clusters of galaxies cosmology - lund observatory · galaxies. there is a “clusters” working...
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CLUSTERS of GALAXIES &
COSMOLOGY
Cathy Horellou, Onsala Space Observatory, Chalmers University of Technology, Sweden
Introduction
– Clusters as cosmological tools
– Probes, processes,
& the importance of systematics
Sunyaev-Zelʼdovich observations
Radio synchrotron from clusters (LOFAR...)
XXL: The Ultimate XMM Extragalactic Survey
My own interests
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Vikhlinin et al. 2009 Tuesday, February 5, 2013
Credit: The Virgo consortium, 1996
Observations of clusters make it possible to– measure the growth of structure in the expanding Universe– constrain the cosmological parameters
Ex: The observation of 1 single massive cluster at z = 0.8 (MS1054-0321) made it possible to exclude Ωm > 1 (Jetlema et al. 2001)
Ωm = 1
Numerical simulations of structure formation (dark matter only)
170 Mpc
200 Mpc
Ωm = 0.3ΩΛ = 0.7
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Figure: Horellou & Berge 2005, MNRAS
Cluster number countsin different dark energy models
w = p/ρ : equation-of-state parameter of dark energyw = – 1 (ΛCDM)w = – 0.8w = – 0.6
A constant limiting mass was assumed.
To relate observations to models, it is importantto know the selection function of the survey,
and the Mass-Observable relation
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• Velocity dispersion of cluster galaxies + virial theorem
• Hot gas in equilibrium with the gravitational
• Gravitational lensing (strong + weak lensing)
⇒ Total mass: a few times 1013 to 1015 Msun
• Scaling relations M - Observable
85%
10%5%
GalaxiesHot gasDark matter
kBTe !
!
GMmp
2Re!
"
! 7
!
M
3 " 1014M!
" !
Re!
1Mpc
""1
keV
1
Cluster masses
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Mass
LX
TX
YSZ
N200
σV
Lensing mass
Optical/NIR
X-ray
mm-radio
Scaling relations: Mass – Observable
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Mass
LX
TX
YSZ
N200
σV
Lensing mass
Optical/NIR
X-ray
mm-radio
Scaling relations: Mass – Observable
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Constrain cosmologically-relevant quantities & the cosmological model with clusters:
- Clusters are natural TELESCOPES (Gravitational lenses to probe the high-z Universe)
- Number counts n(M,z)+ 2-point correlation function ξ(M,z) ➜ CosmoParams, neutrino mass,
non-Gaussianity, ...
- Baryon mass fraction in virialized clusters (Allen et al. 2011) ➜ CosmoParams...
- SZ: – Thermal SZ + X-rays of virialized clusters: DA(z) ➜ H0 – Kinetic SZ: Peculiar velocities ➜ CosmoParams... – TCMB(z ≠ 0). ➜ Standard law TCMB = T0(1+z), or more exotic model?
- Dark matter:
– Merging clusters ➜ Constraints on the properties of DM (self-interaction cross-section)– DM annihilation ➜ secondary electrons ➜ SZ signature
➜ gamma rays- Cosmic magnetic fields (LOFAR/SKA) via observations of polarized emission and of
Faraday Rotation Measures (∝∫ neB// dl) of background sources (tomography)Tuesday, February 5, 2013
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B
Relat. e-
Th. e-
p
Radio synchrotron
X-ray (Bremsstrahlung)
γCMB
γCMB
γCMB
Th. e-SZ
(Inverse Compton scattering)
γCMB
γCMB
γCMB
π0
γ+γ Gamma rays
Dark matter
Thermal e- (keV), suprathermal e- (>10 keV), relativistic e- (power-law, MeV-GeV)
BRadio Faraday rotation
(∝∫ neB// dl)
Relat. e-γCMB
X/Gamma(Inv. Compton)
Th. e-
π0
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THE SUNYAEV-ZELʼDOVICH EFFECT &
SZE OBSERVATIONS of CLUSTERS
Picture: Sheldonʼs and Lennartʼs white board in the TV series The Big Bang Theory
x = hν/kT
The Compton parameter y
y ∝∫ neTe dl ∝∫ Pe dl
y is dimensionless
We measure Y = ∫ y dΩin units of solid angle (sr, arcmin2)
Y is tightly related to the Mass!
