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    Energies are given in cm\(^{-1}\). See this link for conversion factors. Electric matrix elements are given in atomic units. Magnetic dipole matrix elements are given in Bohr magnetons, \(\mu_B\). The values of magnetic-dipole hyperfine constants A are listed in MHz. Dipole polarizabilities \(\alpha\) are given in atomic units, \(a_0^3\), where \(a_0\) is the Bohr radius. The atomic units for \(\alpha\) can be converted to SI units via \(\alpha /h \rm{[Hz/(V/m)^2]}\)\(=2.48832 \times 10^{-8} \alpha \) [a.u.], where the conversion coefficient is \( 4\pi \epsilon_0 a^3_0/h \) and the Planck constant \(h\) is factored out.

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    Data are taken from, “M. S. Safronova, V. A. Dzuba, V. V. Flambaum, U. I. Safronova, S. G. Porsev, and M. G. Kozlov, Phys. Rev. A 90, 042513 (2014), DOI: https://doi.org/10.1103/PhysRevA.90.042513", unless noted otherwise.
    Note:
    Transition types ‘M1’, ‘E1’ and ‘E2’ stand for magnetic dipole, electric dipole and electric quadrupole transition, respectively.
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    State Energy
    		 \(\ \lambda \)
    		 \( \alpha \)-variation sensitivity q
    		 Enhancement factor K Lifetime
    \(\ \) \(\ \rm{cm}^{-1} \) nm \(\ \rm{cm}^{-1} \) \(\ \) s
    $$ 5s^24f\ ^2F_{5/2} $$ 0 $$ $$ 0 $$ $$ $$ $$
    $$ 5s^24f\ ^2F_{7/2} $$ 6203(100) 1612(28) 5654 1.8 0.367
    $$ 5s4f^2\ ^4H_{7/2} $$ 20254(940) 494(22) 123621 12 0.133
    $$ 5s4f^2\ ^4H_{9/2} $$ 22519(950) 444(18) 125397 11 0.141
    $$ 5s4f^2\ ^4H_{11/2} $$ 25904(980) 386(14) 128875 10 0.576
    $$ 5s4f^2\ ^4F_{3/2} $$ 29249(900) 342(10) 124872 8.5 6.74 \(\ \times 10^{-3} \)
    $$ 5s4f^2\ ^4H_{13/2} $$ 29727(1000) 336(11) $$ $$ $$ $$ 0.597
    $$ 5s4f^2\ ^4F_{5/2} $$ 30739(900) 325(9) $$ $$ $$ $$ 9.62 \(\ \times 10^{-3} \)
    $$ 5s4f^2\ ^4F_{7/2} $$ 32786(920) 305(8) $$ $$ $$ $$ 1.20 \(\ \times 10^{-2} \)
    $$ 5s4f^2\ ^2H_{9/2} $$ 33152(950) 302(8) $$ $$ $$ $$ 2.78 \(\ \times 10^{-3} \)
    $$ 5s4f^2\ ^4F_{9/2} $$ 34871(950) 287(8) $$ $$ $$ $$ 9.61 \(\ \times 10^{-3} \)
    $$ 5s4f^2\ ^2G_{7/2} $$ 39572(930) 253(6) $$ $$ $$ $$ 5.31 \(\ \times 10^{-4} \)
    $$ 5s4f^2\ ^2H_{11/2} $$ 40319(1000) 248(6) $$ $$ $$ $$ 0.207
    $$ 5s4f^2\ ^2F_{5/2} $$ 42132(900) 237(5) $$ $$ $$ $$ 3.19 \(\ \times 10^{-4} \)

    Transition Type Transition energy
    		 \(\ \lambda \) Matrix element
    		 Transition rate
    \(\ \) \(\ \) \(\ \rm{cm}^{-1} \) nm \(\ \) \(\ \rm{s}^{-1} \)
    $$ 5s^24f\ ^2F_{7/2} - 5s^24f\ ^2F_{5/2} $$ M1 6203 1612 1.84102 \(\ \mu_B \) 2.728
    $$ 5s^24f\ ^2F_{7/2} - 5s^24f\ ^2F_{5/2} $$ E2 6203 1612 0.19504 a.u. 4.891 \(\ \times 10^{-6} \)
    $$ 5s4f^2\ ^4H_{7/2} - 5s^24f\ ^2F_{5/2} $$ E1 20254 493.7 0.00188 a.u. 7.443
    $$ 5s4f^2\ ^4H_{7/2} - 5s^24f\ ^2F_{7/2} $$ E1 14051 711.7 0.00027 a.u. 4.949 \(\ \times 10^{-2} \)
    $$ 5s4f^2\ ^4H_{9/2} - 5s^24f\ ^2F_{7/2} $$ E1 16316 612.9 0.00275 a.u. 6.636
