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Table 2:

Hyperfine structure constants Al and Bl from the literature for low-lying levels of even parity.

E(cm-1)
Configuration Term Method Al(MHz) Bl(MHz) Ref.

0.00
$\rm 4d^45s $ $\rm ^6D_{1/2} $ abmr 1868.2184 (18) - Büttgenbach et al. (1975)
154.19 $\rm 4d^45s $ $\rm ^6D_{3/2} $ abmr 852.5428 (21) -64.572 (41) Büttgenbach et al. (1975)
391.99 $\rm 4d^45s $ $\rm ^6D_{5/2} $ abmr 719.4759 (18) -47.605 (39) Büttgenbach et al. (1975)
695.25 $\rm 4d^45s $ $\rm ^6D_{7/2} $ abmr 690.1978 (16) 20.475 (75) Büttgenbach et al. (1975)
1050.26 $\rm 4d^45s $ $\rm ^6D_{9/2} $ abmr 691.6141 (22) 132.754 (116) Büttgenbach et al. (1975)
1142.79 $\rm 4d^35s^2 $ $\rm ^4F_{3/2} $ abmr 644.16 (54) 32.800 (128) Büttgenbach et al. (1975)
1 586.90 $\rm 4d^35s^2 $ $\rm ^4F_{5/2} $ abmr 372.4853 (17) 33.341 (38) Büttgenbach et al. (1975)
2154.11 $\rm 4d^35s^2 $ $\rm ^4F_{7/2} $ abmr 292.2022 (16) 44.928 (47) Büttgenbach et al. (1975)
2805.36 $\rm 4d^35s^2 $ $\rm ^4F_{9/2} $ abmr 269.6320 (26) 64.315 (130) Büttgenbach et al. (1975)
4998.17 $\rm 4d^35s^2 $ $\rm ^4P_{1/2} $ lrf 540.1 (0.9) - Fraenkel et al. (1988)
5297.92 $\rm 4d^35s^2 $ $\rm ^4P_{3/2} $ lrf 497.7569 (16) 59.902 (14) Fraenkel et al. (1988)
5965.45 $\rm 4d^35s^2 $ $\rm ^4P_{5/2} $ lrf 343.1670 (5) -80.454 (9) Fraenkel et al. (1988)
8410.90 $\rm 4d^45s $ $\rm ^4D_{1/2} $ lrf 1997.0 (1.1) - Fraenkel et al. (1988)
8705.32 $\rm 4d^45s $ $\rm ^4D_{3/2} $ lrf -143.3225 (217) -10.761 (178) Fraenkel et al. (1988)
8827.00 $\rm 4d^35s^2 $ $\rm ^2G_{7/2} $ lrf 420.2938 (11) -49.006 (36) Fraenkel et al. (1988)
9043.14 $\rm 4d^45s $ $\rm ^4D_{5/2} $ lrf -407.8606 (43) 35.060 (75) Fraenkel et al. (1988)
9328.88 $\rm 4d^35s^2 $ $\rm ^2G_{9/2} $ lrf 358.5642 (8) -61.048 (30) Fraenkel et al. (1988)
9439.08 $\rm 4d^35s^2 $ $\rm ^2D_{3/2} $ lrf 389.1039 (23) 73.590 (19) Fraenkel et al. (1988)
9497.52 $\rm 4d^45s $ $\rm ^4D_{7/2} $ lrf -477.0373 (35) 126.899 (81) Fraenkel et al. (1988)
10 126.06 $\rm 4d^35s^2 $ $\rm ^2P_{1/2} $ lrf 323.6590 (4) - Fraenkel et al. (1988)
10 237.51 $\rm 4d^35s^2 $ $\rm ^2D_{5/2} $ lrf 295.6803 (6) 36.501 (12) Fraenkel et al. (1988)
10 922.74 $\rm 4d^45s $ $\rm ^4H_{7/2} $ lif -200 (50) - Kröger (2007)
11 044.08 $\rm 4d^45s $ $\rm ^4H_{9/2} $ lif 334 (50) - Kröger (2007)
11 247.88 $\rm 4d^45s $ $\rm ^4H_{11/2}$ lif 560 (30) - Kröger (2007)
11 344.70 $\rm 4d^5 $ $\rm ^6S_{5/2} $ lrf -639.3786 (79) -0.061 (92) Fraenkel et al. (1988)
11 524.65 $\rm 4d^45s $ $\rm ^4H_{13/2}$ lif 662 (20) - Kröger (2007)
12 102.12 $\rm 4d^35s^2 $ $\rm ^2H_{9/2} $ lrf 384.9669 (33) -163.323 (96) Fraenkel et al. (1988)
12 136.86 $\rm 4d^45s $ $\rm ^4G_{7/2} $ lif 502.4 (1.4) - Kröger (2007)
12 288.25 $\rm 4d^45s $ $\rm ^4F_{3/2} $ ogs -592 (2) - Basar et al. (2008)
13 012.20 $\rm 4d^45s $ $\rm ^4G_{11/2}$ ogs 699 (5) - Basar et al. (2008)
13 515.20 $\rm 4d^35s^2 $ $\rm ^2F_{7/2} $ lrf 136.9050 (6) -48.916 (14) Fraenkel et al. (1988)

Notes. abmr - atomic beam magnetic resonance technique, lrf - laser radio-frequency double resonance, lif - laser induced fluorescence spectroscopy, ogs - optogalvanic spectroscopy.


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