Cluster Lenses High Redshift Clusters MACS A Status

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Cluster Lenses & High Redshift Clusters (MACS) A Status Report Jean-Paul KNEIB Observatoire Astronomique

Cluster Lenses & High Redshift Clusters (MACS) A Status Report Jean-Paul KNEIB Observatoire Astronomique Marseille Provence, Marseille, France H. Ebeling, G. Smith, A. Gal-Yam, I. Smail, A. Edge, J. Greene, P. Hudelot, S. Bardeau, G. Soucail, P. Marshall, E. Egami, G. Covone, E. Jullo and many others October 25, 2005 Ringberg, Hi-z clusters

Outline v. Lensing in Clusters v. Mass Distribution in Cluster: strong & weak lensing

Outline v. Lensing in Clusters v. Mass Distribution in Cluster: strong & weak lensing at low-z v. MACS Clusters (0. 3<z<0. 8): v. ACS deep survey v. MACS Snapshot, RXJ 0152 v(SN search) v. Future prospects October 25, 2005 Ringberg, Hi-z clusters 2

Theory: Lens Diagram CFHT BRI 1990 Z_cluster=0. 375 Z_arc=0. 725 (Soucail et al 1988)

Theory: Lens Diagram CFHT BRI 1990 Z_cluster=0. 375 Z_arc=0. 725 (Soucail et al 1988) October 25, 2005 Ringberg, Hi-z clusters 3

Science with Cluster Lenses • Study the mass distribution of cluster => cosmology? •

Science with Cluster Lenses • Study the mass distribution of cluster => cosmology? • Study the distant lensed Universe • Direct constrain on cosmological parameters October 25, 2005 Ringberg, Hi-z clusters 4

Theory: Lens Mapping a The lensing equation is a mapping from image plane to

Theory: Lens Mapping a The lensing equation is a mapping from image plane to source plane: q - b = Dls/Ds. a = Dls/Ds df/dq For a point mass, the deflection angle is: a = 4 GM/bc 2 (b is the impact parameter) -> typically 10” for a 1014 Solar mass Amplification matrix: October 25, 2005 Ringberg, Hi-z clusters 5

Cluster Lenses Insensitive to: • Nature of matter • Physical state of matter Cleanest

Cluster Lenses Insensitive to: • Nature of matter • Physical state of matter Cleanest available probe of Dark Matter Strong Lensing in the core, Weak lensing on large scale Most massive clusters Einstein radius: 10 -45” October 25, 2005 Ned Wrigth, UCLA Ringberg, Hi-z clusters 6

Mass distribution in cluster cores October 25, 2005 Ringberg, Hi-z clusters 7

Mass distribution in cluster cores October 25, 2005 Ringberg, Hi-z clusters 7

Cluster Lens: Mass Reconstruction • Parameterized mass distribution, involving various multiple image system (works

Cluster Lens: Mass Reconstruction • Parameterized mass distribution, involving various multiple image system (works better, less free parameters) • Need to include galaxy scale mass components using scaling relations (dominate locally the mass) October 25, 2005 Ringberg, Hi-z clusters 8

Strong and Weak Lensing Absolute central mass October 25, 2005 relative total mass and

Strong and Weak Lensing Absolute central mass October 25, 2005 relative total mass and slope Ringberg, Hi-z clusters 9

An Example from space: Cl 0024+1654 HST wide field sparse mosaic • 76 orbits,

An Example from space: Cl 0024+1654 HST wide field sparse mosaic • 76 orbits, 38 pointings • Probe regions up to ~5 Mpc Aim: learn cluster physics of clusters by comparing with other mass estimates: X-ray, dynamics October 25, 2005 (Treu et al 2003, Kneib et al 2003) Ringberg, Hi-z clusters 10

0024: Shear Profile SIS fitting strong lensing data • Extrapolate strong lensing models at

0024: Shear Profile SIS fitting strong lensing data • Extrapolate strong lensing models at large scale by exploring various cluster mass profile. • Rule out SIS model • NFW (with large c~20) or Power-law models give comparatively good model. October 25, 2005 NFW fitting strong And weak lesning ~3 Mpc Ringberg, Hi-z clusters 11

Cl 0024: Mass vs. Light • NFW and Power-Law model fit the strong+weak lensing

Cl 0024: Mass vs. Light • NFW and Power-Law model fit the strong+weak lensing But high concentration compared to expectations (similar results on other clusters: A 1689 …) Mass traces Light !!! Red sequence selection Light profile NFW model Broader sequence selection SIS model fitting weak lensing • SIS does not fit the strong+weak lensing • M/L is constant with radius with M/LK~40 October 25, 2005 Kneib et al 2003 Ringberg, Hi-z clusters 12

Questions for Cluster Physics • What are the total mass and structural properties of

Questions for Cluster Physics • What are the total mass and structural properties of massive clusters? • How are the mass and structure of clusters related to the global thermodynamics (Tx, Lx)? • How do cluster substructure and thermodynamics evolve with redshift? • Implications of cluster mass and substructure for cluster Cosmology? October 25, 2005 Ringberg, Hi-z clusters 13

X-ray Luminosity Multi-wavelength/epoch study Dt~2 Gyr z=0 z=0. 2 2 Gyr • z=0. 21+/-0.

