Atomic energy level diagrams

Titanium energy level diagram

Energy levels and transitions of neutral titanium (Ti I): the 88 strongest classified lines below 2 µm from the NIST Atomic Spectra Database and the 74 levels they connect, each line with its vacuum wavelength, frequency and, for 88 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.

Titanium energy level diagram with transition wavelengths and dipole matrix elements

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

Key transitions of titanium

Transitionλ vac (nm)λ air (nm)ν (THz)|⟨J‖er‖J′⟩| (ea₀)A (s⁻¹)Γ/2π up. (MHz)branch (%)Use
a 3F4 – 5D°4391.5443391.4334765.66680.7832.300e+06––optical pumping a3F4 -> y5D4 -> a5F5
a 3F4 – y 3F°4399.9767399.8636749.52483.7094.840e+078.69788.6400 nm
a 5F5 – y 5G°6498.3120498.1730601.61597.8697.800e+0712.43100broad laser-cooling line of metastable Ti
a 5F4 – y 5G°5499.2458499.1066600.49066.8276.900e+0712.2489.7a5F4 - y5G5 line of the laser-cooling multiplet
a 5F3 – y 5G°4500.0898499.9503599.47735.8696.200e+0712.1581.2a5F3 - y5G4 line of the laser-cooling multiplet
a 5F2 – y 5G°3500.8606500.7209598.55474.9575.660e+0711.9775.3a5F2 - y5G3 line of the laser-cooling multiplet
a 5F1 – y 5G°2501.5675501.4276597.71114.2355.760e+0711.8877.2a5F1 - y5G2 line of the laser-cooling multiplet
a 5F5 – y 5G°5501.7560501.6161597.48652.3287.900e+0612.2410.3a5F5 - y5G5 line of the laser-cooling multiplet
a 5F4 – y 5G°4502.1426502.0026597.02652.7861.380e+0712.1518.1a5F4 - y5G4 line of the laser-cooling multiplet
a 5F3 – y 5G°3502.4269502.2868596.68872.7771.760e+0711.9723.4a5F3 - y5G3 line of the laser-cooling multiplet
a 5F2 – y 5G°2502.6246502.4844596.45402.2181.570e+0711.8821a5F2 - y5G2 line of the laser-cooling multiplet
a 5F5 – 5D°4524.0044523.8586572.11820.506*4.000e+05––decay channel y5D4 -> a5F5
a 5F5 – z 5G°61039.96491039.6800288.27170.9381.220e+050.01941100narrow laser-cooling 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).

47Ti hyperfine structure (I = 5/2)

LevelA (MHz)B (MHz)Shift of each F level from the centre of gravity (MHz)
a 3F3-52.9047(7)28.082(9)F=1/2: +545.90 F=3/2: +458.96 F=5/2: +316.87 F=7/2: +123.84 F=9/2: -114.23 F=11/2: -389.76
a 3F4-37.9918(6)37.681(10)F=3/2: +493.40 F=5/2: +387.32 F=7/2: +243.04 F=9/2: +64.81 F=11/2: -141.92 F=13/2: -370.50
a 5F5-74.8450(25)-28.67(5)F=5/2: +1110.25 F=7/2: +856.99 F=9/2: +527.93 F=11/2: +120.49 F=13/2: -368.49 F=15/2: -942.73
z 5G°6-85(9)77(5)F=7/2: +1518.12 F=9/2: +1112.00 F=11/2: +625.25 F=13/2: +63.65 F=15/2: -565.98 F=17/2: -1255.75
5D°4-96.60(20)-0(3)F=3/2: +1207.38 F=5/2: +965.95 F=7/2: +627.92 F=9/2: +193.27 F=11/2: -338.04 F=13/2: -966.06
y 5G°6-14.2(3)-1(7)F=7/2: +248.06 F=9/2: +184.50 F=11/2: +106.67 F=13/2: +14.51 F=15/2: -92.11 F=17/2: -213.28

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

Isotope shifts

Transitionλ vac (nm)IsotopesShift (MHz)
a 3F4 – 5D°4391.54446-48-943(3)
a 3F4 – 5D°4391.54450-48884(3)
a 3F4 – 5D°4391.54447-48-448(3)
a 3F4 – 5D°4391.54449-48474(3)
a 5F5 – y 5G°6498.31246-48-716.2(4)
a 5F5 – y 5G°6498.31250-48671.6(21)
a 5F5 – y 5G°6498.31247-48-346(3)
a 5F5 – y 5G°6498.31249-48355(3)
a 5F4 – y 5G°5499.24646-48-706.7(9)
a 5F4 – y 5G°5499.24650-48669.4(4)
a 5F3 – y 5G°4500.09046-48-703.2(12)
a 5F3 – y 5G°4500.09050-48660.1(6)
a 5F2 – y 5G°3500.86146-48-691.3(23)
a 5F2 – y 5G°3500.86150-48652.0(5)
a 5F1 – y 5G°2501.56746-48-682.7(3)
a 5F1 – y 5G°2501.56750-48642.1(4)
a 5F5 – y 5G°5501.75646-48-714.0(6)
a 5F5 – y 5G°5501.75650-48682.9(6)
a 5F4 – y 5G°4502.14346-48-702(5)
a 5F4 – y 5G°4502.14350-48670.6(11)
a 5F3 – y 5G°3502.42746-48-690.1(5)
a 5F3 – y 5G°3502.42750-48660.29(28)

