) diagram (SVG) transitions (CSV) levels (CSV) source code
Key transitions of xenon
| Transition | λ vac (nm) | λ air (nm) | ν (THz) | |⟨J‖er‖J′⟩| (ea₀) | A (s⁻¹) | Γ/2π up. (MHz) | branch (%) | Use |
|---|---|---|---|---|---|---|---|---|
| 1S0 – 2[1/2]°1 | 104.3835 | – | 2872.02930(10) | 0.315 | 5.900e+07 | – | – | 104.4 nm VUV line: absolute calibration, hyperfine struct… |
| 1S0 – 2[3/2]°1 | 105.6128 | – | 2838.5989 | 0.580 | 1.930e+08 | – | – | 105.6 nm VUV line: absolute calibration, hyperfine struct… |
| 1S0 – 2[1/2]°1 | 106.1256 | – | 2824.8845 | 0.175 | 1.740e+07 | – | – | 106.1 nm VUV line: absolute calibration used for the ioni… |
| 1S0 – 2[3/2]°1 | 106.8168 | – | 2806.6042 | 0.819 | 3.720e+08 | – | – | 106.8 nm VUV line |
| 1S0 – 2[3/2]°1 | 109.9718 | – | 2726.086012 | 0.283 | 4.080e+07 | – | – | 110 nm line measured by Ramsey-comb |
| 1S0 – 2[3/2]°1 | 146.9612 | – | 2039.9425 | 1.133 | 2.730e+08 | – | – | 147 nm resonance line: VUV-lamp first step of the optical… |
| 1S0 – 2[3/2]°2 | 149.1034 | – | 2010.6345 | – | 2.331e-02 | 3.71e-09 | 100 | 149.1 nm M2 decay of the metastable 3P2 state |
| 2[3/2]°2 – 2[1/2]1 | 450.2241 | 450.0979 | 665.873836 | 0.444 | 1.460e+06 | – | – | 450.1 nm |
| 2[1/2]°0 – 2[1/2]1 | 764.4127 | 764.2023 | 392.186651 | 3.727 | 2.100e+07 | – | – | 764.2 nm |
| 2[1/2]°0 – 2[3/2]1 | 820.8591 | 820.6335 | 365.2179 | 4.047 | 2.000e+07 | – | – | 820.86 nm |
| 2[3/2]°2 – 2[3/2]2 | 823.3897 | 823.1634 | 364.0955 | 6.277 | 2.860e+07 | – | – | 823.2 nm |
| 2[3/2]°2 – 2[3/2]1 | 841.1501 | 840.9190 | 356.4078 | 1.642 | 3.060e+06 | – | – | 841.15 nm |
| 2[3/2]°2 – 2[5/2]3 | 882.1832 | 881.9410 | 339.8302 | 8.436 | 3.000e+07 | 4.681 | 100 | 881.9 nm |
| 2[3/2]°1 – 2[3/2]2 | 895.4709 | 895.2251 | 334.7875 | 3.789 | 8.100e+06 | – | – | 895.5 nm second step |
| 2[3/2]°1 – 2[3/2]1 | 916.5168 | 916.2653 | 327.0998 | 5.231 | 2.400e+07 | – | – | 916 nm optical pumping into 6p[3/2]1, which decays to the… |
| 2[3/2]°2 – 2[1/2]°0 | 1095.3836 | 1095.0837 | 273.687184 | – | – | 1.243e-06 | – | proposed optical frequency standard: two-photon clock tra… |
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).
129Xe hyperfine structure (I = 1/2)
| Level | A (MHz) | B (MHz) | Shift of each F level from the centre of gravity (MHz) |
|---|---|---|---|
| 2[3/2]°2 | -2384.4(12) | – | F=3/2: +3576.60 F=5/2: -2384.40 |
| 2[3/2]°1 | -959.1(7) | – | F=1/2: +959.10 F=3/2: -479.55 |
| 2[1/2]°1 | -5808.0(20) | – | F=1/2: +5808.00 F=3/2: -2904.00 |
| 2[3/2]1 | -1308.9(6) | – | F=1/2: +1308.89 F=3/2: -654.45 |
| 2[3/2]2 | -889.6(4) | – | F=3/2: +1334.40 F=5/2: -889.60 |
| 2[3/2]1 | -4424.0(10) | – | F=1/2: +4424.00 F=3/2: -2212.00 |
| 2[3/2]1 | -2740.4(9) | – | F=1/2: +2740.40 F=3/2: -1370.20 |
| 2[3/2]2 | -2895(5) | – | F=3/2: +4341.90 F=5/2: -2894.60 |
| 2[1/2]1 | 1977.0(10) | – | F=1/2: -1977.00 F=3/2: +988.50 |
| 2[3/2]°1 | 1657(12) | – | F=1/2: -1657.00 F=3/2: +828.50 |
| 2[1/2]°1 | -579(6) | – | F=1/2: +579.00 F=3/2: -289.50 |
| 2[3/2]°1 | 913(23) | – | F=1/2: -913.00 F=3/2: +456.50 |
| 2[1/2]°1 | -4548(15) | – | F=1/2: +4548.00 F=3/2: -2274.00 |
Measured A, B constants; sources in the data file.
