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MASS AND ENTROPY PROFILES OF X-RAY BRIGHT RELAXED GROUPS

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Title: MASS AND ENTROPY PROFILES OF X-RAY BRIGHT RELAXED GROUPS


1
MASS AND ENTROPY PROFILES OF X-RAY BRIGHT RELAXED
GROUPS
FABIO GASTALDELLO UC IRVINE BOLOGNA D. BUOTE
P. HUMPHREY L. ZAPPACOSTA J. BULLOCK W. MATHEWS
UCSC F. BRIGHENTI BOLOGNA
2
OUTLINE
  • MASS RESULTS AND c-M PLOT FOR X-RAY GROUPS
  • ENTROPY PROFILES
  • FOCUS ON SOME PARTICULAR OBJECTS

3
DM DENSITY PROFILE
The concentration parameter c do not depend
strongly on the innermost data points, r lt 0.05
rvir (Bullock et al. 2001, B01 Dolag et al.
2004, D04).
Navarro et al. 2004
4
c-M RELATION
  • c slowly declines as M increases (slope of -0.1)
  • Constant scatter (slogc 0.14)
  • the normalization depends sensitively on the
    cosmological parameters, in particular s8 and w
    (D04,Kuhlen et al. 2005).

Bullock et al. 2001
5
Selection Effects
Wechsler et al. 2002
Concentrations for relaxed halos are larger by
10 compared to the whole population (Jing 2000,
Wechsler 2002, Maccio 2006). They show also
smaller scatter (slogc 0.10)
6
A SPECIAL ERA IN X-RAY ASTRONOMY
  • High sensitivity due to high effective area, i.e.
    more photons
  • 1 arcsec resolution

7
Clusters X-ray results
8
THE PROJECT
  • Improve significantly the constraints on the c-M
    relation by analyzing a wider mass range with
    many more systems, in particular obtaining
    accurate mass constraints on relaxed systems with
    1012 M 1014 Msun
  • There are very few constraints on groups scale
    (1013 M 1014 Msun) , where numerical
    predictions are more accurate because a large
    number of halo can be simulated.

9
SELECTION OF THE SAMPLE
  • In Gastaldello et al. 2007 we selected a sample
    of 16 objects in the 1-3 keV range from the XMM
    and Chandra archives with the best available data
    with
  • no obvious disturbance in surface brightness at
    large scale
  • with a dominant elliptical galaxy at the center
  • with a cool core
  • with a Fe gradient
  • The best we can do to ensure hydrostatic
    equilibrium and recover mass from X-rays.

10
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11
RESULTS
  • After accounting for the mass of the hot gas, NFW
    stars is the best fit model

MKW 4
NGC 533
12
RESULTS
  • No detection of stellar mass due to poor sampling
    in the inner 20 kpc or localized AGN disturbance

Buote et al. 2002
NGC 5044
13
RESULTS
  • NFW stars best fit model
  • We failed to detect stellar mass in all objects,
    due to poor sampling in the inner 20 kpc or
    localized AGN disturbance. Stellar M/L in K band
    for the objects with best available data is
    0.57?0.21, in reasonable agreement with SP
    synthesis models ( 1)
  • Adopting more complicated models, like
    introducing AC or N04 did not improve the fits.
    AC produces too low stellar mass-to-light ratios

14
c-M relation for groups
We obtain a slope a-0.226?0.076, c decreases
with M at the 3s level
15
THE X-RAY c-M RELATION
  • Buote et al. 2007
  • c-M relation for 39 systems ranging in mass
    from ellipticals to the most massive galaxy
    clusters (0.06-20) x 1014 Msun.
  • A power law fit requires at high significance
    (6.6s) that c decreases with increasing M
  • Normalization and scatter consistent with relaxed
    objects

16
THE X-RAY c-M RELATION
WMAP 1 yr Spergel et al. 2003
17
THE X-RAY c-M RELATION
WMAP 3yr Spergel et al. 2006
18
CLUSTERS PREFER HIGH s8
Evrard et al. 2007
19
CLUSTERS PREFER HIGH s8
Evrard et al. 2007
20
CAVEATS/FUTURE WORK
  • HE (10-15 from simulations, e.g. Nagai et al.
    2006, Rasia et al. 2006). No results yet on the
    magnitude for the bias on c (if there is one) due
    to radial dependence of turbulence
  • Selection bias
  • Semi-analytic model prediction of c-M
  • Gas physics and AC (problems also with rotation
    curves of spirals Kassim et al. 2006, Gnedin et
    al. 2006 but also positive claims M31 mass model
    of Seigar et al. 2007)
  • Extend the profiles at large radii (r500 is
    possible to reach for groups)

21
MASS CONCLUSIONS
  • The crucial mass regime of groups has provided
    the crucial evidence of the decrease of c with
    increasing M
  • c-M relation offers interesting and novel
    approach to potentially constrain cosmological
    parameters
  • See constraints on the c-z relation (poster by L.
    Zappacosta)

22
ENTROPY PROFILES
23
ENTROPY PROFILES
24
ENTROPY PROFILES
25
THE BASELINE INTRACLUSTER ENTROPY PROFILE FROM
GRAVITATIONAL STRUCTURE FORMATION
VOIT ET AL. 2005
26
COMPARISON WITH MASSIVE CLUSTERS AND
GRAVITATIONAL SIMULATIONS
PRATT ET AL. 2006
27
COMPARISON WITH MASSIVE CLUSTERS AND
GRAVITATIONAL SIMULATIONS
28
COMPARISON WITH MASSIVE CLUSTERS AND
GRAVITATIONAL SIMULATIONS
29
ENTROPY PROFILES FOR AGN HEATING
VOIT ET AL. 2006
30
ENTROPY PROFILES
NGC 4325 AGN DISTURBANCE RUSSELL ET AL. 2007
31
ENTROPY PROFILES
32
RGH80
33
AWM4 AND AGN FEEDBACK
In this scenario there is a clear dichotomy
between active and radio quiet clusters one
would expect the cluster population to bifurcate
into systems with strong temperature gradients
and feedback and those without either
Donahue et al. 2005
34
AWM4 AND AGN FEEDBACK
35
AWM4 AND AGN FEEDBACK
36
ENTROPY CONCLUSIONS
BROKEN POWER LAW ENTROPY PROFILES FOR GROUPS WITH
STEEPER INNER SLOPES AND FLATTER OUTER SLOPES
SEEM TO POINT TO HIGHER IMPORTANCE OF LOCAL AGN
HEATING INTERPLAY BETWEEN AGN AND MERGINGS THE
PUZZLE AWM4 (MORE DATA RADIO, POSTER BY S.
GIACINTUCCI, CHANDRA !)
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