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

Closed and nearly closed transitions of titanium

Transitionλ vacuum (nm)Lower levelA (s⁻¹)Leak per scattered photonPhotons before a leakWhere the leak goes
a 5F5 → z 5G°61039.9649metastable1.220e+05 measured1.95 × 10−7 from semi-empirical calc.5.13 × 106a 3G5 ≈ 1.95 × 10−7 (long-lived)
a 5F5 → y 5G°6498.3120metastable7.800e+07 measured2.5 × 10−6 from measured data400,000a 3G5 ≈ 5.13 × 10−7 (long-lived); a 3H6 ≈ 1.16 × 10−7; a 3H5 ≈ 5.28 × 10−9; 1 weaker lines; the listed lines add up to ≈ 6.34 × 10−7
a 5F1 → x 5D°0429.6958metastable1.390e+08 measured0.142 % from semi-empirical calc.704a 5P1 ≈ 0.132 % (long-lived); a 5D1 ≈ 5.67 × 10−5; a 3P1 ≈ 2.04 × 10−5 (long-lived); 4 weaker lines
a 3F4 → x 3G°5337.2420metastable9.000e+07 measured3.29 % from semi-empirical calc.30a 3H6 ≈ 1.85 %; b 3F4 1.29 % (long-lived); 3F4 ≈ 8.79 × 10−4; 10 weaker lines
a 3F3 → x 3G°4335.5597metastable8.400e+07 measured9.39 % from semi-empirical calc.11a 3F4 6.69 % (long-lived); a 3H5 ≈ 1.83 %; b 3F3 0.658 % (long-lived); 18 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 Ti 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
a 3F23G°3226.4719226.40181323.7515E10.961 NIST2.300e+07 NIST–NIST ASD (accuracy D)
a 3F3o 3D°2227.7405227.67021316.3775E11.947 NIST1.300e+08 NIST–NIST ASD (accuracy C)
a 3F4o 3D°3228.0671227.99671314.4924E11.963 NIST9.400e+07 NIST–NIST ASD (accuracy C)
a 3F2r 3F°2230.0567229.98591303.1240E11.440 NIST6.900e+07 NIST–NIST ASD (accuracy C)
a 3F3r 3F°3230.3446230.27371301.4957E11.551 NIST5.700e+07 NIST–NIST ASD (accuracy C)
a 3F4r 3F°4230.6384230.56741299.8377E11.683 NIST5.200e+07 NIST–NIST ASD (accuracy C)
a 3F4q 3D°3238.5246238.45191256.8616E10.494 measured5.200e+06 measured4.38Lawler, Guzman, Wood, Sneden, Cowan, Astrophys. J. Suppl. Ser. 205, 11 (2013)
a 3F3s 3F°3242.2040242.13051237.7683E10.799 NIST1.300e+07 NIST–NIST ASD (accuracy C)
a 3F4s 3F°4242.4986242.42501236.2645E11.038 NIST1.700e+07 NIST–NIST ASD (accuracy C)
a 3F43G°5244.1724244.09841227.7901E10.754 NIST7.200e+06 NIST9.29NIST ASD (accuracy C)
a 3F2s 3D°1252.1300252.05411189.0393E10.974 measured4.000e+07 measured33.3Lawler, Guzman, Wood, Sneden, Cowan, Astrophys. J. Suppl. Ser. 205, 11 (2013)
a 3F3s 3D°2253.0631252.98711184.6548E11.183 measured3.500e+07 measured28.8Lawler, Guzman, Wood, Sneden, Cowan, Astrophys. J. Suppl. Ser. 205, 11 (2013)
a 3F4s 3D°3254.2681254.19181179.0407E11.616 measured4.600e+07 measured38.4Lawler, Guzman, Wood, Sneden, Cowan, Astrophys. J. Suppl. Ser. 205, 11 (2013)
a 3F2t 3F°2260.0692259.99151152.7412E11.731 measured6.900e+07 measured40.7Lawler, Guzman, Wood, Sneden, Cowan, Astrophys. J. Suppl. Ser. 205, 11 (2013)
a 3F3t 3F°3260.5919260.51401150.4291E11.963 measured6.300e+07 measured37Lawler, Guzman, Wood, Sneden, Cowan, Astrophys. J. Suppl. Ser. 205, 11 (2013)
a 3F4t 3F°4261.2068261.12881147.7209E12.453 measured7.600e+07 measured44.8Lawler, Guzman, Wood, Sneden, Cowan, Astrophys. J. Suppl. Ser. 205, 11 (2013)
a 3F3t 3F°2261.2250261.14701147.6408E10.804 measured1.470e+07 measured8.67Lawler, Guzman, Wood, Sneden, Cowan, Astrophys. J. Suppl. Ser. 205, 11 (2013)
a 3F4t 3F°3262.0721261.99391143.9313E10.982 measured1.550e+07 measured9.11Lawler, Guzman, Wood, Sneden, Cowan, Astrophys. J. Suppl. Ser. 205, 11 (2013)
a 3F3u 3D°3263.2318263.15341138.8914E11.117 measured1.980e+07 measured8.12Lawler, Guzman, Wood, Sneden, Cowan, Astrophys. J. Suppl. Ser. 205, 11 (2013)
