Many astrophysical emission line spectra are
produced by the
collisional excitation of a variety of ionization
stages of elements
commonly found in cosmic plasmas. Their
interpretation requires an
accurate knowledge of the atomic structure of
these ions and their
excitation and emission rates (Mason &
Monsignori Fossi 1994). In
the past a number of spectral codes have been
constructed to aid in the
interpretation of astrophysical spectra.
Examples include those of
Landini & Monsignori Fossi (1970,
1990), Tucker
& Koren (1971), Mewe
(1972), Mewe & Gronenschild
(1981),
Mewe et al. (1985),
Kato (1976),
Raymond & Smith (1977),
Stern et al. (1978), and
Gaetz & Salpeter
(1983). A comparison and critique of
different plasma emission codes
for X-ray and UV spectra is published by
Mason (1996a). Many of these
codes were assembled at a time when the necessary
atomic data such
collision strengths were often lacking. Often
the formula
(Van Regemorter 1962), or
variations, were used to estimate electron
excitation rates. Because of the increasing
power of computer
technology, reliable calculations of many of
these excitation rates are
continually becoming available.
Recent papers have attempted to provide more accurate representations for the atomic parameters, in particular for the iron ions (cf. Brickhouse et al. 1995; Monsignori Fossi & Landini 1994a; Mewe et al. 1995).
The basic goal for the CHIANTI database is to construct a database that includes the best available calculations of atomic parameters for analyzing astrophysical emission line spectra. In implementing the database, we also tried to achieve several other goals: 1. the database could be readily updated, 2. the database would be easy to distribute, 3. it would be transparent to the end user, 4. accuracy would be maintained by visually examining as much of the input data as possible, 5. it would use a data and programming structure that would facilitate the development of programs by end users.
The basic unit of the data base is the individual
ion. For each ion
there is a directory that contains a file
specifying its energy levels,
a file providing wavelengths and radiative rates,
and a file providing
fits to the collision strengths which give the
electron excitation
rates. Each file contains information on the
source of the data and
other relevant comments. The energy level
information is largely taken
from the NIST database of observed energy levels
(Martin et al. 1995),
updated by more recent observed values and
supplemented by our best
theoretical estimates where energy levels are not
known. Radiative
data are obtained from available publications and
supplemented where
necessary by new calculations. Collision
strengths ('s) and
upsilons (
's - collision strengths
averaged over a Maxwellian
velocity distribution) have all been visually
inspected and scaled
according to the formulation of Burgess &
Tully (1992). Elemental
abundances can be freely specified and the
ionization equilibrium is
determined from steady state calculations, for
which the Arnaud &
Rothenflug (1985) calculation is supplied.
At the present time, the database is capable of reproducing the optically thin emission line spectrum at wavelengths greater than 50 Å for electron densities less than about 1015 cm-3. The ions necessary to calculate the spectrum below 50 Å will be developed in the near future. There is no long wavelength limit to the database but, in a practical sense, it becomes less comprehensive at longer wavelengths because neutrals are not included. The scaling of the upsilons should be accurately reproducible for nearly any range of temperature. Astrophysically abundant elements from hydrogen through nickel are included. Tables 1 (click here) and 2 (click here) show which ions are currently included in the CHIANTI database.
Ion | I | II | III | IV | V | VI | VII | VIII | IX | X | XI | XII | XIII | XIV | XV | XVI |
H | ||||||||||||||||
He | ![]() | |||||||||||||||
C | ![]() | ![]() | ![]() | |||||||||||||
N | ![]() | ![]() | ![]() |
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O | ![]() | ![]() | ![]() |
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Ne | ![]() | ![]() | ![]() |
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Mg | ![]() | ![]() | ![]() |
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Al | ![]() | ![]() |
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Si | ![]() | ![]() | ![]() |
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S | ![]() | ![]() | ![]() |
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Ar | ![]() | ![]() |
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Ca | ![]() | ![]() | ![]() | ![]() | ![]() |
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Fe | ![]() | ![]() |
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Ni |
![]() |
Ion | XVII | XVIII | XIX | XX | XXI | XXII | XXIII | XXIV | XXV | XXVI | XXVII | XXVIII |
Ar | ||||||||||||
Ca | ![]() | ![]() | ||||||||||
Fe | ![]() | ![]() | ![]() |
![]() | ![]() | ![]() | ![]() |
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Ni | ![]() | ![]() | ![]() |
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A package of programs written in Interactive Data Language (IDL) are also supplied. These allow the calculation of level populations, synthetic spectra, and density and temperature sensitive line ratios. Because of the nature of the database, further capabilities and interfaces to other programming languages, such as Fortran or C, can be readily implemented in the future. The package is freely available for downloading over the internet. The CHIANTI database and accompanying IDL routines have been incorporated into the scientific analysis software for the Coronal Diagnostic Spectrometer onboard the Solar and Heliospheric Observatory (SOHO) by C.D. Pike and G. Del Zanna.