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Recent advances in the CHIANTI database in the Xray range

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Title: Recent advances in the CHIANTI database in the Xray range


1
Recent advances in the CHIANTI database in the
X-ray range
Enrico Landi
Naval Research Laboratory
2
Overview
  • Introduction
  • What is CHIANTI
  • New features of the CHIANTI database
  • Comparison with X-ray observations
  • Conclusions

3
Introduction
  • X-ray spectra are of primary importance for
    quantitative studies of the physics of many
    astrophysical objects
  • Emission and absorption of line and continuum
    radiation in the X-rays offer a wide variety of
    diagnostic tools to determine the physical
    properties of emitting sources
  • For this reason, in the recent past, several
    instruments have been flown to observe
    astrophysical sources in the X-ray range
  • Chandra ROSAT
  • XMM Yohkoh
  • RHESSI SMM
  • RESIK and many others

4
Why a database?
  • X-ray spectra are composed by line and continuum
    radiation, emitted by highly charged ions.
  • Observed X-ray spectral lines come from
  • Rydberg series in the H-,He-like sequences
  • High-energy configurations (ngt2) in highly
  • charged Fe and Ni ions
  • Innershell transitions
  • Dielectronic satellite lines
  • Continuum radiation comes from
  • Free-free radiation
  • Free-bound radiation

5
  • In order to study this radiation and use it for
    plasma diagnostic purposes, a large amount of
    atomic data are needed for both line and
    continuum radiation
  • To address this need, several databases have been
    created in the past
  • CHIANTI
  • MEKAL
  • APEC/APED
  • ADAS
  • Arcetri Spectral Code

6
Requirements for a database
  • In order to be suitable for the analysis of
    modern high-resolution spectra, atomic data bases
    need to
  • - be complete no lines left behind
  • - be accurate plasma diagnostics not
    hindered by atomic physics
    uncertainties
  • - be easy-to-use
  • - be transparent - the user can independently
    check the original data and their accuracy
  • - no black box
  • - all data independently refereed in peer
  • reviewed literature
  • Also, atomic data and predicted emissivities from
    data bases need to be benchmarked against
    observations

7
The CHIANTI database
  • CHIANTI consists of
  • A database of atomic data and transition rates
  • A suite of IDL programs for plasma diagnostics
  • CHIANTI is able to calculate
  • Line emissivities for more than 230 ions
  • innershell transitions
  • dielectronic satellite lines
  • Continuum emissivities for free-free
    radiation
  • free-bound radiation
  • two-photon continuum
  • Under the optically thin plasma assumption

8
  • CHIANTI data are
  • In ASCII format
  • Selected from the refereed literature (no
    unpublished data)
  • With references to original literature
  • CHIANTI is completely transparent to the end
    user
  • FREELY available on the web at
  • http//wwwsolar.nrl.navy.mil/chianti.html
  • Fully documented through user guides
  • CHIANTI also maintains a mailing list
  • email assistance to users at
  • chianti_help_at_halcyon.nrl.navy.mil

9
  • CHIANTI has enjoyed great success in the
    astrophysical community. CHIANTI data have been
  • Included in the software of several satellite
    borne missions
  • SOHO/CDS (EUV)
  • SOHO/EIT (EUV)
  • TRACE (UV)
  • Solar-B (EUV,X-rays)
  • STEREO (EUV)
  • RHESSI (X-rays)
  • Included in other spectral codes
  • APEC/APED
  • PintOfAle
  • Arcetri Spectral Code
  • ADAS

10
State-of-the-art
  • Literature data for the X-rays have several
    limitations
  • Missing configurations (ngt3 in many Fe ions)
  • Limited atomic models for n3 configurations
    (usually due
  • to computer memory limitation in the past)
  • Missing processes
  • resonances
  • ionization effects on level populations
  • recombination effects on level populations
  • cascades from higher levels
  • Uncertainties in line identifications

11
CHIANTI 5.0
  • The CHIANTI database has been recently greatly
    expanded. The main features of the next CHIANTI
    release (Version 5.0) are
  • New data for high-energy configurations in Fe
    XVII-XXIII
  • n3,4,5,6,7 Fe XVII
  • n3,4,5 Fe XVIII-XXIII
  • New data for satellite lines
  • Ionization and recombination effects in level
    populations
  • Complete re-assessment of energy levels and line
    identifications
  • Other data and new ions for EUV and UV lines

12
New data for high-energy configurations in Fe
XVII-XXIII
  • We have made use of the Flexible Atomic Code, by
    Dr. M.F. Gu, to calculate
  • Energy levels
  • Radiative transition rates
  • Collisional transition rates (including
    resonances)
  • for all configurations with
  • n3,4,5,6,7 Fe XVII
  • n3,4,5 Fe XVIII-XXIII
  • These data allow to predict lines in the 7-12
    Angstrom range
  • Few if any data were available in the literature
    for most of these configurations
  • Data will be published separately (Landi Gu
    2005)