Isotope shifts
| Transition | λ vac (nm) | Isotopes | Shift (MHz) |
|---|---|---|---|
| 1S0 – 2[1/2]°1 | 104.383 | 136-134 | 213(12) |
| 1S0 – 2[1/2]°1 | 104.383 | 136-132 | 365(18) |
| 1S0 – 2[1/2]°1 | 104.383 | 136-131 | 492(20) |
| 1S0 – 2[1/2]°1 | 104.383 | 136-130 | 523(24) |
| 1S0 – 2[1/2]°1 | 104.383 | 136-129 | 678(24) |
| 1S0 – 2[1/2]°1 | 104.383 | 136-128 | 692(22) |
| 1S0 – 2[1/2]°1 | 104.383 | 136-126 | 869(25) |
| 1S0 – 2[1/2]°1 | 104.383 | 136-124 | 1069(22) |
| 1S0 – 2[3/2]°1 | 105.613 | 136-134 | 219(15) |
| 1S0 – 2[3/2]°1 | 105.613 | 136-132 | 354(20) |
| 1S0 – 2[3/2]°1 | 105.613 | 136-131 | 545(17) |
| 1S0 – 2[3/2]°1 | 105.613 | 136-130 | 529(30) |
| 1S0 – 2[3/2]°1 | 105.613 | 136-129 | 684(27) |
| 1S0 – 2[3/2]°1 | 105.613 | 136-128 | 726(20) |
| 1S0 – 2[3/2]°1 | 105.613 | 136-126 | 912(20) |
| 1S0 – 2[3/2]°1 | 105.613 | 136-124 | 1116(20) |
| 1S0 – 2[1/2]°1 | 106.126 | 136-134 | 207(12) |
| 1S0 – 2[1/2]°1 | 106.126 | 136-132 | 384(18) |
| 1S0 – 2[1/2]°1 | 106.126 | 136-131 | 531(23) |
| 1S0 – 2[1/2]°1 | 106.126 | 136-130 | 557(11) |
| 1S0 – 2[1/2]°1 | 106.126 | 136-129 | 675(14) |
| 1S0 – 2[1/2]°1 | 106.126 | 136-128 | 747(19) |
Shift = ν(first isotope) − ν(second isotope).
