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Detailed Plasma and Fluorescence Diagnostics of a Stellar X-Ray Flare

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Detailed Plasma and Fluorescence Diagnostics of a Stellar X-Ray Flare. Paola Testa (1) Fabio Reale(2), Jeremy Drake(3), Barbara Ercolano(3), David Huenemoerder(1) ... – PowerPoint PPT presentation

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Title: Detailed Plasma and Fluorescence Diagnostics of a Stellar X-Ray Flare


1
Detailed Plasma and Fluorescence Diagnostics of a
Stellar X-Ray Flare
  • Paola Testa (1)
  • Fabio Reale(2), Jeremy Drake(3), Barbara
    Ercolano(3), David Huenemoerder(1), David
    Garcia-Alvarez(3,4)
  • 1 MIT, 2 Universita di Palermo (Italy), 3 SAO, 4
    Imperial College

July 11 2007 - CXC X-ray spectroscopy workshop
2
Rationale
HETGS observation of the G1 III giant HR 9024
Hertzsprung gap giant, 3M?, 13R?, peak
Lx1032ergs/s
(see also Ayres et al 2007, Nordon Behar 2006)
Motivations
  • X-ray activity in evolved intermediate mass stars
  • Coronal structuring
  • Physics of stellar flares
  • Plasma diagnostics, and geometry diagnostics
  • hydrodynamic loop modeling (Testa et al. 2007,
    ApJ, 663)
  • fluorescence emission

Diagnostic Tools
Comparison of results from the two independent
analyses
July 11 2007 - CXC X-ray spectroscopy workshop
3
HETGS Spectrum
HR 9024 Hertzsprung gap giant, 3M?, 13R?, peak
Lx1032ergs/s
July 11 2007 - CXC X-ray spectroscopy workshop
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Light curve and hardness ratio
HR 9024 Hertzsprung gap giant, 3M?, 13R?, peak
Lx1032ergs/s
July 11 2007 - CXC X-ray spectroscopy workshop
5
X-ray activity of intermediate-mass giants
  • HR 9024 Hertzsprung gap giant, 3M?, 13R?,
    Lx1032ergs/s
  • Evolved intermediate mass star what are the
    characteristics of the X-ray production
    mechanisms? How is the corona structured (typical
    size, filling factors, )? (e.g., Ayres et al.
    1998, Ayres et al. 2007)
  • These giants are thought to develop a dynamo when
    they enter the convective region of the H-R
    diagram, also given their typical fast rotation
    in MS (when they are non-coronal late-B/early-A
    dwarfs)
  • Variability flares are very unusual in these
    massive evolved giants

July 11 2007 - CXC X-ray spectroscopy workshop
6
Hydrodynamic Modeling
  • For the hydrodynamic modeling we use information
    mainly from the continuum that is strong, and it
    probes the hot flaring plasma
  • we derive T and EM by fitting the continuum in
    line-free regions (according to both APED and
    CHIANTI)
  • Loop Model
  • start with an educated guess for the parameters
  • synthesize the HETG spectrum of the solution
  • repeat the analysis carried out on the observed
    spectrum and compare the same quantities
  • refine the model if needed

July 11 2007 - CXC X-ray spectroscopy workshop
7
Hydrodynamic Modeling
MEG cts/s
T
T vs. n
EM
(Testa et al. 2007, ApJ, 663, 1232)
8
Hydrodynamic Modeling
  • Model parameters
  • loop semi-length L 5 1011 cm
  • R?/2, as in normal coronae
  • cross-section radius r 4.5 1010 cm,
    i.e. aspect ratio
    r/L0.1 as in typical solar loops
  • impulsive heating (15 ks starting 8 ks before
    the beginning of the observation) at the
    footpoints volumetric heating 4 erg/cm3/s,
    heating rate 1033 erg/s

July 11 2007 - CXC X-ray spectroscopy workshop
9
Hydrodynamic Modeling
  • Cross-check of results
  • light curves in strong spectral features
  • Fe XXV,
  • Si XIV,
  • Mg XII

(Testa et al. 2007, ApJ)
July 11 2007 - CXC X-ray spectroscopy workshop
10
Hydrodynamic Modeling
  • Cross-check of results
  • EM(T)
  • (flare)

(Testa et al. 2007, ApJ)
July 11 2007 - CXC X-ray spectroscopy workshop
11
Hydrodynamic Modeling
  • Cross-check of results
  • cross-section radius - we derive estimates from
    the normalization of different light curves
  • (a) integrated MEG counts (r 4.9 1010 cm),
  • (b) EM from continuum (r 4.3
    1010 cm),
  • (c) single spectral features (r 4.8 1010
    cm)
  • they all agree with each other within a 15

July 11 2007 - CXC X-ray spectroscopy workshop
12
In the HEG spectrum there is evidence of Fe K?
fluorescence (1.94Å, 6.4keV) that provides an
independent diagnostic for the coronal geometry
Geometry Diagnostics from Fluorescence
HEG
July 11 2007 - CXC X-ray spectroscopy workshop
13
Geometry Diagnostics from Fluorescence
  • the fluorescence efficiency depends on (e.g.,
    Bai 1979)
  • the solid angle subtended by the cold material as
    seen by the X-ray source h
  • the inclination angle at which the reflecting
    surface is viewed by the observer ?
  • the Fe abundance of the cold material

July 11 2007 - CXC X-ray spectroscopy workshop
14
Geometry Diagnostics from Fluorescence
July 11 2007 - CXC X-ray spectroscopy workshop
15
Results
  • the X-ray characteristics of HR9024 are typical
    of normal coronae but scaled up to the larger
    stellar radius
  • HETGS allows for the first time to test HD models
    predictions for single spectral features we find
    very good agreement at least for the hottest
    feature of Fe XXV
  • the HEG spectrum shows evidence of Fe K?
    fluorescence emission, and its analysis provides
    an independent check of the results of the
    hydrodynamic modeling
  • the fluorescence efficiency predicted from the
    HD model is in agreement with the observed one
    within the uncertainties

July 11 2007 - CXC X-ray spectroscopy workshop
16
Thank you!
July 11 2007 - CXC X-ray spectroscopy workshop
17
Hydrodynamic Modeling
  • Cross-check of results
  • light curves in strong spectral features
  • Fe XXV, Si XIV, Mg XII

18
Hydrodynamic Modeling
t0-10ks
Comparison of MEG observed spectrum with
predictions of loop model
t10-15ks
t15-30ks
t30-45ks
19
Hydrodynamic Modeling
t0-10ks
Comparison of MEG observed spectrum with
predictions of loop model
t10-15ks
t15-30ks
t30-45ks
20
Hydrodynamic Modeling
Apex T
Apex ne
max v
Apex p
21
Hydrodynamic Modeling
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