The Kompaneets equationChange in the photon occupation number ∆n
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Zelʼdovich & Sunyaev 1969; Reviews by Birkinshaw 1999; Carstrom et al. 2002
APEX
-SZ
LABO
CA
The SZ effect: Inverse Compton scattering of CMB
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1. Thermal SZ effect
Decrement in the radio/mm, increment in the submm
ΔTSZ,th/TCMB(ν) ∝∫clusterneTedl = gas pressure
2. Kinetic SZ effect: ~10 times weaker
ΔTSZ,kin/TCMB(ν) ∝-vpec/c
Depends on the mass of the intracluster gas.
Current observations are sensitive to clusters with masses M > a few 1014 Msun.
Important: independent of redshift!
3. Relativistic SZ effect(High Te, high frequencies)
Characteristic distortions of the CMB spectrum:
APEX
-SZ
LABO
CA
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Planck observation of Abell 2319 at z = 0.056 (DL = 236 Mpc)Image Credit: ESA / HFI & LFI Consortia
2 degrees
The Planck Early Science SZ catalog: 189 clusters (incl. 20 new)(the Planck Collaboration 2011, A&A)
Angular resolution: 24ʼ to 5ʼ
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Reichardt et al. 2013
South Pole TelescopeAngular resolution 1ʼ
150 + 95 GHz
Planck: Beam dilution
ROSAT: Cosmological dimming
224 cluster candidatesin 720 deg2 (out of 2500 deg2),
158 confirmed in opt/NIR.Median z = 0.55
Mlim = 5 1014/h Msun at z > 0.6
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APEX-SZPI: Adrian Lee
• Mapping the SZ decrement at 2 mm (150 GHz)
• Angular resolution of 1ʼ; FOV = 24ʼ
• Observations between 2005 and 2010
• 48 clusters + 2 deep fields.
Dec 2009Tuesday, February 5, 2013
Example of APEX-SZ 150 GHz maps (Schwan et al. 2012, The ESO Messenger)
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The Bullet Cluster at z = 0.3
Credit: X-ray: NASA/CXC/CfA/M.Markevitch et al.; Optical: NASA/STScI; Magellan/U.Arizona/D.Clowe et al.; Lensing Map: NASA/STScI; ESO WFI; Magellan/U.Arizona/D.Clowe et al.
Hot gas (X-ray)
Dark matter (lensing)
Galaxies
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The Bullet Cluster as a gravitational lens (Johansson, Horellou et al. 2010, A&A)
• 17 submm galaxies (APEX-LABOCA 870 micron map)
• The brightest one is a z = 2.8 galaxy located near a caustic line and magnified ~ 100 times
Red:Total mass distribution (Weak lensing from Clowe et al.)Red: X-ray (XMM)
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The Bullet Cluster at z = 0.3
Star: Bright submm galaxy (50 mJy at 870 micron, Johansson et al. 2010) at z=2.8 near a critical line of the Bullet Cluster and magnified 100 times; its flux at 2 mm is negligible compared to the SZ
SZ decrement (APEX-SZ, 2mm): Halverson et al. 2009
SZ increment (LABOCA, 870 micron): Horellou et al., in prep
Contours: X-rayColors: SZ, resolution 27”
Substructure in the SZ, offset from the X-ray
Contours + Colors: SZ, resolution 1.4ʼ
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The SZE spectrum
Abell 2163 at z = 0.3, Nord et al. 2009
Fixing temperature gives constraint on peculiar velocity-central Compton
parameter
vpec,los = –140 ± 460 km s−1,
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Abell 2163 at z = 0.3, Nord et al. 2009
De-projected density & temperature
Joint X-ray/SZ analysis:
SZ: ∫losneTe dl
X-ray: ∫losne2
Lambda(Te) dl
Assuming spherical symmetry, one can use the Abel transformation
ne
Te
