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K. Makishima Cooling Flow, 31 May 2003
The ASCA View on Cooling Flows
and its Implications K. Max Makishima (U. Tokyo /RIKEN)
in collaboration with Yasusi Ikebe, Yasusi Fukazawa, Kyoko Matsushita, Haiguan Xu, Takayuki Tamura, Isao
Takahashi, and Madoka Kawaharada
Makishima et al. PASJ, 53, 401 (2001)
1. ASCA and the Gas Imaging Spectrometer2. Summary of the ASCA Results3. Physics in the “post-CF” Era4. The Prospect for ASTRO-E2
K. Makishima Cooling Flow, 31 May 2003
1. ASCA and the GIS Ohashi et al. PASJ 48, 157 (1996)Makishima et al. PASJ 48, 171 (1996)
0.5 1 2 5 10Energy (keV)
0.1
1e-2
1e-3
1e-4
cts/
sec/
cm2 /
keV
Blanck sky (CXB+NXB)
Sunlit earth (solar X-ray+ NXB) Mg
SiS
Ar
Night earth (NXB)
Cu
GIS background spectra
45 arcmin
Fornax Cluster with the GIS
K. Makishima Cooling Flow, 31 May 2003
0.01
0.1
1
2 3 4 5 6
EM
coo
l /E
M h
ot
Hot component temperature (keV)
A2199
A1795
A21
47
A11
9
A4963A0335
A35
58
A10
60
Hydra-A
A2634
A2063
A40
59
A40
0
MK
W3s
VirgoCen
AWM7
A53
9
AW
M4
A262
2a. The central cool emission is exclusively associated with cD galaxies
cD clusters(B-M I, I-II, or II)
non-cD clusters(B-M II or III)
2. Summary of the ASCA Results
Consistent with previous
knowledge
From 2T fits
K. Makishima Cooling Flow, 31 May 2003
EMcool / EMhot0
0.2
0.4
0.6
0.8
1
0.01 0.1 1
Cen
tral
iron
abu
ndan
ce (
sola
r)
Centaurus
VirgoAWM7A262
A496A2199
A2063
A539A1060A400
cD clustersNon-cD clusters
2b: The cool ICM phase is metal-enriched
- According to the CF scenario, a metal-rich portion would cool and disappear quickly -- a contradiction.
- The chemical abundance of ICM differs between the central and outer regions (Fukazawa et al. MNRAS 313, 21, 2000)
- The cool component appear to be associated with the cD galaxy, rather than with cooling portion of the ICM.
K. Makishima Cooling Flow, 31 May 2003
CF
rat
e w
ith
ASC
A (
M0 /
yr)
A1795
Hydra-A
A2199A496
3A0335
MKW3s
Centaurus
VirgoAWM7
A262
CF rate before ASCA (M0 /yr)
- Hot emission from the cluster core was mistaken for the cool emission.
- The central potential “dimple” was not properly considered.
100101
10
100- Ikebe et al. (1997)- Xu et al. (1998)- Ikebe et al. (1999)- Makishima et al (2001)
Reconfirmed with Chandra and XMM-Newton
2c. The CF rate was previously overestimated
A good example will be given by the next speaker
K. Makishima Cooling Flow, 31 May 2003
Projected radius (arcmin)101
ASCA GIS 0.7-3 keV
101
ASCA GIS 3-10 keV
Beta model(convolved)
100 kpc
The central excess surface brightness is nearly color-independent (A1795; Xu et al. Ap
J 500,738, 1998).
2d. The centrally peaked surface brightness is due to central potential deepening
Sur
face
bri
ghtn
ess
(a.u
.)
1-beta fits(95 clusters)
2-beta fits(26 clusters)
15
10
5
0
8
6
4
2
00.03 0.1 0.3 1 Core radius (Mpc)
Num
ber
60 kpc
220 kpc
The ICM profile involve two spatial scales (ROSAT+ASCA; Ota et al. A
pJL 567, L23, 2002) .
K. Makishima Cooling Flow, 31 May 2003
2e. The central cool component traces the central potential deepening
Ikebe astroph/0112132
ASCA
A1795
EPIC-MOSEPIC-PN
8
6
4
2Tem
pera
ture
(ke
V)
0.1 0.2 0.5 1 2 5 10Projected radius (arcmin)
Tcool ~ Thot / 2, with a common radial temperature profile (Ikebe astro-ph/0112132 ; Allen et al. MNRAS 328, L37, 2001)
44
43
42
41
40 1 2 5 10
Temperature (keV)
Log
LX (
e rg /
s )Cool component
obeys the same Lx-T relation as the entire
cluster sample
Most detailed 2T analysis: Ikebe et al. ApJ 525, 58 (1999) Tcool may simply reflect the central potential depth
An isothermal hot ICM fills the entire potential well.