13
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14
New data for satellite lines
  • New data have been added to CHIANTI 5.0 for
    dielectronic satellite lines and innershell
    transitions, to match observations
  • Fe XXIII innershell transitions
  • S XVI, Ca XVIII, Fe XXIV dielectronic
    satellite lines
  • These new lines also provide diagnostic tools for
    measuring the plasma electron temperature
  • These lines allow to study RHESSI spectra in the
    6-9 keV energy range

15
Fe XXV
Fe XXV
Fe XXV
Fe XXIV satellites
Fe XXIV satellites
Fe XXIV satellites
16
Ionization and Recombination
  • Recently, Behar Doron (2002) and Gu (2003)
    demonstrated that ionization and recombination
    are important contributors to steady-state level
    population in highly ionized Fe ions
  • CHIANTI 5.0 incorporates data and software to
    take these two processes into account
  • All recombination and ionization data have been
    taken from the Flexible Atomic Code calculations
    by Gu (2003).

17
  • We make use of the Coronal Model Approximation
  • Without Ionization/Recombination
  • With Ionization/Recombination
  • Where nq-1, nq, nq1 ion fractions
  • CI, REC total ion. and rec. rates
  • Egi total excitation rate level i
  • Dig total de-excitation rate level i

18
  • The Coronal Model Approximation is not valid if
    metastable levels have non-negligible population
  • As the electron density increases, the population
    of metastable levels in highly ionized Fe ions
    also increases
  • The maximum density at which metastable level
    populations are negligible changes from ion to
    ion
  • Ion Log Ne(max)
  • Fe XVII any
  • Fe XVIII gt 13
  • Fe XIX 12
  • Fe XX 12
  • Fe XXI 12
  • Fe XXII 13
  • Fe XXIII gt 13
  • Fe XXIV any

19
Fe XVII
Fe XVIII
Fe XX
Fe XIX
20
Fe XXI
Fe XXII
Fe XXIV
Fe XXIII
21
Comparison with X-ray observations
  • We have compared the new CHIANTI 5.0 with
    observations of a moderate solar flare
  • Instrument SMM/FCS (Bragg crystal
    spectrometer)
  • Date of observation August 25, 1980
  • Wavelength ranges 13.1-22.4 A (channel 1)
  • 10.6-14.9 A (channel 2)
  • 7.3-10.1 A (channel 3)
  • Spectral resolution 1-20 mA (depending on the
    channel)
  • Source M 1.5 flare
  • Spectral scan Duration 17.5 minutes
  • Ions observed H-like O,Ne,Mg
  • He-like O,Ne,Na,Mg,Al
  • Fe ions Fe XVII to Fe XXIII
  • Ni ions Ni XIX, Ni XX

22
Comparison method
  • FCS spectra were not observed simultaneously, so
    the flare plasma was analyzed as a function of
    time
  • The Emission Measure analysis showed that
  • The flare plasma was isothermal
  • The temperature was decreasing slowly
  • The emission measure decreased by a factor 6
    during the observation
  • This allowed us to use the Emission Measure as a
    tool to compare CHIANTI 5 emissivities and
    observed fluxes for each ion, to
  • Assess the quality of CHIANTI 5 data
  • Identify blends from other ions and evaluate
    their contribution to the total intensity
    (additional check on atomic physics)
  • Identify areas where improvements are still needed

23
  • In case of isothermal plasma
  • We can define, for all the lines of the same ion,
    the ratio
  • If there are no blends and no atomic physics
    problems, all the ratios must be the same at all
    temperatures, within the uncertainties.

24
Example Fe XIX
CHIANTI 5
CHIANTI 4.2
Time bin 1
Time bin 2
25
Example Fe XVII
  • Long standing problems
  • Strong 15.01 A line lower than predicted
  • Resonant scattering?
  • Satellites in 15.01/15.26 intensity ratios?
  • Disagreement in 2p-3s/2p-3d ratios
  • Innershell ionization to 3s?
  • Satellite contributions to line ratios?
  • Existing atomic data
  • DW collision rates from many authors
  • Only very recently resonance data have been
    considered
  • Doron Behar (2002) showed that recombination is
    important for Fe XVII

26
  • We used CHIANTI 5.0 to check the importance of
    many additional processes in Fe XVII level
    population
  • Process Importance
  • Cascades Moderate
  • Collisional ionization Moderate
  • Recombination Crucial
  • Resonances Crucial
  • We have compared the FCS spectrum with CHIANTI
    5.0 predictions obtained with and without those
    processes

27
CHIANTI 4.2
15.01 A
CHIANTI 5.0
15.01 A
28
Results and Conclusions
  • CHIANTI 5.0 reproduces observed high- and low-
    resolution X-ray spectra with great accuracy
  • All relevant configurations in Fe ions are now
    included
  • Blending from ions of different species is
    accounted for
  • Most lines are reproduced within 30
  • CHIANTI 5.0 represents a major advance over
    previous versions and other databases
  • New diagnostic tools are now available to measure
    the physical properties of the emitting plasmas
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