Emission-line ratios derived from transitions in Fe XVI can be used as
diagnostics
in high-temperature plasmas such as the corona, active regions and flares
(Flower & Nussbaumer 1975;
Vernazza & Reeves 1978;
Dere 1978, 1982; Mason & Monsignori Fossi 1994; Dere et al. 1997;
Brosius et al. 1997a).
Keenan et al.
(1994) have found good agreement between the observed and
theoretical
line ratios when they included the electron excitation rates computed by
Tayal (1994) in their calculations.
Furthermore, spatially resolved EUV emission-line profiles
of this ion can be used to detect velocity fields in the low corona
(Neupert et al. 1992); and simultaneous EUV and radio observations enable
the coronal magnetic field structure to be interpreted
(Brosius et al. 1993, 1997b). Fe XVI emission lines
have also been observed in the EUV spectra of non-supergiant
B stars (Cassinelli 1994), of the eclipsing binary Algol
(Stern
et al. 1995) and of the nearby K2 dwarf Eridani
(Schmitt
et al. 1996).
As a study object of atomic physics Na-like Fe XVI is a fairly simple ion. Hence we use this calculation as a test case to evaluate important effects that must be taken into account when studying electron impact excitation of highly ionized iron-group ions. The ultimate aim of the present work is to produce reliably evaluated collision data for astrophysical applications. With these goals in mind we compare the present results with the two most recent computations for this system: the 10 level close-coupling approximation by Tayal (1994), which takes into account the resonance structure at low energies, and a distorted wave calculation by Cornille et al. (1997). For reviews of earlier work see Badnell & Moores (1994) and Dere et al. (1997).
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