a 3F2u 3D°2263.3201263.24161138.5095E11.061 measured2.500e+07 measured10.2Lawler, Guzman, Wood, Sneden, Cowan, Astrophys. J. Suppl. Ser. 205, 11 (2013)
a 3F2u 3D°1264.1882264.10951134.7685E12.295 measured1.930e+08 measured77.8Lawler, Guzman, Wood, Sneden, Cowan, Astrophys. J. Suppl. Ser. 205, 11 (2013)
a 3F3u 3D°2264.5051264.42631133.4090E12.686 measured1.580e+08 measured64.5Lawler, Guzman, Wood, Sneden, Cowan, Astrophys. J. Suppl. Ser. 205, 11 (2013)
a 3F4u 3D°3264.7423264.66341132.3937E13.152 measured1.550e+08 measured63.5Lawler, Guzman, Wood, Sneden, Cowan, Astrophys. J. Suppl. Ser. 205, 11 (2013)
a 3F2v 3G°3266.2757266.19651125.8723E10.745 measured8.500e+06 measured8.44Lawler, Guzman, Wood, Sneden, Cowan, Astrophys. J. Suppl. Ser. 205, 11 (2013)
a 3F3v 3G°4267.0387266.95931122.6556E11.007 measured1.200e+07 measured10.5Lawler, Guzman, Wood, Sneden, Cowan, Astrophys. J. Suppl. Ser. 205, 11 (2013)
a 3F4v 3G°5268.0717267.99211118.3294E11.171 measured1.310e+07 measured11.4Lawler, Guzman, Wood, Sneden, Cowan, Astrophys. J. Suppl. Ser. 205, 11 (2013)
a 3F2v 3F°3293.4392293.35341021.6509E10.944 measured1.020e+07 measured4.9Lawler, Guzman, Wood, Sneden, Cowan, Astrophys. J. Suppl. Ser. 205, 11 (2013)
a 3F3v 3F°4293.8165293.73061020.3392E10.907 measured7.300e+06 measured3.67Lawler, Guzman, Wood, Sneden, Cowan, Astrophys. J. Suppl. Ser. 205, 11 (2013)
a 3F2v 3F°2294.2851294.19911018.7143E12.642 measured1.110e+08 measured53.3Lawler, Guzman, Wood, Sneden, Cowan, Astrophys. J. Suppl. Ser. 205, 11 (2013)
a 3F3v 3F°3294.9115294.82541016.5504E13.021 measured1.030e+08 measured49.4Lawler, Guzman, Wood, Sneden, Cowan, Astrophys. J. Suppl. Ser. 205, 11 (2013)
a 3F4v 3F°4295.6995295.61321013.8415E13.570 measured1.110e+08 measured55.7Lawler, Guzman, Wood, Sneden, Cowan, Astrophys. J. Suppl. Ser. 205, 11 (2013)
a 3F3v 3F°2295.7659295.67951013.6139E10.942 measured1.390e+07 measured6.67Lawler, Guzman, Wood, Sneden, Cowan, Astrophys. J. Suppl. Ser. 205, 11 (2013)
a 3F4v 3F°3296.8087296.72211010.0527E10.931 measured9.600e+06 measured4.61Lawler, Guzman, Wood, Sneden, Cowan, Astrophys. J. Suppl. Ser. 205, 11 (2013)
a 3F3w 3F°3298.4174298.33031004.6080E10.934 measured9.500e+06 measured45.2Lawler, Guzman, Wood, Sneden, Cowan, Astrophys. J. Suppl. Ser. 205, 11 (2013)
a 3F4w 3F°4300.1740300.0865998.7289E11.211 measured1.220e+07 measured57.1Lawler, Guzman, Wood, Sneden, Cowan, Astrophys. J. Suppl. Ser. 205, 11 (2013)
a 3F2w 3G°3318.7372318.6451940.5631E13.277 measured9.600e+07 measured63.5Lawler, Guzman, Wood, Sneden, Cowan, Astrophys. J. Suppl. Ser. 205, 11 (2013)
a 3F3w 3G°4319.2915319.1992938.9303E13.915 measured1.060e+08 measured67Lawler, Guzman, Wood, Sneden, Cowan, Astrophys. J. Suppl. Ser. 205, 11 (2013)
a 3F4w 3G°5320.0838319.9914936.6060E14.661 measured1.220e+08 measured74.2Lawler, Guzman, Wood, Sneden, Cowan, Astrophys. J. Suppl. Ser. 205, 11 (2013)
a 3F2x 3G°3334.2834334.1873896.8212E13.193 measured7.900e+07 measured84.5Lawler, Guzman, Wood, Sneden, Cowan, Astrophys. J. Suppl. Ser. 205, 11 (2013)
a 3F3x 3G°4335.5597335.4633893.4101E13.755 measured8.400e+07 measured89.9Lawler, Guzman, Wood, Sneden, Cowan, Astrophys. J. Suppl. Ser. 205, 11 (2013)
a 3F2w 3D°1337.1402337.0434889.2219E12.117 measured7.900e+07 measured78.2Lawler, Guzman, Wood, Sneden, Cowan, Astrophys. J. Suppl. Ser. 205, 11 (2013)
a 3F4x 3G°5337.2420337.1452888.9535E14.329 measured9.000e+07 measured97.2Lawler, Guzman, Wood, Sneden, Cowan, Astrophys. J. Suppl. Ser. 205, 11 (2013)
a 3F3w 3D°2337.8545337.7575887.3420E12.618 measured7.200e+07 measured65.7Lawler, Guzman, Wood, Sneden, Cowan, Astrophys. J. Suppl. Ser. 205, 11 (2013)