X-ray Luminosity Multi-wavelength/epoch study Dt~2 Gyr z=0 z=0. 2 2 Gyr • z=0. 21+/-0. 04 • Lx>8 x 1044 erg/s z=0. 5 z~1 • Study of 10 clusters at z~0. 2 – – HST, WFPC 2, F 702 W, 7 5 ksec Chandra, ACIS-I(S), 4 -40 ksec UKIRT, UFTI, 9 ksec October 25, 2005 Ringberg, Hi-z clusters CFHT 12 k, BRI, weak shear A 68 A 209 A 267 A 383 A 773 A 963 Ellis et al. 1991 A 1763 A 1835 A 2218 Kneib et al. 1996 A 2219 Smail et al. 1995 14

Example: Abell 68 (z=0. 25) Smith et al 2001, 2003, 2005 Triply-imaged “ERO” R-K=5.

Example: Abell 68 (z=0. 25) Smith et al 2001, 2003, 2005 Triply-imaged “ERO” R-K=5. 4 z=1. 6 Data and constraints – ID multiple image systems (HST) – Spectroscopic redshifts (Keck+) – Weak lensing constraints (HST) Measurements – Cluster mass (R<500 kpc) – Dark matter morphology October 25, 2005 Ringberg, Hi-z clusters 15

Quantitative structural classification Smith et al. , 2005 Relaxed Typical Unrelaxed Atypical Unrelaxed Mass

Quantitative structural classification Smith et al. , 2005 Relaxed Typical Unrelaxed Atypical Unrelaxed Mass [Lensing] ICM [X-ray] Ndm 1 Mcen/Mtot Ttot/Tann Δr (arcsec) 2 1 0. 97± 0. 01 0. 77± 0. 01 0. 8± 0. 1 1. 0± 0. 1 <1 10± 2 22± 1 0. 96± 0. 01 1. 0± 0. 2 Ø 70% of X-ray luminous cluster cores at z=0. 2 are dynamically immature and strongly heterogeneous October 25, 2005 Ringberg, Hi-z clusters 16

M-T relation or M-T scatter plot? Smith et al. , 2005 Structural segregatio n

M-T relation or M-T scatter plot? Smith et al. , 2005 Structural segregatio n [~40%] Finoguenov et al. , 2001 Possible Systematics? [~10 -20%] • Unrelaxed clusters are 40% hotter than relaxed clusters (2. 5σ) • Consistent with hydro simulations of cluster-cluster mergers (Ricker & Sarazin 2001, Randall et al. 2003) October 25, 2005 Ringberg, Hi-z clusters 17

Better agreement with weak lensing? October 25, 2005 Ringberg, Hi-z clusters 18

Better agreement with weak lensing? October 25, 2005 Ringberg, Hi-z clusters 18

weak lensing shear profile October 25, 2005 Ringberg, Hi-z clusters 19

weak lensing shear profile October 25, 2005 Ringberg, Hi-z clusters 19

(~150 z/cluster) lensing dynamics weak lensing scatter plots… Lensing October 25, 2005 Ringberg, Hi-z

(~150 z/cluster) lensing dynamics weak lensing scatter plots… Lensing October 25, 2005 Ringberg, Hi-z clusters X-ray 20

Better agreement with weak lensing? • Offset between dynamics and mass: sign of merger

Better agreement with weak lensing? • Offset between dynamics and mass: sign of merger due to optical selection ? Or the fact that those systems are still young? • A big scatter between Tx and Mass: we can probably do better (including strong lensing) but … limited by cluster substructure • Need better data and statistics … ie. go from sample of 10 s to sample of 100 s October 25, 2005 Ringberg, Hi-z clusters 21

The MAssive Cluster Survey (MACS) • MACS is covering a very wide area and

The MAssive Cluster Survey (MACS) • MACS is covering a very wide area and thus is able to discover the most x-ray luminous clusters unlike other surveys. • Most massive clusters should be strong lenses • ~120 z>0. 3 MACS clusters to be observed with Chandra & ACS SNAP • 10 MACS cluster have been observed with HST/ACS October 25, 2005 Ringberg, Hi-z clusters 22