    $$ 5s4f^2\ ^4H_{9/2} - 5s4f^2\ ^4H_{7/2} $$ M1 2265 4415 3.85331 \(\ \mu_B \) 4.654 \(\ \times 10^{-1} \)
    $$ 5s4f^2\ ^4H_{11/2} - 5s4f^2\ ^4H_{9/2} $$ M1 3385 2954 4.46125 \(\ \mu_B \) 1.735
    $$ 5s4f^2\ ^4F_{3/2} - 5s^24f\ ^2F_{5/2} $$ E1 29249 341.9 0.00342 a.u. 1.484 \(\ \times 10^{2} \)
    $$ 5s4f^2\ ^4F_{3/2} - 5s4f^2\ ^4H_{7/2} $$ E2 8995 1112 0.41986 a.u. 2.906 \(\ \times 10^{-4} \)
    $$ 5s4f^2\ ^4H_{13/2} - 5s4f^2\ ^4H_{11/2} $$ M1 3823 2616 3.94520 \(\ \mu_B \) 1.676
    $$ 5s4f^2\ ^4F_{5/2} - 5s^24f\ ^2F_{5/2} $$ E1 30739 325.3 0.00293 a.u. 8.426 \(\ \times 10^{1} \)
    $$ 5s4f^2\ ^4F_{5/2} - 5s^24f\ ^2F_{7/2} $$ E1 24536 407.6 0.00198 a.u. 1.956 \(\ \times 10^{1} \)
    $$ 5s4f^2\ ^4F_{5/2} - 5s4f^2\ ^4F_{3/2} $$ M1 1490 6711 3.02227 \(\ \mu_B \) 1.358 \(\ \times 10^{-1} \)
    $$ 5s4f^2\ ^4F_{7/2} - 5s^24f\ ^2F_{5/2} $$ E1 32786 305.0 0.00280 a.u. 6.993 \(\ \times 10^{1} \)
    $$ 5s4f^2\ ^4F_{7/2} - 5s^24f\ ^2F_{7/2} $$ E1 26583 376.2 0.00165 a.u. 1.292 \(\ \times 10^{1} \)
    $$ 5s4f^2\ ^4F_{7/2} - 5s4f^2\ ^4H_{7/2} $$ M1 12532 798.0 0.17406 \(\ \mu_B \) 2.011 \(\ \times 10^{-1} \)
    $$ 5s4f^2\ ^4F_{7/2} - 5s4f^2\ ^4F_{5/2} $$ M1 2047 4885 3.45759 \(\ \mu_B \) 3.457 \(\ \times 10^{-1} \)
    $$ 5s4f^2\ ^2H_{9/2} - 5s^24f\ ^2F_{7/2} $$ E1 26949 371.1 0.00948 3.565 \(\ \times 10^{2} \)
    $$ 5s4f^2\ ^2H_{9/2} - 5s4f^2\ ^4H_{7/2} $$ M1 12898 775.3 0.68350 \(\ \mu_B \) 2.704
    $$ 5s4f^2\ ^4F_{9/2} - 5s^24f\ ^2F_{7/2} $$ E1 28668 348.8 0.00461 a.u. 1.014 \(\ \times 10^{2} \)
    $$ 5s4f^2\ ^4F_{9/2} - 5s4f^2\ ^4H_{7/2} $$ M1 14617 684.1 0.47324 \(\ \mu_B \) 1.887
    $$ 5s4f^2\ ^4F_{9/2} - 5s4f^2\ ^4H_{9/2} $$ M1 12352 809.6 0.31751 \(\ \mu_B \) 5.125 \(\ \times 10^{-1} \)
    $$ 5s4f^2\ ^4F_{9/2} - 5s4f^2\ ^4F_{7/2} $$ M1 2085 4796 2.17854 \(\ \mu_B \) 1.160 \(\ \times 10^{-1} \)
    $$ 5s4f^2\ ^2G_{7/2} - 5s^24f\ ^2F_{5/2} $$ E1 39572 252.7 0.00971 a.u. 1.481 \(\ \times 10^{3} \)
    $$ 5s4f^2\ ^2G_{7/2} - 5s^24f\ ^2F_{7/2} $$ E1 33369 299.7 0.00649 a.u. 3.966 \(\ \times 10^{2} \)
    $$ 5s4f^2\ ^2G_{7/2} - 5s4f^2\ ^4H_{7/2} $$ M1 19318 517.7 0.36685 \(\ \mu_B \) 3.271
    $$ 5s4f^2\ ^2G_{7/2} - 5s4f^2\ ^4H_{7/2} $$ E2 19318 517.7 0.05278 \(\ \mu_B \) 1.049 \(\ \times 10^{-4} \)
    $$ 5s4f^2\ ^2G_{7/2} - 5s4f^2\ ^4H_{9/2} $$ M1 17053 586.4 0.31357 \(\ \mu_B \) 1.644
    $$ 5s4f^2\ ^2H_{11/2} - 5s4f^2\ ^4H_{9/2} $$ M1 17800 561.8 0.20464 \(\ \mu_B \) 5.309 \(\ \times 10^{-1} \)
    $$ 5s4f^2\ ^2H_{11/2} - 5s4f^2\ ^4H_{13/2} $$ M1 10592 944.1 0.61320 \(\ \mu_B \) 1.004
    $$ 5s4f^2\ ^2H_{11/2} - 5s4f^2\ ^2H_{9/2} $$ M1 7167 1395 1.62592 \(\ \mu_B \) 2.188
    $$ 5s4f^2\ ^2H_{11/2} - 5s4f^2\ ^4F_{9/2} $$ M1 5448 1836 1.66384 \(\ \mu_B \) 1.006
    $$ 5s4f^2\ ^2F_{5/2} - 5s^24f\ ^2F_{5/2} $$ E1 42132 237.3 0.01101 a.u. 3.062 \(\ \times 10^{3} \)
    $$ 5s4f^2\ ^2F_{5/2} - 5s^24f\ ^2F_{7/2} $$ E1 35929 278.3 0.00214 a.u. 7.140 \(\ \times 10^{1} \)
    $$ 5s4f^2\ ^2F_{5/2} - 5s4f^2\ ^4F_{3/2} $$ M1 12883 776.2 0.43453 \(\ \mu_B \) 1.815