Chlorine energy level diagram
Energy levels and transitions of neutral chlorine (Cl I): the 79 strongest classified lines below 2 µm from the NIST Atomic Spectra Database and the 43 levels they connect, each line with its vacuum wavelength, frequency and, for 77 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 chlorine
| Transition | λ vac (nm) | λ air (nm) | ν (THz) | |⟨J‖er‖J′⟩| (ea₀) | A (s⁻¹) | Γ/2π up. (MHz) | branch (%) | Use |
|---|---|---|---|---|---|---|---|---|
| 3p5 2P°3/2 – 3p44s 2S1/2 | 100.4678 | – | 2983.9668 | 0.791 | 6.250e+08 | 153 | 65 | interstellar Cl I 1005 A absorption line |
| 3p5 2P°3/2 – 3p45s 2[0]1/2 | 107.9882 | – | 2776.1591 | 0.259 | 5.380e+07 | 27.3 | 31.4 | interstellar Cl I 1080 A absorption line |
| 3p5 2P°3/2 – 3p43d 2F5/2 | 108.8059 | – | 2755.2962 | ≈0.573 | 8.604e+07 | 48.23 | 28.4 | interstellar Cl I 1088 A line |
| 3p5 2P°3/2 – 3p45s 2[2]3/2 | 109.0739 | – | 2748.5269 | 0.369 | 5.330e+07 | 17.72 | 47.9 | interstellar Cl I 1091 A absorption line |
| 3p5 2P°3/2 – 3p45s 2[2]5/2 | 109.4769 | – | 2738.4092 | 0.745 | 1.430e+08 | 25.34 | 89.8 | interstellar Cl I 1095 A absorption line |
| 3p5 2P°3/2 – 3p43d 2D5/2 | 109.7369 | – | 2731.9196 | ≈1.250 | 3.993e+08 | 5.184 | 100 | interstellar Cl I 1097 A line |
| 3p5 2P°3/2 – 3p44p 4S°3/2 | 116.6384 | – | 2570.2734 | – | – | – | – | two-photon LIF |
| 3p5 2P°1/2 – 3p44p 4S°3/2 | 117.8512 | – | 2543.8211 | – | – | – | – | TALIF detection of spin-orbit excited Cl |
| 3p5 2P°3/2 – 3p44s 2D3/2 | 118.8751 | – | 2521.9103 | 0.300 | 2.710e+07 | – | – | VUV resonance line of the 3p5 - 3p4 4s array |
| 3p5 2P°3/2 – 3p44s 2D5/2 | 118.8774 | – | 2521.8620 | 1.077 | 2.330e+08 | – | – | VUV resonance line of the 3p5 - 3p4 4s array |
| 3p5 2P°1/2 – 3p44s 2D3/2 | 120.1352 | – | 2495.4581 | 0.899 | 2.360e+08 | – | – | VUV resonance line of the 3p5 - 3p4 4s array |
| 3p5 2P°3/2 – 3p44s 2P1/2 | 133.5726 | – | 2244.4162 | 0.640 | 1.740e+08 | 79.58 | 34.8 | VUV resonance line of the 3p5 - 3p4 4s array |
| 3p5 2P°3/2 – 3p44s 2P3/2 | 134.7240 | – | 2225.2349 | 1.422 | 4.190e+08 | 105.4 | 85.2 | 134.72 nm VUV resonance line |
| 3p5 2P°1/2 – 3p44s 2P1/2 | 135.1656 | – | 2217.9640 | 0.887 | 3.230e+08 | 79.58 | 64.6 | VUV resonance line of the 3p5 - 3p4 4s array |
| 3p5 2P°1/2 – 3p44s 2P3/2 | 136.3447 | – | 2198.7827 | 0.613 | 7.500e+07 | 105.4 | 14.8 | 136.34 nm VUV line from the metastable 2P1/2 level |
| 3p5 2P°3/2 – 3p44s 4P1/2 | 137.3116 | – | 2183.2997 | ≈0.038 | 5.698e+05 | – | – | VUV resonance line of the 3p5 - 3p4 4s array |
| 3p5 2P°3/2 – 3p44s 4P3/2 | 137.9528 | – | 2173.1526 | 0.239 | 1.100e+07 | – | – | VUV resonance line of the 3p5 - 3p4 4s array |
| 3p5 2P°3/2 – 3p44s 4P5/2 | 138.9693 | – | 2157.2575 | 0.043 | 2.300e+05 | 0.1061 | 34.5 | VUV resonance line of the 3p5 - 3p4 4s array |
| 3p44s 4P5/2 – 3p44p 4S°3/2 | 725.8618 | 725.6618 | 413.0159 | 3.365 | 1.500e+07 | – | – | 725.9 nm |
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).
