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Abundance studies using Xray spectroscopy of clusters of galaxies

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Hard to discriminate between Ia models, but see extremes Hydra A / M87 ... Similar results in Hydra A. 4. Enrichment by winds. XMM-Newton RGS results ... – PowerPoint PPT presentation

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Title: Abundance studies using Xray spectroscopy of clusters of galaxies


1
Abundance studies using X-ray spectroscopy of
clusters of galaxies
  • Jelle S. Kaastra
  • Collaborators
  • Norbert Werner, Jelle de Plaa,
  • Aurora Simionescu, Jacco Vink

2
Outline
  • Importance clusters
  • Observational challenges
  • Enrichment by supernovae
  • Enrichment by winds
  • Future prospects
  • Conclusions

3
1. Importance clusters of galaxies for abundance
studies
  • Largest bound structures
  • Fair samples of the Universe
  • Deep potential wells, retains most of the gas
  • Hot gas no significant hiding of metals in
    dust ( more gas than stars)?
  • Spatial extent allows mapping

4
Abundance diagnostics hot gas in collisional
ionisation equilibrium
T 1 keV
T 0.2 keV
T 5 keV
5
Which elements can we see?
K-shell

6
Powerful X-ray eyes XMM-Newton
  • 3 imaging CCDs (EPIC) with moderate energy
    resolution
  • 2 Reflection Grating Spectrometers (RGS) with
    high spectral resolution

7
2. Observational challenges
  • Fe bias
  • Complex temperature structure

8
The Fe bias
Multi-T
1T
  • 1T models sometimes too simple e.g. in cool
    cores
  • Using 1T gives biased abundances (Fe-bias, Buote
    2000)?
  • Example core M87 (Molendi Gastaldello 2001)?

9
Complex temperature structure I(de Plaa et al.
2006)?
  • Sérsic 159-3, central 4 arcmin
  • Better fits 1T?wdem?gdem
  • Implication for Fe 0.36?0.35?0.24
  • Implication for O 0.36?0.30?0.19

10
Temperature maps(Hydra A, Simionescu et al.
2008)?
11
Complex temperature structure II(Simionescu et
al. 2008)?
  • Example Hydra A
  • Central 3 arcmin
  • Full spectrum Gaussian in log T (s0.2)?
  • 1T fits individual regions also Gaussian
  • Confirmed by DEM analysis (blue purple)?

12
Implications for Fe abundance(Simionescu et al.
2008)?
  • Central 3 arcmin Hydra A, 1T models
  • (errors on Fe 0.01 to 0.02)?

13
3. Enrichment by supernovae
14
Supernova yields core collapse
15
Supernova yields Ia
16
Decomposing abundances into SN types(De Plaa et
al. 2006)?
  • Deep exposure XMM-Newton Sérsic 159-3
  • Data include RGS
  • 50 SN Ia by number
  • Ca problem

17
Another case 2A 0335096(Werner et al. 2006)?
  • Current best case deep XMM-Newton observation of
    one of brightest clusters
  • First evidence of traces of Cr (0.50.2 Solar)?

2A 0335096, Werner et al. 2005
18
Decomposing 2A 0335096(Werner et al. 2006)?
  • Use here WDD model
  • Central 3 arcmin
  • Sn Ia 25
  • Increases to 37 in 3-9 arcmin annulus
  • Ni W7 model predicts more
  • Also here Ca problem

19
Analysis of a large sample (De Plaa et al. 2007)?
  • 22 clusters, 685 ks net exposure
  • Taken from HIFLUGCS sample (Reiprich Böhringer
    2002)?
  • All spectra extracted from within 0.2 R500
  • Use wdem model

20
Solution to the Ca problem(De Plaa et al. 2007)?
  • Also sample shows Ca excess
  • Problem solved by adopting SN Ia yields based on
    Tycho SNR (Badenes et al. 2006)?
  • Best fit Ia/(Iacc) number ratio 0.440.05

WDD
Tycho
21
Sample mean abundance ratios(De Plaa et al.
2007)?
22
Comparison between clusters(Simionescu et al.
2008)?
  • 6 clusters with deep exposures, taken from
    literature
  • Most have 30-40 contribution Ia
  • Hard to discriminate between Ia models, but see
    extremes Hydra A / M87

23
Radial profiles example 2A 0335096(Werner et
al. 2006)?
S
Si
Fe
Ar
24
Comparison between clusters radial
profiles(Simionescu et al. 2008)?
  • All elements have decreasing abundances
  • Also valid for O (contrary to earlier suggestions
    of flat O profile, Tamura et al. 2004)?

25
Abundance ratios constant? (Simionescu et al.
2008)?
  • Si/Fe flat within 0.1 R200, maybe break at
    0.05R200
  • O/Fe increases, but only slightly per dex in
    radius, O/Fe increases by 0.250.09 (Fe decreases
    by 0.72)?

Si/Fe
O/Fe
26
Consequences of flat oxygen profiles(Simionescu
et al. 2008)?
  • Flattish O/Fe profiles ? not only Ia contribute
    to core enrichment
  • Ram pressure stripping works already at Mpc scale
    (compare to 130 kpc core Hydra A)?
  • Continued cc SN activity over past 1010 year?
  • Early central enrichment cc SN?

27
Cosmic feedback(Simionescu et al. 2006, 2007)?
  • In M87, radio lobes show cool, enriched material
    levitated by the AGN outflow
  • Similar results in Hydra A

28
4. Enrichment by winds
29
XMM-Newton RGS results
  • Reflection Grating Spectrometer optimal for point
    sources
  • But still the best for moderately extended
    sources, like cooling cores of clusters
  • ?? (Å) 0.138 ?? (arcmin)?

30
RGS results M 87(Werner et al. 2006)?
  • Exposure time 169 ks
  • Lines from O, N, C
  • C/Fe 0.740.13
  • N/Fe 1.620.21
  • O/Fe 0.590.04
  • Ne/Fe 1.250.12
  • Mg/Fe 0.600.06
  • Fe 1.060.03
  • ? AGB winds for CN!

Continuum-subtracted RGS spectrum
31
Nitrogen with RGS other cases
  • M87 N/Fe 1.620.21
  • 2A 0335096 (Werner et al. 2006) 1.30.4
  • Sérsic 159-3 (De Plaa et al. 2006) 0.00.5
  • Centaurus (Sanders et al. 2008) 1.5-3
  • Need for more deep exposures with RGS

32
Groups of galaxies
  • O/Fe ratio 0.5-0.6 x Solar in 4 groups
  • N/Fe 1.1-1.2 x Solar in NGC 4472 NGC 4636, but
    1.6 in M87
  • Need more data this year deeper spectra of NGC
    5044 NGC 5813

33
5. Future prospects
  • Long term XEUS (ESA), Con-X (NASA) gt2018 (30 x
    effective area EPIC, resolution RGS, imaging)?
  • Mid-term NeXT (Japan) 2013/14
  • Short term (2011-2012)
  • SXC (SpektrRG X-ray Calorimeter
  • (Netherlands, USA, Japan, Germany, Russia)?

34
Future SXC
35
SXC Measuring clusters ISM simultaneously
36
How accurate can we getcomparison XMM-Newton
with SXC
37
Which elements will we see?(XEUS)?
K-shell

38
6. Conclusions
  • XMM-Newton observations of clusters of galaxies
    can disentangle contributions different SN types
    in clusters of galaxies
  • In a few cases, CN abundances can be measured
    also
  • After 2012, we will have a new generation of
    instrumentation allowing more and more accurate
    abundance measurements
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