Closed and nearly closed transitions of xenon
| Transition | λ vacuum (nm) | Lower level | A (s⁻¹) | Leak per scattered photon | Photons before a leak | Where the leak goes |
|---|---|---|---|---|---|---|
| 1S0 → 2[3/2]°1 | 146.9612 | ground | 2.730e+08 NIST | closed | – | no other level can be reached by electric-dipole decay |
| 1S0 → 2[1/2]°1 | 129.5588 | ground | 2.530e+08 NIST | closed | – | no other level can be reached by electric-dipole decay |
| 2[3/2]°2 → 2[5/2]3 | 882.1832 | metastable | 3.000e+07 NIST | closed | – | no other level can be reached by electric-dipole decay |
| 1S0 → 2[3/2]°1 | 119.2038 | ground | 5.930e+08 NIST | ≥ 0.51 % from NIST data | ≤ 196 | 2[3/2]1 0.403 %; 2[5/2]2 8.05 × 10−4; 2[1/2]0 2.68 × 10−4; 2 more possible paths without a listed rate |
| 1S0 → 2[1/2]°1 | 125.0209 | ground | 1.490e+07 NIST | ≥ 2.31 % from this site's HFR fit | ≤ 43 | 2[1/2]1 2.29 %; 2[3/2]2 ≈ 1.27 × 10−4; 2 more possible paths without a listed rate |
| 2[3/2]°2 → 2[1/2]1 | 980.2386 | metastable | 3.110e+07 NIST | ≥ 5.49 % from this site's HFR fit | ≤ 18 | 2[3/2]°1 5.47 %; 2[1/2]°0 ≈ 1.93 × 10−4 (long-lived); 1 more possible path without a listed rate |
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 Xe transitions below 2 µm
| Lower level | Upper level | λ vacuum (nm) | λ air (nm) | ν (THz) | Type | |⟨J‖er‖J′⟩| (ea₀) | A (s⁻¹) | Branching (%) | Source of matrix element / A |
|---|---|---|---|---|---|---|---|---|---|
| 1S0 | 2[3/2]°1 | 104.1170 | – | 2879.3798 | E1 | 0.363 NIST | 7.900e+07 NIST | – | NIST ASD (accuracy C+) |
| 1S0 | 2[1/2]°1 | 104.3835 | – | 2872.0293 | E1 | 0.315 NIST | 5.900e+07 NIST | – | NIST ASD (accuracy C) |
| 1S0 | 2[3/2]°1 | 104.7137 | – | 2862.9724 | E1 | 0.465 NIST | 1.270e+08 NIST | – | NIST ASD (accuracy C+) |
| 1S0 | 2[1/2]°1 | 105.0107 | – | 2854.8756 | E1 | 0.121 NIST | 8.500e+06 NIST | – | NIST ASD (accuracy D+) |
| 1S0 | 2[3/2]°1 | 105.4996 | – | 2841.6453 | E1 | 0.316 NIST | 5.750e+07 NIST | – | NIST ASD (accuracy C+) |
| 1S0 | 2[3/2]°1 | 105.6128 | – | 2838.5989 | E1 | 0.580 NIST | 1.930e+08 NIST | – | NIST ASD (accuracy C+) |
| 1S0 | 2[1/2]°1 | 106.1256 | – | 2824.8845 | E1 | 0.175 NIST | 1.740e+07 NIST | – | NIST ASD (accuracy C+) |
| 1S0 | 2[3/2]°1 | 106.8168 | – | 2806.6042 | E1 | 0.819 NIST | 3.720e+08 NIST | – | NIST ASD (accuracy C+) |
| 1S0 | 2[3/2]°1 | 107.0410 | – | 2800.7243 | E1 | 0.148 NIST | 1.200e+07 NIST | – | NIST ASD (accuracy D+) |
| 1S0 | 2[3/2]°1 | 107.8585 | – | 2779.4969 | E1 | 0.119 NIST | 7.600e+06 NIST | – | NIST ASD (accuracy D+) |
| 1S0 | 2[1/2]°1 | 108.5443 | – | 2761.9366 | E1 | 0.285 NIST | 4.280e+07 NIST | – | NIST ASD (accuracy C+) |
| 1S0 | 2[3/2]°1 | 109.9718 | – | 2726.0860 | E1 | 0.283 NIST | 4.080e+07 NIST | – | NIST ASD (accuracy C+) |
| 1S0 | 2[3/2]°1 | 111.0714 | – | 2699.0961 | E1 | 0.552 NIST | 1.500e+08 NIST | – | NIST ASD (accuracy C+) |