35Cl hyperfine structure (I = 3/2)
| Level | A (MHz) | B (MHz) | Shift of each F level from the centre of gravity (MHz) |
|---|---|---|---|
| 3p5 2P°3/2 | 205.04687(3) | 54.87290(6) | F=0: -700.34 F=1: -550.16 F=2: -194.94 F=3: +475.07 |
| 3p5 2P°1/2 | 1037.209(14) | – | F=1: -1296.51 F=2: +777.91 |
Measured A, B constants; sources in the data file.
Closed and nearly closed transitions of chlorine
| Transition | λ vacuum (nm) | Lower level | A (s⁻¹) | Leak per scattered photon | Photons before a leak | Where the leak goes |
|---|---|---|---|---|---|---|
| 3p5 2P°3/2 → 3p44s 4P5/2 | 138.9693 | ground | 2.300e+05 NIST | closed | – | no other level can be reached by electric-dipole decay |
| 3p5 2P°3/2 → 3p44s 2D5/2 | 118.8774 | ground | 2.330e+08 NIST | 7.13 × 10−8 from semi-empirical calc. | 1.4 × 107 | 3p44p 4P°3/2 ≈ 5 × 10−8; 3p44p 4P°5/2 ≈ 2.11 × 10−8; 3p44p 4D°7/2 ≈ 1.53 × 10−10 |
| 3p5 2P°3/2 → 3p43d 2F5/2 | 108.8059 | ground | 8.604e+07 semi-empirical | 5.67 % from semi-empirical calc. | 18 | 3p44p 2D°3/2 ≈ 1.9 %; 3p44p 4S°3/2 ≈ 1.21 %; 3p44p 2P°3/2 ≈ 1.15 %; 6 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 Cl 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 |
|---|---|---|---|---|---|---|---|---|---|
| 3p5 2P°3/2 | 3p44s 2S1/2 | 100.4678 | – | 2983.9668 | E1 | 0.791 measured | 6.250e+08 measured | 65 | Alkhayat, Irving, Federman, Ellis, Cheng, Lifetimes and Oscillator Strengths for Ultravio… |
| 3p5 2P°3/2 | 3p45s 2[0]1/2 | 107.9882 | – | 2776.1591 | E1 | 0.259 measured | 5.380e+07 measured | 31.4 | Alkhayat, Irving, Federman, Ellis, Cheng, Lifetimes and Oscillator Strengths for Ultravio… |
| 3p5 2P°3/2 | 3p43d 2F5/2 | 108.8059 | – | 2755.2962 | E1 | 0.573 semi-empirical | 8.604e+07 semi-empirical | 28.4 | Kurucz, R. L., Can. J. Phys. 89, 417 (2011); semi-empirical line list gf1700.pos of 2013-… |
| 3p5 2P°3/2 | 3p45s 2[2]3/2 | 109.0739 | – | 2748.5269 | E1 | 0.369 measured | 5.330e+07 measured | 47.9 | Alkhayat, Irving, Federman, Ellis, Cheng, Lifetimes and Oscillator Strengths for Ultravio… |
| 3p5 2P°3/2 | 3p45s 2[2]5/2 | 109.4769 | – | 2738.4092 | E1 | 0.745 measured | 1.430e+08 measured | 89.8 | Alkhayat, Irving, Federman, Ellis, Cheng, Lifetimes and Oscillator Strengths for Ultravio… |
| 3p5 2P°3/2 | 3p43d 2D5/2 | 109.7369 | – | 2731.9196 | E1 | 1.250 semi-empirical | 3.993e+08 semi-empirical | 100 | Kurucz, R. L., Can. J. Phys. 89, 417 (2011); semi-empirical line list gf1700.pos of 2013-… |