a 3F4w 3D°3338.6913338.5941885.1496E12.717 measured5.500e+07 measured47.5Lawler, Guzman, Wood, Sneden, Cowan, Astrophys. J. Suppl. Ser. 205, 11 (2013)
a 3F2y 3G°3363.6498363.5462824.3987E13.910 measured9.200e+07 measured85.4Lawler, Guzman, Wood, Sneden, Cowan, Astrophys. J. Suppl. Ser. 205, 11 (2013)
a 3F3y 3G°4364.3711364.2673822.7668E14.422 measured9.100e+07 measured86.1Lawler, Guzman, Wood, Sneden, Cowan, Astrophys. J. Suppl. Ser. 205, 11 (2013)
a 3F4y 3G°5365.4535365.3494820.3299E14.801 measured8.700e+07 measured89.6Lawler, Guzman, Wood, Sneden, Cowan, Astrophys. J. Suppl. Ser. 205, 11 (2013)
a 3F2x 3F°2373.0867372.9806803.5463E12.541 measured5.040e+07 measured80.1Lawler, Guzman, Wood, Sneden, Cowan, Astrophys. J. Suppl. Ser. 205, 11 (2013)
a 3F3x 3F°3374.2122374.1059801.1295E12.945 measured4.790e+07 measured75.7Lawler, Guzman, Wood, Sneden, Cowan, Astrophys. J. Suppl. Ser. 205, 11 (2013)
a 3F4x 3F°4375.3925375.2858798.6107E13.708 measured5.850e+07 measured90.1Lawler, Guzman, Wood, Sneden, Cowan, Astrophys. J. Suppl. Ser. 205, 11 (2013)
a 3F2y 5G°3376.4437376.3367796.3807E1 (intercombination)0.0679 measured2.500e+04 measured0.0333Lawler, Guzman, Wood, Sneden, Cowan, Astrophys. J. Suppl. Ser. 205, 11 (2013)
a 3F2y 5G°2377.4392377.3320794.2800E1 (intercombination)0.139 measured1.450e+05 measured0.194Lawler, Guzman, Wood, Sneden, Cowan, Astrophys. J. Suppl. Ser. 205, 11 (2013)
a 3F3y 5G°4377.5397377.4324794.0688E1 (intercombination)0.099 measured4.100e+04 measured0.0537Lawler, Guzman, Wood, Sneden, Cowan, Astrophys. J. Suppl. Ser. 205, 11 (2013)
a 3F3y 5G°3378.8702378.7626791.2802E1 (intercombination)0.0657 measured2.300e+04 measured0.0306Lawler, Guzman, Wood, Sneden, Cowan, Astrophys. J. Suppl. Ser. 205, 11 (2013)
a 3F4y 5G°5378.9875378.8799791.0352E1 (intercombination)0.117 measured4.600e+04 measured0.0598Lawler, Guzman, Wood, Sneden, Cowan, Astrophys. J. Suppl. Ser. 205, 11 (2013)
a 3F45D°4391.5443391.4334765.6668E1 (intercombination)0.783 measured2.300e+06 measured–NIST ASD Ti I lines table (local copy data/nist/Ti_I_lines_from1nm.tsv)
a 3F2y 3D°1394.9788394.8670759.0090E12.274 measured5.670e+07 measured82.2Lawler, Guzman, Wood, Sneden, Cowan, Astrophys. J. Suppl. Ser. 205, 11 (2013)
a 3F3y 3D°2395.7453395.6334757.5388E12.340 measured3.580e+07 measured66.2Lawler, Guzman, Wood, Sneden, Cowan, Astrophys. J. Suppl. Ser. 205, 11 (2013)
a 3F4y 3D°3395.9326395.8205757.1806E13.198 measured4.770e+07 measured69.6Lawler, Guzman, Wood, Sneden, Cowan, Astrophys. J. Suppl. Ser. 205, 11 (2013)
a 3F2y 3F°2398.2888398.1762752.7012E12.658 measured4.530e+07 measured80.2Lawler, Guzman, Wood, Sneden, Cowan, Astrophys. J. Suppl. Ser. 205, 11 (2013)
a 3F3y 3F°3399.0887398.9758751.1926E13.123 measured4.440e+07 measured75Lawler, Guzman, Wood, Sneden, Cowan, Astrophys. J. Suppl. Ser. 205, 11 (2013)
a 3F4y 3F°4399.9767399.8636749.5248E13.709 measured4.840e+07 measured88.6Lawler, Guzman, Wood, Sneden, Cowan, Astrophys. J. Suppl. Ser. 205, 11 (2013)
a 5F2x 5D°2429.0277428.9070698.7719E12.714 measured3.780e+07 measured27.3Lawler, Guzman, Wood, Sneden, Cowan, Astrophys. J. Suppl. Ser. 205, 11 (2013)
a 5F1x 5D°1429.2136429.0929698.4691E12.333 measured4.650e+07 measured33Lawler, Guzman, Wood, Sneden, Cowan, Astrophys. J. Suppl. Ser. 205, 11 (2013)
a 5F1x 5D°0429.6958429.5749697.6854E12.333 measured1.390e+08 measured99.9Lawler, Guzman, Wood, Sneden, Cowan, Astrophys. J. Suppl. Ser. 205, 11 (2013)