| 1S0 | 2[1/2]°1 | 112.9308 | – | 2654.6555 | E1 | 0.0969 NIST | 4.400e+06 NIST | – | NIST ASD (accuracy D+) |
| 1S0 | 2[3/2]°1 | 117.0412 | – | 2561.4273 | E1 | 0.574 NIST | 1.390e+08 NIST | – | NIST ASD (accuracy B+) |
| 1S0 | 2[3/2]°1 | 119.2038 | – | 2514.9581 | E1 | 1.220 NIST | 5.930e+08 NIST | – | NIST ASD (accuracy B+) |
| 1S0 | 2[1/2]°1 | 125.0209 | – | 2397.9385 | E1 | 0.208 NIST | 1.490e+07 NIST | – | NIST ASD (accuracy B+) |
| 1S0 | 2[1/2]°1 | 129.5588 | – | 2313.9493 | E1 | 0.903 NIST | 2.530e+08 NIST | 80.2 | NIST ASD (accuracy A+) |
| 1S0 | 2[3/2]°1 | 146.9612 | – | 2039.9425 | E1 | 1.133 NIST | 2.730e+08 NIST | – | NIST ASD (accuracy A+) |
| 1S0 | 2[3/2]°2 | 149.1034 | – | 2010.6345 | M2 | – | 2.331e-02 measured | 100 | Walhout, Witte, Rolston, Phys. Rev. Lett. 72, 2843 (1994) (abstract) |
| 2[3/2]°2 | 2[3/2]2 | 368.6950 | 368.5900 | 813.1179 | E1 | 0.236 NIST | 4.500e+05 NIST | – | NIST ASD (accuracy D) |
| 2[3/2]°2 | 2[5/2]3 | 369.4538 | 369.3487 | 811.4477 | E1 | 0.232 NIST | 3.100e+05 NIST | – | NIST ASD (accuracy D+) |
| 2[3/2]°2 | 2[5/2]3 | 379.7384 | 379.6306 | 789.4710 | E1 | 0.174 NIST | 1.600e+05 NIST | – | NIST ASD (accuracy C) |
| 2[3/2]°2 | 2[3/2]2 | 395.2042 | 395.0924 | 758.5761 | E1 | 0.292 NIST | 5.600e+05 NIST | 16 | NIST ASD (accuracy C+) |
| 2[3/2]°2 | 2[5/2]3 | 396.8663 | 396.7540 | 755.3991 | E1 | 0.338 NIST | 5.300e+05 NIST | 22.2 | NIST ASD (accuracy C+) |
| 2[3/2]°2 | 2[5/2]3 | 419.4711 | 419.3530 | 714.6915 | E1 | 0.237 NIST | 2.200e+05 NIST | – | NIST ASD (accuracy B) |
| 2[3/2]°2 | 2[1/2]1 | 450.2241 | 450.0979 | 665.8738 | E1 | 0.444 NIST | 1.460e+06 NIST | – | NIST ASD (accuracy C+) |
| 2[3/2]°2 | 2[3/2]2 | 452.5950 | 452.4681 | 662.3857 | E1 | 0.324 NIST | 4.600e+05 NIST | – | NIST ASD (accuracy C+) |
| 2[3/2]°1 | 2[1/2]0 | 458.4031 | 458.2747 | 653.9930 | E1 | 0.249 NIST | 1.300e+06 NIST | – | NIST ASD (accuracy C) |
| 2[3/2]°2 | 2[3/2]2 | 462.5571 | 462.4276 | 648.1199 | E1 | 0.769 NIST | 2.420e+06 NIST | 25.9 | NIST ASD (accuracy B) |
| 2[3/2]°2 | 2[5/2]3 | 467.2533 | 467.1226 | 641.6058 | E1 | 0.937 NIST | 2.490e+06 NIST | 45.6 | NIST ASD (accuracy B) |
| 2[3/2]°2 | 2[3/2]1 | 469.2285 | 469.0972 | 638.9051 | E1 | 0.207 NIST | 2.800e+05 NIST | – | NIST ASD (accuracy C+) |
| 2[3/2]°2 | 2[5/2]2 | 469.8335 | 469.7021 | 638.0823 | E1 | 0.434 NIST | 7.360e+05 NIST | 12.4 | NIST ASD (accuracy B) |
| 2[3/2]°1 | 2[3/2]2 | 473.5476 | 473.4152 | 633.0777 | E1 | 0.601 NIST | 1.380e+06 NIST | – | NIST ASD (accuracy C+) |
| 2[3/2]°1 | 2[1/2]0 | 480.8363 | 480.7019 | 623.4814 | E1 | 0.485 NIST | 4.290e+06 NIST | 37.3 | NIST ASD (accuracy B) |
| 2[3/2]°1 | 2[3/2]1 | 483.1057 | 482.9708 | 620.5525 | E1 | 0.317 NIST | 6.000e+05 NIST | 6 | NIST ASD (accuracy D+) |
| 2[3/2]°1 | 2[3/2]2 | 484.4646 | 484.3293 | 618.8119 | E1 | 0.444 NIST | 7.020e+05 NIST | 7.51 | NIST ASD (accuracy B) |