| 3p5 2P°3/2 | 3p44p 4S°3/2 | 116.6384 | – | 2570.2734 | two-photon | – | – | – | – |
| 3p5 2P°1/2 | 3p44p 4S°3/2 | 117.8512 | – | 2543.8211 | two-photon | – | – | – | – |
| 3p5 2P°3/2 | 3p44s 2D3/2 | 118.8751 | – | 2521.9103 | E1 | 0.300 NIST | 2.710e+07 NIST | – | NIST ASD (accuracy C) |
| 3p5 2P°3/2 | 3p44s 2D5/2 | 118.8774 | – | 2521.8620 | E1 | 1.077 NIST | 2.330e+08 NIST | – | NIST ASD (accuracy C) |
| 3p5 2P°1/2 | 3p44s 2D3/2 | 120.1352 | – | 2495.4581 | E1 | 0.899 measured | 2.360e+08 measured | – | Schwab and Anderson (1982), absorption technique; Table 3 of Biemont, Gebarowski, Zeippen… |
| 3p5 2P°3/2 | 3p44s 2P1/2 | 133.5726 | – | 2244.4162 | E1 | 0.640 NIST | 1.740e+08 NIST | 34.8 | NIST ASD (accuracy C) |
| 3p5 2P°3/2 | 3p44s 2P3/2 | 134.7240 | – | 2225.2349 | E1 | 1.422 NIST | 4.190e+08 NIST | 85.2 | NIST ASD (accuracy C+) |
| 3p5 2P°1/2 | 3p44s 2P1/2 | 135.1656 | – | 2217.9640 | E1 | 0.887 NIST | 3.230e+08 NIST | 64.6 | NIST ASD (accuracy C+) |
| 3p5 2P°1/2 | 3p44s 2P3/2 | 136.3447 | – | 2198.7827 | E1 | 0.613 NIST | 7.500e+07 NIST | 14.8 | NIST ASD (accuracy C+) |
| 3p5 2P°3/2 | 3p44s 4P1/2 | 137.3116 | – | 2183.2997 | E1 (intercombination) | 0.0382 semi-empirical | 5.698e+05 semi-empirical | – | Kurucz, R. L., Can. J. Phys. 89, 417 (2011); semi-empirical line list gf1700.pos of 2013-… |
| 3p5 2P°3/2 | 3p44s 4P3/2 | 137.9528 | – | 2173.1526 | E1 (intercombination) | 0.239 NIST | 1.100e+07 NIST | – | NIST ASD (accuracy D) |
| 3p5 2P°3/2 | 3p44s 4P5/2 | 138.9693 | – | 2157.2575 | E1 (intercombination) | 0.0428 NIST | 2.300e+05 NIST | 34.5 | NIST ASD (accuracy D) |
| 3p5 2P°1/2 | 3p44s 4P1/2 | 138.9957 | – | 2156.8474 | E1 (intercombination) | 0.0671 NIST | 1.700e+06 NIST | – | NIST ASD (accuracy D) |
| 3p5 2P°1/2 | 3p44s 4P3/2 | 139.6527 | – | 2146.7004 | E1 (intercombination) | 0.0898 NIST | 1.500e+06 NIST | – | NIST ASD (accuracy D) |
| 3p44s 4P5/2 | 3p45p 2P°3/2 | 410.5939 | 410.4780 | 730.1435 | E1 (intercombination) | 0.165 NIST | 2.000e+05 NIST | – | NIST ASD (accuracy D) |
| 3p44s 4P3/2 | 3p45p 2P°1/2 | 414.8426 | 414.7256 | 722.6656 | E1 (intercombination) | 0.164 NIST | 3.800e+05 NIST | – | NIST ASD (accuracy D) |
| 3p44s 4P5/2 | 3p45p 2D°3/2 | 421.0851 | 420.9665 | 711.9523 | E1 (intercombination) | 0.246 NIST | 4.100e+05 NIST | – | NIST ASD (accuracy D+) |
| 3p44s 4P5/2 | 3p45p 4S°3/2 | 422.7616 | 422.6426 | 709.1289 | E1 | 0.286 NIST | 5.500e+05 NIST | – | NIST ASD (accuracy D+) |