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De-projected density & temperatureProfile of the enclosed gas mass and the total mass
(assuming hydrostatic equilibrium)
Abell 2204, a relaxed cluster at z = 0.15, Basu et al. 2010
ne
Te
Mgas (<R)
Mtot (<R)
fgas (<R)
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APEX-SZ scaling relations Bender et al., in prep
The integrated Compton parameter YSZ is a good proxy of the clusterʼs total mass (e.g. Motl et al. 2006, Arnaud et al. 2010)
Y500
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Lensing follow-up of the 15 clusters of our sample for which no weak lensing data exist
Ongoing PhD work of Matthias Klein, BonnBVR observations with the wide field imager (WFI) on the ESO/
MPG 2.2 m telescope in La Silla, FOV = 33ʼx34ʼ
Photo: www.eso.org
M200 = 11.4 (+2.5 -2.2) x 1014 Msol R200 = 1.96 +/- 0.13 Mpc
RXC 0532
S/N map of the reconstructed projected mass and shear profile
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RADIO SYNCHROTRON OBSERVATIONS of CLUSTERS, LOFAR
The Onsala LOFAR stationCredit: Onsala Space Observatory/Leif Helldner
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Figure: Radio halo of the Bullet Cluster (grey)+ X-ray surface brightness contours (Liang et al. 2000) after subtraction of the radio point sources
• Synchrotron emission on Mpc scale• Low surface brightness:
~3 mJy/arcmin2 at 1.4 GHz• Steep spectrum (α < –1, Sν ~να)⇒ brighter at lower frequencies
• Unpolarized
Detected in ~30% of X-ray clusters (Ferretti et al. 2012)
Origin of the relativistic electrons?
Accelerated in turbulence generated in mergers (e.g. Brunetti 2001)?
Giant radio halos in (some) galaxy clusters
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Feretti et al. 2012Tuesday, February 5, 2013
2 Mpc long radio relic in the z= 0.19 Sausage Cluster
(van Weeren et al. 2010, Science)
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The radio–X-ray correlation
Figure: Brown et al. 2011, ApJRed points: Detection of radio signal at 843 MHz by stacking ~100 clusters
Bi-modality
ON!
OFF!?
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The radio–X-ray correlation
Figure: Brown et al. 2011, ApJRed points: Detection of radio signal at 843 MHz by stacking ~100 clusters
Bi-modality
ON!
OFF!
What about lower X-ray luminosity clusters/groups? ➜ XXL
?
?
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61-67 MHz LOFAR map
Field around Abell 2256: resolution 80”
Inset: resolution 22”x26”
van Weeren et al. 2012 A&A
First LOFAR results: Abell 2256 at 8 - 67 MHz.
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z=0.0594
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LOFAR expectations for radio halosSo far: only about 50 radio halos are detected (VLA, GMRT).
The LOFAR all-sky survey at 120 MHz is expected to detect about 350 giant radio halos at z < 0.6 (Cassano et al. 2010 A&A).
Relation to mergers?
Population of CR electrons
Magnetic field via Rotation Measure Synthesis of polarized background/cluster galaxies.
There is a “Clusters” working group in the “Surveys” Key Science Project (KSP) (PIs Brueggen & Brunetti)
“Magnetism” KSP: Plan to search for polarization from galaxies (isolated/in groups and clusters, star-forming, AGN) and from the cosmic web of filaments.
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die Kunst !
Über!
in der Wissenschaft!" Kandinsky!
PI: Marguerite Pierre (Saclay, France)Consortium of ~100 researchers!
