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I. Balestra I. Balestra , Paolo Tozzi, S. Ettori, P. Rosati, , Paolo Tozzi, S. Ettori, P. Rosati, S. Borgani, V. Mainieri, M. Viola, C. Norman S. Borgani, V. Mainieri, M. Viola, C. Norman Galaxies and Structures through Cosmic Times - Venice, March 2006 Evolution in the chemical enrichment of the intracluster medium

Evolution in the chemical enrichment of the intracluster medium

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I. BalestraI. Balestra, Paolo Tozzi, S. Ettori, P. Rosati, , Paolo Tozzi, S. Ettori, P. Rosati, S. Borgani, V. Mainieri, M. Viola, C. NormanS. Borgani, V. Mainieri, M. Viola, C. Norman

Galaxies and Structures through Cosmic Times - Venice, March 2006

Evolution in the chemical enrichment of the intracluster

medium

High redshift(z>0.3) clusters in medium-deep Chandraexposures(ACIS-I andACIS-S)

Science:Scaling relations(temperature, luminosity, massentropy)Chemical enrichmentAGN around clustersBaryon fraction and cosmological test

RXJ1252: detection of the Fe line at z=1.23

Rosati et al. 2004

Fe Ions concentration as a function of the ICM temperature

Collisionally dominated optically thin coronal plasmaas a function of electron temperature (Mewe 1991)

5 -10 keVFe XXVFe XXVI

The Iron abundance is determined almost uniquely by the K-shell complex at 6.7-6.9 keV rest-frame

We select from the Chandra archive 56 clusters at z>0.3(among them 7 clusters at z>1)

Distribution with temperature and redshift of the sample

We samplecentral regionsbetween 0.15and 0.3 R

vir

depending on the redshiftof the cluster

Temperature vs redshift (56 clusters @ z> 0.3)3 times more objects than in Tozzi et al. 2003

Balestra et al. 2006

Caveat: two differentvalues of solar Fe abundin the literature:

Anders & Grevesse 1989Fe/H = 4.68 × 10-5

Grevesse & Sauval 1998Fe/H = 3.16 × 10-5

ZFeGS

= 1.48 ZFeAG

Scatter comparable with statistical errorshint ofhigherFe abundanceat low kT<5 keV

Fe abundance-Temperature in different redshift bins

Iron abundance -Temperature

Weightedaverage

Balestra et al. 2006

And

ers

& G

reve

sse

1989

Horner 2001 PhDBaumgartner et al. 2005

Local sample 273 clusters observed with ASCAG

reve

sse

& S

auva

l 199

818 local clusters observed with ASCAFinoguenov, Arnaud & David 2001

And

ers

& G

reve

sse

1989

XMM-Grating data from cool core cluster Peterson et al. 2003

Iron abundance versus redshift

Balestra et al. 2006

Average Iron abundance versus redshift

Balestra et al. 2006

We find an increase of a factor about 2 in Z

Fe

from z=1.2 to z=0.4 in the central 0.2 R

vir of

hot clustersconsistent with Z

Fe = 0.55 (1+z)-1.3

This larger sample showshigher Z

Fe at z<0.5,

implying significant evolution (Tozzi et al. 2003 was still consistentwith no evolution, with weak hints of decrease at less than 2 σ c.l.)

It is known that locally ZFe

= 0.6 in cold-core clusters and Zfe = 0.2/0.3 in

non cold-core clusters (see De Grandi et al. 2001; 2004).

Is this evolution associated to the evolution of the cold-cores with Iron peak within the central 0.1 R

vir?

First check: Iron abundances are not affected by masking of the central 0.1 R

vir (when possible)

More directly, there is no correlation with the central surface brightness(cooling time)

Fe Abundance vs central Surface Brightness

Is the Iron abundance evolution expected?

Ettori 2005

Fe abundance in the ICM from the observed cosmic Star Formation Ratewith large delay times for TyIa Sne (~4 Gyr, see Dahlen et al. 2004)

CONCLUSIONS

Clear detection of the Iron line in the large majority of high-z clusters, up to z~1.3

Correlation in the Iron abundance – Temperature relation at high-z: Iron abundance starts to increase below 5 keV

Fe abundance ~ 0.25 Z⊙ constant for z>0.6

Higher average Fe abundance in the z~0.4-0.6 redshift range

The decrease of the average Iron abundance from ZFe

=0.4 Z⊙(@ z~0.3)

to ZFe

=0.2 Z⊙ (z~1.3), consistent with cosmic star formation rate only

for large TyIa delay times (~ 4 Gyr).

Open question: production of diffusion of Fe enriched gas betweenz=1.2 and z=0.4?

A sample of ~56 clusters @ z>0.3 observed with Chandra