| 3p44s 4P5/2 | 3p45p 4D°5/2 | 426.5781 | 426.4580 | 702.7845 | E1 | 0.198 NIST | 1.700e+05 NIST | – | NIST ASD (accuracy D+) |
| 3p44s 4P3/2 | 3p45p 4S°3/2 | 432.4551 | 432.3335 | 693.2337 | E1 | 0.419 NIST | 1.100e+06 NIST | – | NIST ASD (accuracy D+) |
| 3p44s 4P3/2 | 3p45p 4D°5/2 | 436.4494 | 436.3268 | 686.8894 | E1 | 0.409 NIST | 6.800e+05 NIST | – | NIST ASD (accuracy D) |
| 3p44s 4P1/2 | 3p45p 2D°3/2 | 437.0726 | 436.9498 | 685.9100 | E1 (intercombination) | 0.340 NIST | 7.000e+05 NIST | – | NIST ASD (accuracy D+) |
| 3p44s 4P5/2 | 3p45p 2D°5/2 | 437.2772 | 437.1544 | 685.5890 | E1 (intercombination) | 0.193 NIST | 1.500e+05 NIST | – | NIST ASD (accuracy D+) |
| 3p44s 4P3/2 | 3p45p 4D°3/2 | 438.1126 | 437.9896 | 684.2817 | E1 | 0.482 NIST | 1.400e+06 NIST | – | NIST ASD (accuracy D) |
| 3p44s 4P1/2 | 3p45p 4S°3/2 | 438.8791 | 438.7558 | 683.0867 | E1 | 0.245 NIST | 3.600e+05 NIST | – | NIST ASD (accuracy D+) |
| 3p44s 4P5/2 | 3p45p 4D°7/2 | 439.0984 | 438.9751 | 682.7455 | E1 | 0.684 NIST | 1.400e+06 NIST | – | NIST ASD (accuracy D) |
| 3p44s 4P1/2 | 3p45p 4D°1/2 | 439.1636 | 439.0403 | 682.6441 | E1 | 0.257 NIST | 7.900e+05 NIST | – | NIST ASD (accuracy D+) |
| 3p44s 4P1/2 | 3p45p 2S°1/2 | 440.3757 | 440.2520 | 680.7653 | E1 (intercombination) | 0.221 NIST | 5.800e+05 NIST | – | NIST ASD (accuracy D+) |
| 3p44s 4P5/2 | 3p45p 4P°3/2 | 440.4257 | 440.3020 | 680.6880 | E1 | 0.353 NIST | 7.400e+05 NIST | – | NIST ASD (accuracy D) |
| 3p44s 4P5/2 | 3p45p 4P°5/2 | 443.9734 | 443.8488 | 675.2487 | E1 | 0.602 NIST | 1.400e+06 NIST | – | NIST ASD (accuracy D) |
| 3p44s 4P1/2 | 3p45p 4D°3/2 | 444.7071 | 444.5823 | 674.1346 | E1 | 0.200 NIST | 2.300e+05 NIST | – | NIST ASD (accuracy D) |
| 3p44s 4P3/2 | 3p45p 4P°1/2 | 444.7387 | 444.6138 | 674.0868 | E1 | 0.196 NIST | 4.400e+05 NIST | – | NIST ASD (accuracy D) |
| 3p44s 2P3/2 | 3p45p 2P°1/2 | 447.0622 | 446.9368 | 670.5833 | E1 | 0.376 NIST | 1.600e+06 NIST | – | NIST ASD (accuracy D) |
| 3p44s 4P3/2 | 3p45p 2D°5/2 | 447.6560 | 447.5304 | 669.6938 | E1 (intercombination) | 0.338 NIST | 4.300e+05 NIST | – | NIST ASD (accuracy D+) |
| 3p44s 2P3/2 | 3p44p 2D°3/2 | 449.2292 | 449.1032 | 667.3486 | E1 | 0.293 NIST | 4.800e+05 NIST | – | NIST ASD (accuracy D+) |
| 3p44s 2P3/2 | 3p45p 2P°3/2 | 452.7451 | 452.6182 | 662.1661 | E1 | 0.967 NIST | 5.100e+06 NIST | – | NIST ASD (accuracy C) |
| 3p44s 2P3/2 | 3p45p 2D°3/2 | 465.5344 | 465.4041 | 643.9748 | E1 | 0.312 NIST | 4.900e+05 NIST | – | NIST ASD (accuracy D+) |