a 5F3y 5F°4451.9289451.8022663.3620E12.878 measured2.020e+07 measured17.6Lawler, Guzman, Wood, Sneden, Cowan, Astrophys. J. Suppl. Ser. 205, 11 (2013)
a 5F2y 5F°3452.4065452.2797662.6616E12.828 measured2.500e+07 measured21.8Lawler, Guzman, Wood, Sneden, Cowan, Astrophys. J. Suppl. Ser. 205, 11 (2013)
a 5F1y 5F°2452.8574452.7304662.0019E12.301 measured2.310e+07 measured20.6Lawler, Guzman, Wood, Sneden, Cowan, Astrophys. J. Suppl. Ser. 205, 11 (2013)
a 5F2y 5F°1454.5961454.4687659.4699E12.296 measured3.790e+07 measured33.8Lawler, Guzman, Wood, Sneden, Cowan, Astrophys. J. Suppl. Ser. 205, 11 (2013)
a 5F3y 5F°2455.0039454.8763658.8789E12.799 measured3.370e+07 measured30Lawler, Guzman, Wood, Sneden, Cowan, Astrophys. J. Suppl. Ser. 205, 11 (2013)
a 5F5y 5G°6498.3120498.1730601.6159E17.869 measured7.800e+07 measured100Lawler, Guzman, Wood, Sneden, Cowan, Astrophys. J. Suppl. Ser. 205, 11 (2013)
a 5F4y 5G°5499.2458499.1066600.4906E16.827 measured6.900e+07 measured89.7Lawler, Guzman, Wood, Sneden, Cowan, Astrophys. J. Suppl. Ser. 205, 11 (2013)
a 5F3y 5G°4500.0898499.9503599.4773E15.869 measured6.200e+07 measured81.2Lawler, Guzman, Wood, Sneden, Cowan, Astrophys. J. Suppl. Ser. 205, 11 (2013)
a 5F2y 5G°3500.8606500.7209598.5547E14.957 measured5.660e+07 measured75.3Lawler, Guzman, Wood, Sneden, Cowan, Astrophys. J. Suppl. Ser. 205, 11 (2013)
a 5F1y 5G°2501.5675501.4276597.7111E14.235 measured5.760e+07 measured77.2Lawler, Guzman, Wood, Sneden, Cowan, Astrophys. J. Suppl. Ser. 205, 11 (2013)
a 5F5y 5G°5501.7560501.6161597.4865E12.328 measured7.900e+06 measured10.3Lawler, Guzman, Wood, Sneden, Cowan, Astrophys. J. Suppl. Ser. 205, 11 (2013)
a 5F4y 5G°4502.1426502.0026597.0265E12.786 measured1.380e+07 measured18.1Lawler, Guzman, Wood, Sneden, Cowan, Astrophys. J. Suppl. Ser. 205, 11 (2013)
a 5F3y 5G°3502.4269502.2868596.6887E12.777 measured1.760e+07 measured23.4Lawler, Guzman, Wood, Sneden, Cowan, Astrophys. J. Suppl. Ser. 205, 11 (2013)
a 5F2y 5G°2502.6246502.4844596.4540E12.218 measured1.570e+07 measured21Lawler, Guzman, Wood, Sneden, Cowan, Astrophys. J. Suppl. Ser. 205, 11 (2013)
a 5F3y 5G°2504.2019504.0614594.5881E10.593 measured1.110e+06 measured1.49Lawler, Guzman, Wood, Sneden, Cowan, Astrophys. J. Suppl. Ser. 205, 11 (2013)
a 5F4y 5G°3504.4990504.3584594.2379E10.649 measured9.500e+05 measured1.26Lawler, Guzman, Wood, Sneden, Cowan, Astrophys. J. Suppl. Ser. 205, 11 (2013)
a 5F5y 5G°4504.6821504.5414594.0224E10.487 measured4.160e+05 measured0.545Lawler, Guzman, Wood, Sneden, Cowan, Astrophys. J. Suppl. Ser. 205, 11 (2013)
a 5F55D°4524.0044523.8586572.1182E10.506 theory4.000e+05 theory–Eustice, Filin, Schrott, Porsev, Cheung, Novoa, Stamper-Kurn, Safronova, Phys. Rev. A 107…
b 3F2y 5G°3665.2192665.0355450.6672E1 (intercombination)0.111 measured1.200e+04 measured0.016Lawler, Guzman, Wood, Sneden, Cowan, Astrophys. J. Suppl. Ser. 205, 11 (2013)
b 3F3y 5G°4665.8851665.7013450.2165E1 (intercombination)0.148 measured1.660e+04 measured0.0217Lawler, Guzman, Wood, Sneden, Cowan, Astrophys. J. Suppl. Ser. 205, 11 (2013)
a 3G4y 5G°3876.6087876.3680341.9912E1 (intercombination)0.200 measured1.710e+04 measured0.0227Lawler, Guzman, Wood, Sneden, Cowan, Astrophys. J. Suppl. Ser. 205, 11 (2013)
a 3G3y 5G°2878.2547878.0135341.3503E1 (intercombination)0.208 measured2.600e+04 measured0.0348Lawler, Guzman, Wood, Sneden, Cowan, Astrophys. J. Suppl. Ser. 205, 11 (2013)
a 5F5z 5G°61039.96491039.6800288.2717E10.938 measured1.220e+05 measured100Duim, Eustice, Schrott, Sawaoka, Stamper-Kurn, "Narrow-line magneto-optical trap of titan…

