Table 1: Nd III lines used in the RV and magnetic field analysis of $\gamma$ Equ. The columns give laboratory wavelength, effective Landé factor, excitation potentials and J values of the lower and upper levels.
$\lambda$ (Å) $g_{\rm eff}$ Transition (cm ^-1)

4759.54^bc 1.621 5093₈ - 26098₇

4796.49^bc 1.553 1138₅ - 21981₆

4927.49^a 1.186 3714₇ - 24003₇

4942.68^b 1.479 3714₇ - 23941₆

5012.94^d 1.677 5093₈ - 25036₇

5203.92^ad 0.919 1138₅ - 20349₅

5286.75^a 1.421 5093₈ - 24003₇

5294.11^a 0.615 0₄ - 18884₄

5677.18^a 1.579 5093₈ - 22703₇

5802.54^c 1.531 2387₆ - 19617₅

5845.02^a 1.101 5093₈ - 22197₉

5851.54^c 1.617 3714₇ - 20799₆

5987.68^a 1.163 3714₇ - 20411₇

^a Previously identified and classified Nd III lines.
^b Lines included in Crosswhite's (1976) unpublished list.
^c Lines detected in the laboratory spectrum (Aldénius 2001 and private communication).
^d Reclassified and newly classified lines.

**Table 1:** Nd III lines used in the RV and magnetic field analysis of $\gamma$ Equ. The columns give laboratory wavelength, effective Landé factor, excitation potentials and J values of the lower and upper levels.
$\lambda$ (Å)	$g_{\rm eff}$	Transition (cm ^-1)
4759.54^bc	1.621	5093₈ - 26098₇
4796.49^bc	1.553	1138₅ - 21981₆
4927.49^a	1.186	3714₇ - 24003₇
4942.68^b	1.479	3714₇ - 23941₆
5012.94^d	1.677	5093₈ - 25036₇
5203.92^ad	0.919	1138₅ - 20349₅
5286.75^a	1.421	5093₈ - 24003₇
5294.11^a	0.615	0₄ - 18884₄
5677.18^a	1.579	5093₈ - 22703₇
5802.54^c	1.531	2387₆ - 19617₅
5845.02^a	1.101	5093₈ - 22197₉
5851.54^c	1.617	3714₇ - 20799₆
5987.68^a	1.163	3714₇ - 20411₇

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