| 2[3/2]°1 | 2[3/2]1 | 491.7879 | 491.6506 | 609.5971 | E1 | 0.531 NIST | 1.600e+06 NIST | – | NIST ASD (accuracy C+) |
| 2[3/2]°1 | 2[5/2]2 | 492.4525 | 492.3151 | 608.7743 | E1 | 0.536 NIST | 9.740e+05 NIST | 16.4 | NIST ASD (accuracy B) |
| 2[1/2]1 | 2[3/2]°2 | 530.7834 | 530.6358 | 564.8112 | E1 | 0.243 NIST | 1.600e+05 NIST | – | NIST ASD (accuracy C+) |
| 2[1/2]1 | 2[3/2]°2 | 546.1551 | 546.0034 | 548.9145 | E1 | 0.317 NIST | 2.500e+05 NIST | – | NIST ASD (accuracy B+) |
| 2[1/2]1 | 2[3/2]°2 | 571.7297 | 571.5712 | 524.3605 | E1 | 0.402 NIST | 3.500e+05 NIST | – | NIST ASD (accuracy C+) |
| 2[1/2]1 | 2[3/2]°2 | 619.9971 | 619.8256 | 483.5385 | E1 | 0.623 NIST | 6.600e+05 NIST | – | NIST ASD (accuracy B+) |
| 2[1/2]1 | 2[5/2]°2 | 648.9558 | 648.7765 | 461.9613 | E1 | 0.796 NIST | 9.400e+05 NIST | – | NIST ASD (accuracy B) |
| 2[1/2]1 | 2[3/2]°1 | 731.8878 | 731.6862 | 409.6153 | E1 | 0.381 NIST | 2.500e+05 NIST | – | NIST ASD (accuracy C+) |
| 2[1/2]1 | 2[3/2]°2 | 738.8038 | 738.6004 | 405.7809 | E1 | 1.115 NIST | 1.250e+06 NIST | – | NIST ASD (accuracy B+) |
| 2[1/2]°0 | 2[1/2]1 | 764.4127 | 764.2023 | 392.1867 | E1 | 3.727 NIST | 2.100e+07 NIST | – | NIST ASD (accuracy C+) |
| 2[1/2]°1 | 2[1/2]0 | 788.9563 | 788.7393 | 379.9862 | E1 | 2.913 NIST | 3.500e+07 NIST | – | NIST ASD (accuracy C+) |
| 2[1/2]°0 | 2[3/2]1 | 796.9530 | 796.7338 | 376.1733 | E1 | 1.596 NIST | 3.400e+06 NIST | 34 | NIST ASD (accuracy D+) |
| 2[1/2]°0 | 2[3/2]1 | 820.8591 | 820.6335 | 365.2179 | E1 | 4.047 NIST | 2.000e+07 NIST | – | NIST ASD (accuracy C) |
| 2[3/2]°2 | 2[3/2]2 | 823.3897 | 823.1634 | 364.0955 | E1 | 6.277 NIST | 2.860e+07 NIST | – | NIST ASD (accuracy B+) |
| 2[1/2]°1 | 2[1/2]1 | 826.8792 | 826.6520 | 362.5590 | E1 | 3.683 NIST | 1.620e+07 NIST | – | NIST ASD (accuracy C+) |
| 2[3/2]°1 | 2[1/2]0 | 828.2392 | 828.0116 | 361.9636 | E1 | 3.217 NIST | 3.690e+07 NIST | – | NIST ASD (accuracy B) |
| 2[1/2]°1 | 2[3/2]2 | 834.9117 | 834.6823 | 359.0709 | E1 | 7.767 NIST | 4.200e+07 NIST | – | NIST ASD (accuracy C+) |
| 2[3/2]°2 | 2[3/2]1 | 841.1501 | 840.9190 | 356.4078 | E1 | 1.642 NIST | 3.060e+06 NIST | – | NIST ASD (accuracy B+) |
| 2[1/2]°0 | 2[1/2]1 | 852.4885 | 852.2543 | 351.6675 | E1 | 0.550 NIST | 3.300e+05 NIST | – | NIST ASD (accuracy D+) |
| 2[1/2]°1 | 2[1/2]0 | 857.8378 | 857.6022 | 349.4745 | E1 | 1.283 NIST | 5.280e+06 NIST | 45.9 | NIST ASD (accuracy B) |
| 2[1/2]°1 | 2[3/2]1 | 865.0880 | 864.8504 | 346.5456 | E1 | 1.517 NIST | 2.400e+06 NIST | 24 | NIST ASD (accuracy D+) |
| 2[1/2]°1 | 2[3/2]2 | 869.4549 | 869.2162 | 344.8051 | E1 | 1.324 NIST | 1.080e+06 NIST | 11.6 | NIST ASD (accuracy B) |
| 2[3/2]°2 | 2[5/2]3 | 882.1832 | 881.9410 | 339.8302 | E1 | 8.436 NIST | 3.000e+07 NIST | 100 | NIST ASD (accuracy A+) |
| 2[1/2]°1 | 2[3/2]1 | 893.3289 | 893.0837 | 335.5902 | E1 | 4.819 NIST | 2.200e+07 NIST | – | NIST ASD (accuracy C) |
