Title: MASS AND ENTROPY PROFILES OF X-RAY BRIGHT RELAXED GROUPS
1MASS 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
2OUTLINE
-
- MASS RESULTS AND c-M PLOT FOR X-RAY GROUPS
- ENTROPY PROFILES
- FOCUS ON SOME PARTICULAR OBJECTS
3DM 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
4c-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
5Selection 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)
6A SPECIAL ERA IN X-RAY ASTRONOMY
- High sensitivity due to high effective area, i.e.
more photons
7Clusters X-ray results
8THE 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.
9SELECTION 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(No Transcript)
11RESULTS
- After accounting for the mass of the hot gas, NFW
stars is the best fit model
MKW 4
NGC 533
12RESULTS
- No detection of stellar mass due to poor sampling
in the inner 20 kpc or localized AGN disturbance
Buote et al. 2002
NGC 5044
13RESULTS
- 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
14c-M relation for groups
We obtain a slope a-0.226?0.076, c decreases
with M at the 3s level
15THE 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
16THE X-RAY c-M RELATION
WMAP 1 yr Spergel et al. 2003
17THE X-RAY c-M RELATION
WMAP 3yr Spergel et al. 2006
18CLUSTERS PREFER HIGH s8
Evrard et al. 2007
19CLUSTERS PREFER HIGH s8
Evrard et al. 2007
20CAVEATS/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)
21MASS 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)
22ENTROPY PROFILES
23ENTROPY PROFILES
24ENTROPY PROFILES
25THE BASELINE INTRACLUSTER ENTROPY PROFILE FROM
GRAVITATIONAL STRUCTURE FORMATION
VOIT ET AL. 2005
26COMPARISON WITH MASSIVE CLUSTERS AND
GRAVITATIONAL SIMULATIONS
PRATT ET AL. 2006
27COMPARISON WITH MASSIVE CLUSTERS AND
GRAVITATIONAL SIMULATIONS
28COMPARISON WITH MASSIVE CLUSTERS AND
GRAVITATIONAL SIMULATIONS
29ENTROPY PROFILES FOR AGN HEATING
VOIT ET AL. 2006
30ENTROPY PROFILES
NGC 4325 AGN DISTURBANCE RUSSELL ET AL. 2007
31ENTROPY PROFILES
32RGH80
33AWM4 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
34AWM4 AND AGN FEEDBACK
35AWM4 AND AGN FEEDBACK
36ENTROPY 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 !)