| 3p44s 2P3/2 | 3p45p 4S°3/2 | 467.5845 | 467.4536 | 641.1515 | E1 (intercombination) | 0.201 NIST | 2.000e+05 NIST | – | NIST ASD (accuracy D+) |
| 3p44s 2P3/2 | 3p45p 4D°1/2 | 467.9075 | 467.7765 | 640.7089 | E1 (intercombination) | 0.234 NIST | 5.400e+05 NIST | – | NIST ASD (accuracy D+) |
| 3p44s 2P3/2 | 3p45p 2S°1/2 | 469.2836 | 469.1523 | 638.8301 | E1 | 0.335 NIST | 1.100e+06 NIST | – | NIST ASD (accuracy D+) |
| 3p44s 2P3/2 | 3p45p 4D°5/2 | 472.2576 | 472.1255 | 634.8071 | E1 (intercombination) | 0.256 NIST | 2.100e+05 NIST | – | NIST ASD (accuracy D+) |
| 3p44s 2P3/2 | 3p45p 4D°3/2 | 474.2055 | 474.0729 | 632.1994 | E1 (intercombination) | 0.297 NIST | 4.200e+05 NIST | – | NIST ASD (accuracy D+) |
| 3p44s 2P3/2 | 3p45p 4P°1/2 | 481.9780 | 481.8433 | 622.0045 | E1 (intercombination) | 0.208 NIST | 3.900e+05 NIST | – | NIST ASD (accuracy D) |
| 3p44s 2P3/2 | 3p45p 2D°5/2 | 485.4062 | 485.2706 | 617.6116 | E1 | 0.279 NIST | 2.300e+05 NIST | – | NIST ASD (accuracy D+) |
| 3p44s 2P3/2 | 3p44p 2P°3/2 | 497.8007 | 497.6619 | 602.2339 | E1 | 0.292 NIST | 3.500e+05 NIST | – | NIST ASD (accuracy D+) |
| 3p44s 4P5/2 | 3p44p 4S°3/2 | 725.8618 | 725.6618 | 413.0159 | E1 | 3.365 NIST | 1.500e+07 NIST | – | NIST ASD (accuracy D) |
| 3p44s 4P5/2 | 3p44p 2P°3/2 | 741.6160 | 741.4118 | 404.2422 | E1 (intercombination) | 1.945 NIST | 4.700e+06 NIST | – | NIST ASD (accuracy D) |
| 3p44s 4P3/2 | 3p44p 4S°3/2 | 754.9151 | 754.7073 | 397.1208 | E1 | 3.193 NIST | 1.200e+07 NIST | – | NIST ASD (accuracy D) |
| 3p44s 4P3/2 | 3p44p 2P°3/2 | 771.9706 | 771.7581 | 388.3470 | E1 (intercombination) | 1.651 NIST | 3.000e+06 NIST | – | NIST ASD (accuracy D) |
| 3p44s 4P1/2 | 3p44p 4S°3/2 | 774.7102 | 774.4970 | 386.9737 | E1 | 2.405 NIST | 6.300e+06 NIST | – | NIST ASD (accuracy C) |
| 3p44s 4P5/2 | 3p44p 2D°5/2 | 788.0384 | 787.8216 | 380.4287 | E1 (intercombination) | 1.615 NIST | 1.800e+06 NIST | – | NIST ASD (accuracy D) |
| 3p44s 4P1/2 | 3p44p 2P°3/2 | 792.6825 | 792.4645 | 378.1999 | E1 (intercombination) | 1.437 NIST | 2.100e+06 NIST | – | NIST ASD (accuracy D) |
| 3p44s 4P5/2 | 3p44p 4D°3/2 | 798.2792 | 798.0597 | 375.5484 | E1 | 1.268 NIST | 1.600e+06 NIST | – | NIST ASD (accuracy E) |
| 3p44s 4P3/2 | 3p44p 2D°3/2 | 800.0056 | 799.7857 | 374.7379 | E1 (intercombination) | 1.457 NIST | 2.100e+06 NIST | – | NIST ASD (accuracy D) |
