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2. Emission line intensities

The emissivity (power per unit volume, erg cm-3 s-1) for an optically thin spectral line at wavelength tex2html_wrap_inline3754 is given by:


equation312

where tex2html_wrap_inline3756s-1) is the Einstein spontaneous emission coefficient (A value); tex2html_wrap_inline3762 is the electron number density (cm-3); Nj(X+m) is the number density of the level j of the ion X+m:


equation324

where tex2html_wrap_inline3772 is the population of level j relative to the total N(X+m) number density of ion X+m and is a function of the electron temperature and density; tex2html_wrap_inline3780 is the ionization ratio of ion X+m which is predominantly a function of temperature; tex2html_wrap_inline3784 is the element abundance relative to hydrogen which varies in different astrophysical plasmas and also in different solar features; tex2html_wrap_inline3786 is the hydrogen abundance relative to electron density (tex2html_wrap_inline3788).

The flux at the Earth (erg cm-2 s-1) in a spectral line is given by:
equation343

where V is the volume of emission and R is the earth-to-object distance.

In low density plasmas the collisional excitation processes are generally faster than ionization and recombination timescales, therefore the collisional excitation is dominant over ionization and recombination in populating excited states. The low lying level populations can then be treated separately from the ionization and recombination processes.

The number density population of level j must be calculated by solving the statistical equilibrium equations for a number of low lying levels and including all the important collisional and radiative excitation and de-excitation mechanisms:


eqnarray349
with tex2html_wrap_inline3800 and tex2html_wrap_inline3802 the electron and proton collisional excitation rate coefficients (cm3 s-1), Rj,i the stimulated absorption rate coefficient (s-1) and Aj,i the spontaneous radiation transition probability (s-1).

In this release of CHIANTI, we do not include proton excitation rates, which are important for fine structure transitions in highly ionized systems. An extensive review of theoretical work, together with recommended data has been compiled by Copeland et al. (1996).

The ratios of emission line intensities provide a multitude of spectroscopic diagnostics for determining the plasma parameters. Extensive reviews have recently been provided by Mason & Monsignori Fossi (1994), Dwivedi (1994) and Doschek (1997),

together with a very useful bibliography by Keenan (1996).


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