The inside-out Growth of the Stellar Mass Distribution in Galaxy Clusters since z 1

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The inside-out Growth of the Stellar Mass Distribution in Galaxy Clusters since z 1 Remco van der Burg CEA Saclay, France A&A in press (ArXiv:1412.2137) Henk Hoekstra, Adam Muzzin, Cristóbal Sifón, Michael Balogh, Sean McGee

Dark Matter Haloes follow NFW* Profiles *Navarro, Frenk, White (1997)! R 200 : Radius at which the average density inside is 200 times the critical density. M 200 : enclosed mass within this sphere! Concentration:

Mass and Concentration of Dark Matter Haloes evolve with Redshift Mass increase factor ~ 10 since z=2 N-body simulations: c ~ 3 in this regime Reproduced by CLASH (talks yesterday)

Presence of Baryons can alter Distribution of Dark Matter! Important for accurate cosmology with clusters! Baryons can cool and form stars! Stellar/AGN feedback (beyond Tinker+08) (van Daalen+10, Cusworth+13) Powerful constraint for forthcoming large hydrodynamical simulations: M h 10 14 M M h 10 12 M What is the radial distribution of stellar mass in high mass haloes? Moore et al. 1999

Observed Stellar Mass Distributions! Stellar Matter also well described by NFW profile Lin+2004 Muzzin+2007 Budzynski+2012 Lin+2004! Concentration of stars (observations) is consistent with the concentration of the dark matter in similar haloes (simulations)

Observed Stellar Mass Distributions! Stellar Matter also well described by NFW profile Lin+2004 Muzzin+2007 Budzynski+2012 Lin+2004 This is a K-band luminosity profile? These are number density profiles! Concentration of stars (observations) is consistent with the concentration of the dark matter in similar haloes (simulations) Different studies not homogeneous + unknown what happens at high z

Two Galaxy Cluster Samples! 60 clusters at 0.05 < z < 0.26! Canadian-Cluster-Comparison Project! Multi-Epoch Nearby Cluster Survey! ugri-band photometry! 10,000 spectroscopic members (Sifón+2015)! 10 clusters at 0.86 < z < 1.34 from 42 deg 2 SpARCS/SWIRE survey! Gemini CLuster Astrophysics Spectroscopic Survey (GCLASS) (Muzzin+2012)! ugrizjks + 4IRAC band photometry! 457 spectroscopic members vdburg+15 (1412.2137) vdburg+13 (1304.5525) vdburg+14 (1310.0020)

z 0.15 Stellar Mass Distribution vdburg+15 (1412.2137)! NFW profile (c 2) fits ensemble distribution for radii R > 0.10 R 200! Significant excess in the centre, 10 11 M per cluster! No dependence on: redshift, halo mass, BCG stellar mass, cluster central entropy, richness

z 0.15 Stellar Mass Distribution Inner slope ρ r 1.6 vdburg+15 (1412.2137)! NFW profile (c 2) fits ensemble distribution for radii R > 0.10 R 200! Generalized NFW profile gives a better fit overall! Inner slope ρ r 1.63±0.10

z 0.15 Stellar Mass Distribution! NFW profile (c 2) fits ensemble distribution for radii R > 0.10 R 200! Reasonable agreement with dark matter distribution (N-body simulations)

z 1 Stellar Mass Distribution vdburg+14 (ArXiv:1310.0020)! Well fitted by NFW profile with concentration parameter c 7! Stellar Mass at z=1 significantly more concentrated than! Dark matter in N-body simulations! Likely descendants at lower redshift (z=0.15)

Observed Evolution! Complications:! NFW profile no good fit to low-z at small radii! Pseudo-evolution complicates interpretation (e.g. Diemer+13)

Observed Evolution! Complications:! NFW profile no good fit to low-z at small radii! Pseudo-evolution complicates interpretation! Cluster samples are linked progenitors-descendants! Compare profiles on the same physical scale (e.g. Diemer+13) Physical distance

Observed Evolution! Complications:! NFW profile no good fit to low-z at small radii! Pseudo-evolution complicates interpretation! Cluster samples are linked progenitors-descendants! Compare profiles on the same physical scale BCG+ICL growth (e.g. Diemer+13)! Orange region 6 10 11 M : consistent with BCG growth! Clusters accrete stellar mass onto the outskirts Outside Growth Physical distance

Observed Evolution! Inner ~ 400kpc of the stellar mass distribution already present in the centre by z=1! Different from evolution of dark matter distribution in N- body simulations

Outlook! So far simulations with only dark matter! Sub-haloes get destroyed near the centre (Nagai+05)! Test semi-analytic models (sub-halo abundance matching) (In collaboration with! Test recipes for tidal stripping/dynamical friction Ian McCarthy, Sean McGee,! Compare with hydrodynamical simulations Amandine le Brun)

Outlook! So far simulations with only dark matter! Sub-haloes get destroyed near the centre (Nagai+05)! Test semi-analytic models (sub-halo abundance matching) (In collaboration with! Test recipes for tidal stripping/dynamical friction Ian McCarthy, Sean McGee,! Compare with hydrodynamical simulations Amandine le Brun)! Limited sample (10 clusters) consider SZ-selected sample (Planck) (In collaboration with Monique Arnaud, Gabriel Pratt, )

Conclusions An observational study of the build-up of stellar mass in galaxy clusters by combining 2 samples which are progenitors/descendants:! At z=0.15, significant central excess (for R < 0.10 R 200 ) compared to best-fitting NFW profile! Naïve comparison of NFW concentrations suggests a dramatic evolution since z=1! Comparison on the same physical scale indicates inside-out growth of the stellar mass distribution since z=1! Stellar material is already present in the centre (R < 0.4 Mpc)! Significant growth onto the outskirts vdburg+15, A&A in press (ArXiv:1412.2137)

The inside-out Growth of the Stellar Mass Distribution in Galaxy Clusters since z 1 Remco van der Burg CEA Saclay, France A&A in press (ArXiv:1412.2137) Henk Hoekstra, Adam Muzzin, Cristóbal Sifón, Michael Balogh, Sean McGee

Observed Evolution! Different from evolution of dark matter distribution in N- body simulations! Blue galaxies (recently accreted) primarily found on cluster outskirts

Phot-z vs Spec-z

Spec-z completeness

Galaxy number densities

Blue vs red galaxies

SpARCS/GCLASS selection! Does richness correlate with concentration?! So far not seen at low-z! Unlikely that we probe a very peculiar distribution! However, consider SZ-selected sample (Planck)