| 3p44s 4P3/2 | 3p44p 4D°1/2 | 819.6675 | 819.4422 | 365.7489 | E1 | 1.649 NIST | 5.000e+06 NIST | – | NIST ASD (accuracy E) |
| 3p44s 4P5/2 | 3p44p 4D°5/2 | 821.4295 | 821.2038 | 364.9643 | E1 | 3.601 NIST | 7.900e+06 NIST | – | NIST ASD (accuracy D) |
| 3p44s 4P3/2 | 3p44p 4D°3/2 | 833.5597 | 833.3307 | 359.6533 | E1 | 4.277 NIST | 1.600e+07 NIST | – | NIST ASD (accuracy D) |
| 3p44s 4P5/2 | 3p44p 4D°7/2 | 837.8245 | 837.5943 | 357.8225 | E1 | 8.063 NIST | 2.800e+07 NIST | – | NIST ASD (accuracy D) |
| 3p44s 4P1/2 | 3p44p 4D°1/2 | 843.0567 | 842.8250 | 355.6018 | E1 | 3.768 NIST | 2.400e+07 NIST | – | NIST ASD (accuracy D) |
| 3p44s 2P3/2 | 3p44p 2S°1/2 | 855.2790 | 855.0441 | 350.5201 | E1 | 1.083 NIST | 1.900e+06 NIST | – | NIST ASD (accuracy D) |
| 3p44s 4P1/2 | 3p44p 4D°3/2 | 857.7601 | 857.5245 | 349.5062 | E1 | 3.867 NIST | 1.200e+07 NIST | – | NIST ASD (accuracy D) |
| 3p44s 4P3/2 | 3p44p 4D°5/2 | 858.8340 | 858.5981 | 349.0692 | E1 | 5.970 NIST | 1.900e+07 NIST | – | NIST ASD (accuracy D) |
| 3p44s 2P3/2 | 3p44p 4S°3/2 | 868.8667 | 868.6281 | 345.0385 | E1 (intercombination) | 2.247 NIST | 3.900e+06 NIST | – | NIST ASD (accuracy D) |
| 3p44s 4P5/2 | 3p44p 4P°3/2 | 895.0519 | 894.8062 | 334.9442 | E1 | 4.122 NIST | 1.200e+07 NIST | – | NIST ASD (accuracy D) |
| 3p44s 2P3/2 | 3p44p 2P°1/2 | 907.5659 | 907.3168 | 330.3258 | E1 | 3.744 NIST | 1.900e+07 NIST | – | NIST ASD (accuracy D) |
| 3p44s 4P5/2 | 3p44p 4P°5/2 | 912.3646 | 912.1143 | 328.5884 | E1 | 6.183 NIST | 1.700e+07 NIST | – | NIST ASD (accuracy D) |
| 3p44s 4P3/2 | 3p44p 4P°1/2 | 919.4253 | 919.1731 | 326.0650 | E1 | 4.014 NIST | 2.100e+07 NIST | – | NIST ASD (accuracy D) |
| 3p44s 2P3/2 | 3p44p 2D°3/2 | 929.1406 | 928.8857 | 322.6556 | E1 | 2.640 NIST | 4.400e+06 NIST | – | NIST ASD (accuracy E) |
| 3p44s 4P3/2 | 3p44p 4P°3/2 | 939.6437 | 939.3859 | 319.0491 | E1 | 2.253 NIST | 3.100e+06 NIST | – | NIST ASD (accuracy E) |
| 3p44s 4P1/2 | 3p44p 4P°1/2 | 948.9567 | 948.6964 | 315.9180 | E1 | 1.814 NIST | 3.900e+06 NIST | – | NIST ASD (accuracy E) |
| 3p44s 4P3/2 | 3p44p 4P°5/2 | 958.7429 | 958.4800 | 312.6933 | E1 | 4.150 NIST | 6.600e+06 NIST | – | NIST ASD (accuracy D) |
| 3p44s 2P3/2 | 3p44p 2D°5/2 | 959.4853 | 959.2222 | 312.4513 | E1 | 7.923 NIST | 2.400e+07 NIST | – | NIST ASD (accuracy D) |
| 3p44s 4P1/2 | 3p44p 4P°3/2 | 970.5099 | 970.2438 | 308.9020 | E1 | 4.052 NIST | 9.100e+06 NIST | – | NIST ASD (accuracy D) |
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.
