Fig. 11

Number of lines overlapping within their thermal Doppler widths
as a function of wavelength. (Only
lines from the lowest three ionization stages, excluding forbidden lines, were
considered for this plot. The overwhelming majority of these lines is from
iron-group elements. The thermal Doppler width was calculated for a representative
element of this element-group using a temperature typical for SN Ia, and is on the
order of 0.01 Å at a wavelength of 1000 Å.) The behavior that up to 70 lines from
different elements of the iron-group dominated SN Ia ejecta overlap per Doppler
width is the origin of a hidden form of deadlock of the lambda iteration used to
solve the multi-level non-LTE problem, and a straightforward lambda iteration will
fail to converge under such circumstances unless special measures are taken.
This lambda iteration deadlock is a general problem because it is solely
based on the fact that a large number of lines overlap within the thermal Doppler
widths of the lines, and this behavior cannot be influenced by choosing
extremely narrow frequency and radius grids, or by choosing a different procedure to
solve the radiative transfer (comoving frame or observer’s frame).
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