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.

Ti energy levels

LevelEnergy (cm⁻¹)JParityLifetimegJHyperfine A (MHz)Hyperfine B (MHz)Lifetime sourceHyperfine source
a 3F20.0002evenstable0.666––––
a 3F3170.1333even–1.083-52.904728.082–Channappa & Pendlebury 1965 / Aydin et al. 1990, as tabulated in Schrott, Eustice, Sadegh…
a 3F4386.8744even–1.25-37.991837.681–Channappa & Pendlebury 1965 / Aydin et al. 1990, as tabulated in Schrott, Eustice, Sadegh…
a 5F16556.8331even––––––
a 5F26598.7652even–0.99––––
a 5F36661.0063even–1.25––––
a 5F46742.7564even–1.35––––
a 5F56842.9625even–1.41-74.845-28.674–Channappa & Pendlebury 1965 / Aydin et al. 1990, as tabulated in Schrott, Eustice, Sadegh…
b 3F211531.7612even–0.67––––
b 3F311639.8113even–1.08––––
a 3G315108.1113even–0.74––––
a 3G415156.8024even–1.06––––
z 5G°616458.6716odd8.2 µs measured1.333-8577Duim, Eustice, Schrott, Sawaoka, Stamper-Kurn, "Narrow-line magneto-optical trap of titan…Schrott, Eustice, Sadeghpour, Duim, Sawaoka, Filin, Safronova, Stamper-Kurn, "Hyperfine s…
y 3F°225107.4112odd< 17.7 ns measured0.67––Lawler, Guzman, Wood, Sneden, Cowan, Astrophys. J. Suppl. Ser. 205, 11 (2013). Note: deri…–
y 3F°325227.2223odd< 16.9 ns measured1.081––Lawler, Guzman, Wood, Sneden, Cowan, Astrophys. J. Suppl. Ser. 205, 11 (2013). Note: deri…–
y 3D°125317.8141odd< 14.5 ns measured0.542––Lawler, Guzman, Wood, Sneden, Cowan, Astrophys. J. Suppl. Ser. 205, 11 (2013). Note: deri…–
y 3F°425388.3314odd< 18.3 ns measured1.24––Lawler, Guzman, Wood, Sneden, Cowan, Astrophys. J. Suppl. Ser. 205, 11 (2013). Note: deri…–
y 3D°225438.9082odd< 18.5 ns measured1.283––Lawler, Guzman, Wood, Sneden, Cowan, Astrophys. J. Suppl. Ser. 205, 11 (2013). Note: deri…–
y 3D°325643.7013odd< 14.6 ns measured1.362––Lawler, Guzman, Wood, Sneden, Cowan, Astrophys. J. Suppl. Ser. 205, 11 (2013). Note: deri…–
5D°425926.7714odd–1.498-96.6-0.24–Schrott, Eustice, Sadeghpour, Duim, Sawaoka, Filin, Safronova, Stamper-Kurn, "Hyperfine s…
y 5G°226494.3302odd< 13.4 ns measured0.337––Lawler, Guzman, Wood, Sneden, Cowan, Astrophys. J. Suppl. Ser. 205, 11 (2013). Note: deri…–
y 5G°326564.4003odd< 13.3 ns measured0.917––Lawler, Guzman, Wood, Sneden, Cowan, Astrophys. J. Suppl. Ser. 205, 11 (2013). Note: deri…–
y 5G°426657.4164odd< 13.1 ns measured1.151––Lawler, Guzman, Wood, Sneden, Cowan, Astrophys. J. Suppl. Ser. 205, 11 (2013). Note: deri…–
y 5G°526772.9685odd< 13 ns measured1.267––Lawler, Guzman, Wood, Sneden, Cowan, Astrophys. J. Suppl. Ser. 205, 11 (2013). Note: deri…–
x 3F°226803.4202odd< 15.9 ns measured0.675––Lawler, Guzman, Wood, Sneden, Cowan, Astrophys. J. Suppl. Ser. 205, 11 (2013). Note: deri…–
x 3F°326892.9363odd< 15.8 ns measured1.092––Lawler, Guzman, Wood, Sneden, Cowan, Astrophys. J. Suppl. Ser. 205, 11 (2013). Note: deri…–
y 5G°626910.7096odd< 12.8 ns measured1.333-14.2-1.1Lawler, Guzman, Wood, Sneden, Cowan, Astrophys. J. Suppl. Ser. 205, 11 (2013). Note: deri…Schrott, Eustice, Sadeghpour, Duim, Sawaoka, Filin, Safronova, Stamper-Kurn, "Hyperfine s…
x 3F°427025.6594odd< 15.4 ns measured1.254––Lawler, Guzman, Wood, Sneden, Cowan, Astrophys. J. Suppl. Ser. 205, 11 (2013). Note: deri…–
y 3G°327498.9823odd< 9.28 ns measured0.754––Lawler, Guzman, Wood, Sneden, Cowan, Astrophys. J. Suppl. Ser. 205, 11 (2013). Note: deri…–
y 3G°427614.6794odd< 9.46 ns measured1.054––Lawler, Guzman, Wood, Sneden, Cowan, Astrophys. J. Suppl. Ser. 205, 11 (2013). Note: deri…–
y 3G°527750.1355odd< 10.3 ns measured1.206––Lawler, Guzman, Wood, Sneden, Cowan, Astrophys. J. Suppl. Ser. 205, 11 (2013). Note: deri…–
y 5F°128596.3131odd< 8.91 ns measured0.001––Lawler, Guzman, Wood, Sneden, Cowan, Astrophys. J. Suppl. Ser. 205, 11 (2013). Note: deri…–
y 5F°228638.8412odd< 8.91 ns measured1.001––Lawler, Guzman, Wood, Sneden, Cowan, Astrophys. J. Suppl. Ser. 205, 11 (2013). Note: deri…–
y 5F°328702.7783odd< 8.72 ns measured1.249––Lawler, Guzman, Wood, Sneden, Cowan, Astrophys. J. Suppl. Ser. 205, 11 (2013). Note: deri…–
y 5F°428788.3804odd< 8.72 ns measured1.348––Lawler, Guzman, Wood, Sneden, Cowan, Astrophys. J. Suppl. Ser. 205, 11 (2013). Note: deri…–
w 3D°129661.2501odd< 9.9 ns measured0.508––Lawler, Guzman, Wood, Sneden, Cowan, Astrophys. J. Suppl. Ser. 205, 11 (2013). Note: deri…–