The largest XMM project ever
2 x 25 deg2
Equatorial field CFHT-LS, RA = 2h23, DEC=-5dSouthern field BCS, RA=23h30, DEC=-55d
10 ksec per pointing
Extension of the XMM-LSS (Pacaud et al.ʼ06; 5.5 deg2; Chiappetti et al.ʼ12, 11.1 deg2),
C1 clusters: 5-6 /deg2
C2 clusters (50% complete): 12/deg2
XXL is expected to detect ~50 clusters at z > 1and more than 500 clusters in total,
+ 10 000 AGN.
Constrain the evolution of equation-of-state parameter w(z) of dark energy.
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XXL equatorial field:extension of XMM-LSS field
Blue: existing dataRed: new observationsYellow: observations from other programsBlack rectangle: VIPERS spectroscopy
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XXL Southern field:extension of XMM-BCS field
Blue, cyan, magenta: existing dataRed: new observationsYellow: observations from other programsBlack: Optical spectroscopy
Δα = Δδ= 20ʼ (Δα = Δδ = 23’ in the initial central survey)
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From Pierre et al. 2011, MNRAS
Cosmological predictions for the XXL surveyw(z) = w0 + wa z/(1+z)
w(a) = w1 + w2 a, where a= 1/(1+z)
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Frequency Telescope Area Resolution Largest angular scale
Detection limit (5σ) Reference
1.4 GHz VLA (NVSS) All sky δ > –40o 45” 15ʼ 2.5 mJy/bCondon et al.
1998
1.4 GHz VLA (FIRST) All sky δ > –40o 5” 2ʼ 0.15 mJy/b Becker et al.
610 MHz GMRT 12.7 deg2 6.5” 6.9ʼ 1.5 mJy/b Tasse et al. 2007
325 MHz VLA 15.3 deg2 6.7” 4 mJy/b Tasse et al. 2006
240 MHz GMRT 18 deg2 14.7” 11.5ʼ 12.5 mJy/b Tasse et al. 2007
74 MHz VLA 132 deg2 30” 20ʼ 160 mJy/bCohen et al.
2003 Tasse et al. 2006Tasse et al 2006
Existing radio observations of the XXL equatorial field
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Radio observations of XXL
Main goals: Evolution of AGN and cluster-scale radio emission
Equatorial field (at DEC = –5 deg)
* Observed with LOFAR in January (PI Ph. Best)
* GMRT 610 MHz proposal accepted (PI S. Raychaudhury)5” resolution. Point-like sources versus extended emission?
* Jansky VLA (PI V. Smolcic)
Test data 3 GHz, 2 deg2
Future: Map the whole equatorial field at 2-4 GHz, 2” resolution.
Southern field:
* ATCA (PI V. Smolcic)Pilot proposal accepted (5.5 deg2). 2.1 GHz (BW 2 GHz), 15-20 μJy/beam rms
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mm observations of XXL
Main goal: Sunyaev-Zeldovich observations of clustersEquatorial field
* Covered by ACT* Plans to start a systematic SZ follow-up of the most massive/distant clusters* CARMA observations of a few high-z clusters PIs: Adam Mantz, Tom Plagge (Chicago)
* APEX-SZ 2 mm observations of 0.75 deg2 of XMM-LSS, centered on XMM LSS-006, M500 = 1.9 1014 h-1 Msun
Second cluster detected10 μK rms in the central 0.25 deg2
PI: Florian Pacaud (Bonn)
Southern field* Covered by SPT
Figure: APEX-SZ map of XMM-LSS
~50ʼTuesday, February 5, 2013
Conclusion– Clusters are at the crossroad of astrophysics & cosmology:
they are complex individuals and the sites of interesting physical processes;
yet they are rather simple and share common fundamental properties
– To use clusters in cosmology it is essential to understand their astrophysics
– Fortunately, there are/will be new instruments able to measure the tiny signals from clusters, from gamma-rays to radio
– This is a unique time in history...
– ...but with great power comes great responsability (to figure it all out!)
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