A two-phase region is produced within the central potential dimple, by an
admixture of metal-rich cool plasma.
A hierarchical potential is formed by the cluster and the cD galaxy.
2f. The ASCA view of a cD cluster -- “Double-beta” and “2T” (Ikebe et al. ApJ, 525, 58,1999)
K. Makishima Cooling Flow, 31 May 2003
3b. Simple-minded considerations
3a. Conclusion from Makishima et al. (2001)
Through the ASCA study, we have arrived at a novel view on central regions of galaxy clusters. It describes the region around a cD galaxy as a site of significant and active evolution, where plenty of heavy elements are produced, a self-gravitating core develops, the stellar component condensates to the center, and the liberated energy is deposited onto the X-ray emitting plasmas. The scenario makes a sharp contrast to the previous view which emphasized the role of radiative plasma cooling. Novel X-ray information to be available with Chandra, XMM-Newton, and hopefully the rebuilt ASTRO-E will be utilized for further examination of our scenario.
Through the ASCA study, we have arrived at a novel view on central regions of galaxy clusters. It describes the region around a cD galaxy as a site of significant and active evolution, where plenty of heavy elements are produced, a self-gravitating core develops, the stellar component condensates to the center, and the liberated energy is deposited onto the X-ray emitting plasmas. The scenario makes a sharp contrast to the previous view which emphasized the role of radiative plasma cooling. Novel X-ray information to be available with Chandra, XMM-Newton, and hopefully the rebuilt ASTRO-E will be utilized for further examination of our scenario.
3. Physics in the “Post-CF” Era
K. Makishima Cooling Flow, 31 May 2003
3b. A simple idea (Makishima 1994)
- ICM, DM, and galaxies have ~ the same specific energy.
- Since alaxies have much lower specific entropy than ICM, the free energy will be transferred from galaxies to ICM.
- Galaxies will lose energy and fall to the cluster center.
High z Low z
Evolution?
K. Makishima Cooling Flow, 31 May 2003
3c. Supporting evidence- In angular extent, stars < DM < I
CM -- Energy of the galaxies was transferred to the ICM.
- Evidence for gradual galaxy mergers in the cluster center -- Dynamical energy of galaxies was extracted, and was deposited on the ICM.
--> Poster #17. “The Dark Group Candidate, RXJ 0419+2225” by Kawaharada et al.
- The central decrease in Iron-Mass-to-Light -Ratio (IMLR) -- Galaxies gradually fell to the center while ejecting metals.
20 50 100 200 300
IML
R
Centaurus
0.01
1e-3
1e-4
A1060
3D radius (kpc)
Radial IMLR profiles
- The O-profile is flatter than the Fe-profile -- Early SNe II occurred over an extended region, while subsequent SNe Ia occurred closer to the center.
K. Makishima Cooling Flow, 31 May 2003
3d. Numerical estimates- The expected galaxy-to-ICM energy transfer rate ;
-dE/dt ~ N Ri2 n mpv3 (Sazazin 1988, p.152)
~ 2x1044 (N /300) (Ri /10kpc) 2 (n/10-3) (v/500 kms-1)3 erg/s
(N=galaxy number; Ri= interaction radius; n=ICM density; v=galaxy velocity dispersion)
- The intra-cluster magnetic fields are easily “pushed away” by moving galaxies that are good electrical conductors. This makes Ri ~ DM halo of each galaxy.
- The available total dynamical energy in galaxies;
E ~ 5x1062 (Mgal /1014 M0) (v/500 kms-1)2 ergs
E/(dE/dt) ~ 80 Gyr
K. Makishima Cooling Flow, 31 May 2003
Reconnection sites
Hot phase
Cool phase
Magnetic field lines
Galaxy motion/rotation
- Ordered magnetic fields separate the hot and cool phases.- Galaxies’ kinetic energy --> MHD turbulence -->
reconnection --> plasma heating & particle acceleration- The loop-like structure stabilizes the heating/cooling.
3c. A speculative view -- the “cD corona”
4. The Prospect for ASTRO-E2The first improved version of the
M-5 rocket has been launched successfully on 2003 May 9,
putting “Sample-Return” mission into an interplanetary orbit.
We are re-building the Hard X-ray Detector (HXD).
The recovery mission ASTRO-E2 will be launched in 2005.
- The XRS (D measures the expected ICM turbulence.
- The HXD (10-600 keV) searches for particle acceleration.
- The XIS (CCD camera) studies the ICM heating process.
K. Makishima Cooling Flow, 31 May 2003
Conclusion- - Using ASCA, we have pointed out for the first
time that the CF hypothesis needs a significant revision.
- - The view has been reinforced by XMM-Newton and Chandra.
- - We propose that the dynamical energy in the galaxy motion is dissipated onto the ICM.
- - ASTRO-E2 will open the new era of such post-CF physics.