| 2[3/2]°1 | 2[3/2]2 | 895.4709 | 895.2251 | 334.7875 | E1 | 3.789 NIST | 8.100e+06 NIST | – | NIST ASD (accuracy C+) |
| 2[1/2]°1 | 2[5/2]2 | 895.5245 | 895.2787 | 334.7674 | E1 | 1.114 NIST | 7.000e+05 NIST | 11.8 | NIST ASD (accuracy D) |
| 2[3/2]°2 | 2[5/2]2 | 904.7931 | 904.5448 | 331.3381 | E1 | 4.761 NIST | 1.240e+07 NIST | – | NIST ASD (accuracy B+) |
| 2[3/2]°1 | 2[3/2]1 | 916.5168 | 916.2653 | 327.0998 | E1 | 5.231 NIST | 2.400e+07 NIST | – | NIST ASD (accuracy C+) |
| 2[1/2]°1 | 2[1/2]1 | 930.9175 | 930.6622 | 322.0398 | E1 | 2.240 NIST | 4.200e+06 NIST | – | NIST ASD (accuracy D+) |
| 2[3/2]°2 | 2[1/2]1 | 980.2386 | 979.9698 | 305.8362 | E1 | 6.586 NIST | 3.110e+07 NIST | – | NIST ASD (accuracy B+) |
| 2[3/2]°1 | 2[5/2]2 | 992.5911 | 992.3190 | 302.0302 | E1 | 5.601 NIST | 1.300e+07 NIST | – | NIST ASD (accuracy B+) |
| 2[3/2]°1 | 2[1/2]1 | 1084.1297 | 1083.8328 | 276.5282 | E1 | 1.843 NIST | 1.800e+06 NIST | – | NIST ASD (accuracy C+) |
| 2[3/2]°2 | 2[1/2]°0 | 1095.3836 | 1095.0837 | 273.6872 | clock | – | – | – | – |
| 2[1/2]1 | 2[3/2]°1 | 1223.8596 | 1223.5248 | 244.9566 | E1 | 1.942 NIST | 1.390e+06 NIST | – | NIST ASD (accuracy C+) |
| 2[1/2]1 | 2[3/2]°2 | 1262.6849 | 1262.3396 | 237.4246 | E1 | 5.446 NIST | 5.970e+06 NIST | – | NIST ASD (accuracy B+) |
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.
Xe energy levels
Xe⁺ ionisation limit 97833.79 cm⁻¹ = 12.12984 eV (102.214 nm)
Sources
- Allen, Jones, Schofield, J. Opt. Soc. Am. 59, 842 (1969), Table II (read through the publ…
- Anderson, Phys. Rev. 137, A21 (1965) (abstract; read through the publisher page)
- Brandi, Velchev, Hogervorst, Ubachs, Phys. Rev. A 64, 032505 (2001), Table I
- Brandi, Velchev, Hogervorst, Ubachs, Phys. Rev. A 64, 032505 (2001), Table IV
- D'Amico, Pesce, Sasso, Phys. Rev. A 60, 4409 (1999) and Hyperfine Interact. 127, 121 (200…
- Dreissen, Roth, Gruendeman, Krauth, Favier, Eikema, arXiv:2101.07601 (2021)
- Dreissen, Roth, Gruendeman, Krauth, Favier, Eikema, arXiv:2101.07601 (2021) [(2021)] (mea…
- Horiguchi, Chang, Setser, J. Chem. Phys. 75, 1207 (1981) [as tabulated in Doery, Vredenbr…
- Husson et al., 'Mesure de constantes de structure hyperfine de niveaux 6p du xenon et 5p …
- Husson, Grandin, Kucal, J. Physique 40, 551 (1979), Tableau II, p. 554
- Jimenez, Campos, Sanchez del Rio, J. Opt. Soc. Am. 64, 1009 (1974), Table I (read through…
- NIST ASD
- NIST ASD level energies
- Sterr, Bard, Sansonetti, Rolston, Gillaspy, Opt. Lett. 20, 1421 (1995), Table 1 (read thr…
- Sterr, Bard, Sansonetti, Rolston, Gillaspy, Opt. Lett. 20, 1421 (1995), Table 2 (read thr…
- Sterr, Bard, Sansonetti, Rolston, Gillaspy, Opt. Lett. 20, 1421 (1995), abstract and Tabl…
- Suzuki, Katoh, Nishimiya, Spectrochim. Acta A 58, 2519 (2002) [as quoted in Bounds, Kolom…
- Walhout, Sterr, Witte, Rolston, Opt. Lett. 20, 1192 (1995) (abstract, PubMed 19859469). N…
