Table 1: The computed interaction parameters for the 572 considered levels of Fe II. The complete table is available only electronically at the CDS; a short extract is provided here as a guide to its form. For each level tabulated are: the energy E with respect to the ground state, the parity (EVE or ODD), the J quantum number, the principal quantum number n for the optical electron, the orbital angular momentum quantum number l for the optical electron, the adopted series limit energy $E^{\rm limit}$ , the mean square position of the optical electron $\langle {\rm p}_2^2 \rangle$ , the dispersion coefficient C₆ and the static dipole polarizability $\alpha _{\rm d}$ of the level, and the energy denominator $E_{\rm p}$ . Note that we use the definition $\Delta E = C_6/R^6$ , while Kurucz uses $\Delta \nu = C_6^{\rm KURUCZ}/R^6$ ; thus the definitions differ by a factor of h, in addition to the difference in units.
E Parity J n l $E^{\rm limit}$ $\langle {\rm p}_2^2 \rangle$ C₆ $\alpha _{\rm d}$ $E_{\rm p}$

[cm^-1] [cm^-1] [au] [au] [au] [au]

0.000 EVE 4.5 4 0 130 563.000 8.53 29.73 30.5 -0.574

384.790 EVE 3.5 4 0 130 563.000 8.57 29.73 30.6 -0.577

$\vdots$ $\vdots$ $\vdots$ $\vdots$ $\vdots$ $\vdots$ $\vdots$ $\vdots$ $\vdots$ $\vdots$

**Table 1:** The computed interaction parameters for the 572 considered levels of Fe II. The complete table is available only electronically at the CDS; a short extract is provided here as a guide to its form. For each level tabulated are: the energy E with respect to the ground state, the parity (EVE or ODD), the J quantum number, the principal quantum number n for the optical electron, the orbital angular momentum quantum number l for the optical electron, the adopted series limit energy $E^{\rm limit}$ , the mean square position of the optical electron $\langle {\rm p}_2^2 \rangle$ , the dispersion coefficient C₆ and the static dipole polarizability $\alpha _{\rm d}$ of the level, and the energy denominator $E_{\rm p}$ . Note that we use the definition $\Delta E = C_6/R^6$ , while Kurucz uses $\Delta \nu = C_6^{\rm KURUCZ}/R^6$ ; thus the definitions differ by a factor of h, in addition to the difference in units.
E	Parity	J	n	l	$E^{\rm limit}$	$\langle {\rm p}_2^2 \rangle$	C₆	$\alpha _{\rm d}$	$E_{\rm p}$
[cm^-1]					[cm^-1]	[au]	[au]	[au]	[au]
0.000	EVE	4.5	4	0	130 563.000	8.53	29.73	30.5	-0.574
384.790	EVE	3.5	4	0	130 563.000	8.57	29.73	30.6	-0.577
$\vdots$	$\vdots$	$\vdots$	$\vdots$	$\vdots$	$\vdots$	$\vdots$	$\vdots$	$\vdots$	$\vdots$

Source LaTeX | All tables | In the text

	1 Introduction
	2 Line Broadening calculations
	3 Discussion
	4 Concluding remarks
	References