Cl energy levels
| Level | Energy (cm⁻¹) | J | Parity | Lifetime | gJ | Hyperfine A (MHz) | Hyperfine B (MHz) | Lifetime source | Hyperfine source |
|---|---|---|---|---|---|---|---|---|---|
| 3p5 2P°3/2 | 0.000 | 3/2 | odd | stable | 1.3339 | 205.047 | 54.8729 | – | atomic-beam magnetic resonance: Davis, Feld, Zabel, Zacharias, Phys. Rev. 76, 1076 (1949)… |
| 3p5 2P°1/2 | 882.351 | 1/2 | odd | 87.9 s measured | 0.66566 | 1037.21 | – | A. C. Stanton, Chem. Phys. Lett. 122, 385 (1985) (diode-laser absorption); experimental c… | Holloway, Aubrey, King, Proc. Phys. Soc. 76, 984 (1960); King & Jaccarino, Phys. Rev. 84,… |
| 3p44s 4P5/2 | 71958.363 | 5/2 | even | 1.5 µs measured | 1.599 | – | – | G. M. Lawrence, Astrophys. J. 148, 261 (1967), Table 7 (phase-shift method, stated accura… | – |
| 3p44s 4P3/2 | 72488.568 | 3/2 | even | – | 1.722 | – | – | – | – |
| 3p44s 4P1/2 | 72827.038 | 1/2 | even | – | 2.652 | – | – | – | – |
| 3p44s 2P3/2 | 74225.846 | 3/2 | even | 1.51 ns measured | 1.34 | – | – | Schectman, Federman, Beideck, Ellis, Astrophys. J. 406, 735 (1993) (beam-foil) | – |
| 3p44s 2P1/2 | 74865.667 | 1/2 | even | 2 ns measured | 0.663 | – | – | G. M. Lawrence, Astrophys. J. 148, 261 (1967), Table 7 (phase-shift method, stated accura… | – |
| 3p44p 4P°5/2 | 82918.893 | 5/2 | odd | – | 1.591 | – | – | – | – |
| 3p44p 4P°3/2 | 83130.900 | 3/2 | odd | – | 1.723 | – | – | – | – |
| 3p44p 4P°1/2 | 83364.927 | 1/2 | odd | – | 2.617 | – | – | – | – |
| 3p44p 4D°7/2 | 83894.037 | 7/2 | odd | – | 1.422 | – | – | – | – |
| 3p44s 2D5/2 | 84120.263 | 5/2 | even | – | – | – | – | – | – |
| 3p44s 2D3/2 | 84121.872 | 3/2 | even | – | – | – | – | – | – |
| 3p44p 4D°5/2 | 84132.262 | 5/2 | odd | – | 1.308 | – | – | – | – |
| 3p44p 4D°3/2 | 84485.309 | 3/2 | odd | – | 1.163 | – | – | – | – |
| 3p44p 2D°5/2 | 84648.100 | 5/2 | odd | – | 1.269 | – | – | – | – |
| 3p44p 4D°1/2 | 84688.637 | 1/2 | odd | – | 0.059 | – | – | – | – |
| 3p44p 2D°3/2 | 84988.480 | 3/2 | odd | – | 0.986 | – | – | – | – |
| 3p44p 2P°1/2 | 85244.330 | 1/2 | odd | – | 1.28 | – | – | – | – |
| 3p44p 2P°3/2 | 85442.430 | 3/2 | odd | – | 1.327 | – | – | – | – |
| 3p44p 4S°3/2 | 85735.091 | 3/2 | odd | – | 1.877 | – | – | – | – |
| 3p44p 2S°1/2 | 85917.937 | 1/2 | odd | – | 1.379 | – | – | – | – |
| 3p43d 2D5/2 | 91127.030 | 5/2 | even | 30.7 ns measured | – | – | – | Schectman, Federman, Beideck, Ellis, Astrophys. J. 406, 735 (1993) (beam-foil). Note: der… | – |
| 3p45s 2[2]5/2 | 91343.500 | 5/2 | even | 6.28 ns measured | – | – | – | Alkhayat, Irving, Federman, Ellis, Cheng, Lifetimes and Oscillator Strengths for Ultravio… | – |
| 3p45s 2[2]3/2 | 91680.990 | 3/2 | even | 8.98 ns measured | – | – | – | Alkhayat, Irving, Federman, Ellis, Cheng, Lifetimes and Oscillator Strengths for Ultravio… | – |
| 3p43d 2F5/2 | 91906.790 | 5/2 | even | 3.3 ns measured | – | – | – | Schectman, Federman, Beideck, Ellis, Astrophys. J. 406, 735 (1993) (beam-foil) | – |
| 3p45s 2[0]1/2 | 92602.700 | 1/2 | even | 5.83 ns measured | – | – | – | Alkhayat, Irving, Federman, Ellis, Cheng, Lifetimes and Oscillator Strengths for Ultravio… | – |
| 3p44p 2P°3/2 | 94314.206 | 3/2 | odd | – | 1.328 | – | – | – | – |
| 3p45p 4P°5/2 | 94482.236 | 5/2 | odd | – | 1.559 | – | – | – | – |