MACS clusters at 0. 5<z<0. 6 2 Gyr • 10 clusters at z~0. 55

MACS clusters at 0. 5<z<0. 6 2 Gyr • 10 clusters at z~0. 55 • HST/ACS imaging 2 Gyr X-ray Luminosity Dt~2 Gyr z=0 – F 555 W, F 814 W – 5 ksec/filter • Keck/LRIS + VLT/FORS spectroscopy (arcs and cluster galaxies) z=0. 2 z=0. 5 z~1 – Blue and Red spectroscopy • SUBARU/Suprime imaging – Weak lensing and galaxy population October 25, 2005 Ringberg, Hi-z clusters 23

MACS 1149 z=1. 5 z=1. 89 October 25, 2005 Ringberg, Hi-z clusters 24

MACS 1149 z=1. 5 z=1. 89 October 25, 2005 Ringberg, Hi-z clusters 24

MACS 0717 z=2. 96 Ly- blob October 25, 2005 Ringberg, Hi-z clusters 25

MACS 0717 z=2. 96 Ly- blob October 25, 2005 Ringberg, Hi-z clusters 25

MACS 0257 z=1. 06 October 25, 2005 Ringberg, Hi-z clusters 26

MACS 0257 z=1. 06 October 25, 2005 Ringberg, Hi-z clusters 26

MACS/HST weak lensing October 25, 2005 Ringberg, Hi-z clusters 27

MACS/HST weak lensing October 25, 2005 Ringberg, Hi-z clusters 27

MACS/HST weak lensing Marshall et al 2006 Cluster mass reconstruction method using (NFW) blobs

MACS/HST weak lensing Marshall et al 2006 Cluster mass reconstruction method using (NFW) blobs that can combine strong+weak lensing data: using MCMC techniques To cope with complex Shape seen at high-z Simulation data Atomic Inference October 25, 2005 Classical 2 D reconstruction Ringberg, Hi-z clusters 28

4 Mpc filament in MACSJ 0717. 5+3745 Ebeling et al (GO: 10420, cycle 14)

4 Mpc filament in MACSJ 0717. 5+3745 Ebeling et al (GO: 10420, cycle 14) X-ray+Gal density October 25, 2005 Lensing Subaru+Gal density+ ACS survey Ringberg, Hi-z clusters 29

4 Mpc filament in MACSJ 0717. 5+3745 Ebeling, Barrett, Donovan, 2004 Galaxies with Spectra

4 Mpc filament in MACSJ 0717. 5+3745 Ebeling, Barrett, Donovan, 2004 Galaxies with Spectra October 25, 2005 Redshift distribution Ringberg, Hi-z clusters 30

Does cluster substructure evolve? • Current status of MACS strong lensing analysis – Candidate

Does cluster substructure evolve? • Current status of MACS strong lensing analysis – Candidate gravitational multiple images identified – [Ground-based spectroscopy of arcs <~50% complete] • Broad brush demographics: z=0. 2 z=0. 55 Strong lensing clusters 8/10 Unrelaxed clusters 4/10 9/10 Candidate unrelaxed clusters Relaxed cool core clusters 2/10 Relaxed non cool core clusters October 25, 2005 10/10 3/10 1/10 Ringberg, Hi-z clusters 7 9 0/10 3 1 0/10 31

MACS Snapshot ACS Ebeling et al (GO: 10491, cycle 14) • List of 124

MACS Snapshot ACS Ebeling et al (GO: 10491, cycle 14) • List of 124 MACS clusters to be observed with HST/ACS in SNAP mode in F 814 W • Aim at finding effective lensing clusters and strongly distorted arcs (statistics and magnified sources) • 5 clusters already observed October 25, 2005 Ringberg, Hi-z clusters 32

MACS Snapshot ACS Ebeling et al (GO: 10491) First Strong Lensing IDs October 25,

MACS Snapshot ACS Ebeling et al (GO: 10491) First Strong Lensing IDs October 25, 2005 Ringberg, Hi-z clusters 33

RXJ 0152 -29 a massive cluster at z~0. 83 • X-ray luminous cluster at

RXJ 0152 -29 a massive cluster at z~0. 83 • X-ray luminous cluster at z=0. 83 • At least 8 multiple image systems, one at z=3. 9 (Umetsu et al 2005)=> high ellipticity for DM, indicative of a merger. • Ideal probe for VIMOS/IFU • Potential interest for cosmology (Golse et al 2002) October 25, 2005 VIMOS/IFU Field of view Ringberg, Hi-z clusters

Lensing for Cluster Physics • Lensing is probing mass relatively easily, measuring substructure gets

Lensing for Cluster Physics • Lensing is probing mass relatively easily, measuring substructure gets more difficult at higher z, but is clearly seen! • Scattered relation between Mass and X-ray depends on physical state and substructure (merger/relaxed) • Higher substructures at higher redshift (lots of lensing till z~0. 8 in massive systems)? • Cosmology with cluster is likely to be hard - at least with current cluster sample size (10 s) need much larger sample, but will learn some physics. October 25, 2005 Ringberg, Hi-z clusters 35