w 3D°229768.6752odd< 9.12 ns measured1.167––Lawler, Guzman, Wood, Sneden, Cowan, Astrophys. J. Suppl. Ser. 205, 11 (2013). Note: deri…–
x 5D°029829.1120odd< 7.19 ns measured–––Lawler, Guzman, Wood, Sneden, Cowan, Astrophys. J. Suppl. Ser. 205, 11 (2013). Note: deri…–
x 5D°129855.2551odd< 7.09 ns measured1.498––Lawler, Guzman, Wood, Sneden, Cowan, Astrophys. J. Suppl. Ser. 205, 11 (2013). Note: deri…–
x 5D°229907.2862odd< 7.21 ns measured1.497––Lawler, Guzman, Wood, Sneden, Cowan, Astrophys. J. Suppl. Ser. 205, 11 (2013). Note: deri…–
w 3D°329912.2863odd< 8.63 ns measured1.338––Lawler, Guzman, Wood, Sneden, Cowan, Astrophys. J. Suppl. Ser. 205, 11 (2013). Note: deri…–
x 3G°329914.7373odd< 10.7 ns measured0.753––Lawler, Guzman, Wood, Sneden, Cowan, Astrophys. J. Suppl. Ser. 205, 11 (2013). Note: deri…–
x 3G°429971.0864odd< 10.7 ns measured1.089––Lawler, Guzman, Wood, Sneden, Cowan, Astrophys. J. Suppl. Ser. 205, 11 (2013). Note: deri…–
x 3G°530039.1705odd< 10.8 ns measured1.201––Lawler, Guzman, Wood, Sneden, Cowan, Astrophys. J. Suppl. Ser. 205, 11 (2013). Note: deri…–
w 3G°331373.8073odd< 6.62 ns measured0.752––Lawler, Guzman, Wood, Sneden, Cowan, Astrophys. J. Suppl. Ser. 205, 11 (2013). Note: deri…–
w 3G°431489.4764odd< 6.32 ns measured1.052––Lawler, Guzman, Wood, Sneden, Cowan, Astrophys. J. Suppl. Ser. 205, 11 (2013). Note: deri…–
w 3G°531628.6885odd< 6.08 ns measured1.202––Lawler, Guzman, Wood, Sneden, Cowan, Astrophys. J. Suppl. Ser. 205, 11 (2013). Note: deri…–
w 3F°333680.2483odd< 47.6 ns measured1.086––Lawler, Guzman, Wood, Sneden, Cowan, Astrophys. J. Suppl. Ser. 205, 11 (2013). Note: deri…–
w 3F°433700.8844odd< 46.8 ns measured1.254––Lawler, Guzman, Wood, Sneden, Cowan, Astrophys. J. Suppl. Ser. 205, 11 (2013). Note: deri…–
v 3F°233980.6532odd< 4.8 ns measured0.664––Lawler, Guzman, Wood, Sneden, Cowan, Astrophys. J. Suppl. Ser. 205, 11 (2013). Note: deri…–
v 3F°334078.6063odd< 4.8 ns measured1.085––Lawler, Guzman, Wood, Sneden, Cowan, Astrophys. J. Suppl. Ser. 205, 11 (2013). Note: deri…–
v 3F°434204.9854odd< 5.02 ns measured1.252––Lawler, Guzman, Wood, Sneden, Cowan, Astrophys. J. Suppl. Ser. 205, 11 (2013). Note: deri…–
v 3G°337555.0583odd< 9.93 ns measured0.769––Lawler, Guzman, Wood, Sneden, Cowan, Astrophys. J. Suppl. Ser. 205, 11 (2013). Note: deri…–
v 3G°437617.8944odd< 8.77 ns measured1.075––Lawler, Guzman, Wood, Sneden, Cowan, Astrophys. J. Suppl. Ser. 205, 11 (2013). Note: deri…–
v 3G°537690.3275odd< 8.69 ns measured1.198––Lawler, Guzman, Wood, Sneden, Cowan, Astrophys. J. Suppl. Ser. 205, 11 (2013). Note: deri…–
u 3D°137851.8021odd< 4.03 ns measured0.516––Lawler, Guzman, Wood, Sneden, Cowan, Astrophys. J. Suppl. Ser. 205, 11 (2013). Note: deri…–
u 3D°237976.5892odd< 4.08 ns measured1.162––Lawler, Guzman, Wood, Sneden, Cowan, Astrophys. J. Suppl. Ser. 205, 11 (2013). Note: deri…–
u 3D°338159.4613odd< 4.1 ns measured1.331––Lawler, Guzman, Wood, Sneden, Cowan, Astrophys. J. Suppl. Ser. 205, 11 (2013). Note: deri…–
t 3F°238451.3092odd< 5.9 ns measured0.675––Lawler, Guzman, Wood, Sneden, Cowan, Astrophys. J. Suppl. Ser. 205, 11 (2013). Note: deri…–
t 3F°338544.3163odd< 5.88 ns measured1.086––Lawler, Guzman, Wood, Sneden, Cowan, Astrophys. J. Suppl. Ser. 205, 11 (2013). Note: deri…–
t 3F°438670.7234odd< 5.9 ns measured1.25––Lawler, Guzman, Wood, Sneden, Cowan, Astrophys. J. Suppl. Ser. 205, 11 (2013). Note: deri…–
s 3D°139662.0811odd< 8.33 ns measured0.506––Lawler, Guzman, Wood, Sneden, Cowan, Astrophys. J. Suppl. Ser. 205, 11 (2013). Note: deri…–
s 3D°239685.9642odd< 8.23 ns measured1.168––Lawler, Guzman, Wood, Sneden, Cowan, Astrophys. J. Suppl. Ser. 205, 11 (2013). Note: deri…–
s 3D°339715.4393odd< 8.34 ns measured1.327––Lawler, Guzman, Wood, Sneden, Cowan, Astrophys. J. Suppl. Ser. 205, 11 (2013). Note: deri…–
3G°541341.5435odd< 12.9 ns measured1.498––Lawler, Guzman, Wood, Sneden, Cowan, Astrophys. J. Suppl. Ser. 205, 11 (2013). Note: deri…–
s 3F°341457.6393odd–1.146––––
s 3F°441624.2194odd–1.25––––
q 3D°342311.2643odd< 8.42 ns measured1.332––Lawler, Guzman, Wood, Sneden, Cowan, Astrophys. J. Suppl. Ser. 205, 11 (2013). Note: deri…–
r 3F°243467.5372odd––––––
r 3F°343583.3553odd––––––
r 3F°443744.7934odd––––––
o 3D°244079.7612odd––––––
3G°344155.5963odd––––––
o 3D°344233.6203odd––––––