| 3p45p 4P°3/2 | 94663.670 | 3/2 | odd | – | 1.722 | – | – | – | – |
| 3p45p 4D°7/2 | 94732.300 | 7/2 | odd | – | 1.42 | – | – | – | – |
| 3p45p 2D°5/2 | 94827.150 | 5/2 | odd | – | 1.247 | – | – | – | – |
| 3p45p 4P°1/2 | 94973.683 | 1/2 | odd | – | 2.309 | – | – | – | – |
| 3p45p 4D°3/2 | 95313.749 | 3/2 | odd | – | 1.147 | – | – | – | – |
| 3p45p 4D°5/2 | 95400.731 | 5/2 | odd | – | 1.352 | – | – | – | – |
| 3p45p 2S°1/2 | 95534.923 | 1/2 | odd | – | 1.409 | – | – | – | – |
| 3p45p 4D°1/2 | 95597.593 | 1/2 | odd | – | 0.699 | – | – | – | – |
| 3p45p 4S°3/2 | 95612.357 | 3/2 | odd | – | 1.531 | – | – | – | – |
| 3p45p 2D°3/2 | 95706.534 | 3/2 | odd | – | 1.321 | – | – | – | – |
| 3p45p 2P°3/2 | 96313.330 | 3/2 | odd | – | 1.2873 | – | – | – | – |
| 3p44p 2D°3/2 | 96486.198 | 3/2 | odd | – | 0.867 | – | – | – | – |
| 3p45p 2P°1/2 | 96594.096 | 1/2 | odd | – | 0.712 | – | – | – | – |
| 3p44s 2S1/2 | 99534.419 | 1/2 | even | 1.04 ns measured | 1.99 | – | – | Alkhayat, Irving, Federman, Ellis, Cheng, Lifetimes and Oscillator Strengths for Ultravio… | – |
Cl⁺ ionisation limit 104591.01 cm⁻¹ = 12.96763 eV (95.611 nm)
Sources
- A. C. Stanton, Chem. Phys. Lett. 122, 385 (1985) (diode-laser absorption); experimental c…
- Alkhayat, Irving, Federman, Ellis, Cheng, Lifetimes and Oscillator Strengths for Ultravio…
- Alkhayat, Irving, Federman, Ellis, Cheng, Lifetimes and Oscillator Strengths for Ultravio…
- G. M. Lawrence, Astrophys. J. 148, 261 (1967), Table 7 (phase-shift method, stated accura…
- G. M. Lawrence, Astrophys. J. 148, 261 (1967), Table 7 (phase-shift method, stated accura…
- Holloway, Aubrey, King, Proc. Phys. Soc. 76, 984 (1960); King & Jaccarino, Phys. Rev. 84,…
- Kurucz, R. L., Can. J. Phys. 89, 417 (2011); semi-empirical line list gf1700.pos of 2013-…
- NIST ASD
- NIST ASD level energies
- Schectman, Federman, Beideck, Ellis, Astrophys. J. 406, 735 (1993) (beam-foil)
- Schectman, Federman, Beideck, Ellis, Astrophys. J. 406, 735 (1993) (beam-foil). Note: der…
- Schwab and Anderson (1982), absorption technique; Table 3 of Biemont, Gebarowski, Zeippen…
- atomic-beam magnetic resonance: Davis, Feld, Zabel, Zacharias, Phys. Rev. 76, 1076 (1949)…
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 (APS, IOP, Elsevier, Canadian Science Publishing full texts were not accessible). Hyperfine constants of the ground term are second-hand from Chichinin's JPCRD review (method 'compilation'). Signs: A, B as printed (Casimir convention, E = A*C/2 + B*[...]). The M1 A value is the calculated one adopted by NIST. Values marked 'derived' were computed here from the quoted measured numbers. Two-photon entries: wavelength_vac_nm is the laser wavelength (two photons of that wavelength reach the upper level). Second pass (2026-10-01): beam-foil lifetimes of four more levels from arXiv:1910.05803; second-hand measured oscillator strengths of the 3p5 - 4s resonance lines read on the scanned Table 3 of Biemont et al. 1994 (NASA ADS; the image was checked by eye) and converted to A here (derived, method compilation). Lawrence-1967 entries in that table are listed only as alternatives because all but two of them come from an intermediate-coupling analysis of his lifetime measurements. Lines to 4s 4P levels are typed "intercombination".
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