- Walhout, Witte, Rolston, Phys. Rev. Lett. 72, 2843 (1994) (abstract)
Hyperfine entries taken from the comparison table of Bounds et al. are second-hand (method 'compilation', original named in the source); Bounds' own results are listed as alternatives. Isotope-shift keys are kept exactly as printed (pair label 'A-B' with a negative value); see each note on the unverified sign convention. Values converted from mK carry the printed mK numbers alongside. Level energies are NIST ASD values from data/xe/levels.csv; Paschen names in the labels. Entries marked '(abstract)' were read on the publisher's abstract page or HAL record only. Added 2026-10-01 (second pass): VUV isotope shifts of Brandi et al. are printed as nu(136) - nu(A) (positive = lighter isotope at lower frequency); Dreissen et al. print nu(A) - nu(132). 'use_source' / 'use_url' name the paper a use annotation was taken from. Added 2026-10-02 (third pass, papers opened in full): Husson, Grandin, Kucal 1979 (hyperfine constants, printed in mK, converted with 1 mK = 29.9792458 MHz, printed numbers kept in A_mK / B_mK) and Huet et al. 1979 (Lande factors; identical to the NIST ASD values, now with uncertainties). The 4f[3/2]1 and 5f[3/2]1 levels were added for their hyperfine constants only. Added 2026-10-02 (fourth pass, publisher pages read directly): opg.optica.org abstract pages embed the full tables in their HTML and journals.aps.org abstract pages are readable; both were fetched with curl and parsed by script, each Optica table occurs twice in the page (copies compared, identical) a
Atoms with measured data
- Lithium-632 levels, 85 lines
- Lithium-732 levels, 85 lines
- Beryllium-917 levels, 26 lines
- Sodium-2336 levels, 106 lines
- Magnesium-2418 levels, 61 lines
- Magnesium-2518 levels, 61 lines
- Potassium-3934 levels, 84 lines
- Potassium-4034 levels, 84 lines
- Potassium-4134 levels, 84 lines
- Calcium-4035 levels, 61 lines
- Calcium-4335 levels, 61 lines
- Chromium-5256 levels, 87 lines
- Chromium-5356 levels, 87 lines
- Rubidium-8536 levels, 94 lines
- Rubidium-8736 levels, 94 lines
- Strontium-8440 levels, 70 lines
- Strontium-8640 levels, 70 lines
- Strontium-8740 levels, 70 lines
- Strontium-8840 levels, 70 lines
- Cadmium-11115 levels, 21 lines
- Cadmium-11315 levels, 21 lines
- Cadmium-11415 levels, 21 lines
- Caesium-13331 levels, 79 lines
- Barium-13744 levels, 89 lines
- Barium-13844 levels, 89 lines
- Dysprosium-16139 levels, 55 lines
- Dysprosium-16239 levels, 55 lines
- Dysprosium-16339 levels, 55 lines
- Dysprosium-16439 levels, 55 lines
- Erbium-16673 levels, 90 lines
- Erbium-16773 levels, 90 lines
- Erbium-16873 levels, 90 lines
- Thulium-16972 levels, 73 lines
- Ytterbium-17118 levels, 26 lines
- Ytterbium-17318 levels, 26 lines
- Ytterbium-17418 levels, 26 lines
- Mercury-19927 levels, 47 lines
- Mercury-20127 levels, 47 lines
- Mercury-20227 levels, 47 lines