Ti⁺ ionisation limit 55072.50 cm⁻¹ = 6.82812 eV (181.579 nm)

Sources

Transition probabilities are from the machine-readable Table 3 of Lawler et al. 2013 (948 lines), restricted to lines the site draws plus all lines from y5G, y5D4; level energies there (Saloman 2012) equal the NIST energies. NIST ASD already carries A values for most of these lines (often from the same group). rme_J_ea0 is derived from A with the SCHEMA convention. Level lifetimes marked "derived" are 1/sum(A) over the Lawler branches (see note in each entry); only z5G6 has a direct cold-atom lifetime measurement. Isotope shifts are nu(A) - nu(48) as printed in the sources; fermion shifts refer to the hyperfine centre of gravity. Hyperfine A, B follow E = A K/2 + B [3K(K+1) - 4J(J+1)I(I+1)] / [8I(2I-1)J(2J-1)] (Eq. 6 of Schrott et al.); all A are negative. Extra fields beyond SCHEMA.md: top-level ionization_limit, laser_cooling_scheme, conflicts; level fields hyperfine_other, lifetime_other, decay_rates_theory, magnetic_moment_muB; transition fields linewidth_MHz / linewidth_kHz, A_s_other, saturation_intensity_*, doppler_limit_uK, leak_to_metastable, king_plot. Entries whose note says UPPER BOUND / LOWER BOUND / derived / theory are not direct measurements.

Atoms with measured data

All elements: periodic table