THE CHANDRA AND XMM VIEW OF MASS, SLOSHING AND AGN FEEDBACK IN GALAXY GROUPS FABIO GASTALDELLO IASF MILANO, UCI F. BRIGHENTI, D. BUOTE, J. BULLOCK, S. DE GRANDI, D. ECKERT, S. ETTORI, L. DI GESU, S. GHIZZARDI, S. GIACINTUCCI, P. HUMPHREY, W.MATHEWS, S. MOLENDI, E. ROEDIGER, M. ROSSETTI, P. TEMI M. LIMOUSIN, T. VERDUGO, G. FOEX, R. MUNOZ, V. MOTTA, R. CABANAC AND THE SL2S TEAM OUTLINE 1.MASS RESULTS: MASS PROFILE, c-M PLOT AND GAS FRACTIONS FOR X-RAY GROUPS 2.AGN FEEDBACK AND SLOSHING COLD FRONTS IN THE PERSEUS OF GROUPS, NGC LENSING GROUPS AND THE BULLET GROUP DM DENSITY PROFILE Navarro et al The concentration parameter c do not depend strongly on the innermost data points, r < 0.05 r vir (Bullock et al. 2001, B01; Dolag et al. 2004, D04). c-M RELATION Bullock et al c slowly declines as M increases (slope of -0.1) Constant scatter ( logc 0.14) the normalization depends sensitively on the cosmological parameters, in particular 8 and w (D04,Kuhlen et al. 2005). c-M RELATION Macci et al. 2008 X-RAY MASS DETERMINATION Spectra averaged within circular annuli Normalization / shape of spectrum gives gas density / temperature X-RAY MASS DETERMINATION A) Deproject with no need to assume parametrized quantities for gas quantities but smoothing required to obtain a physical mass profile (smoothed inversion) fit gas density and temperature simultaneously assuming only parameterizations for density (or T or entropy) and mass B) Forward-fitting: fit gas density and temperature simultaneously assuming only parameterizations for density (or T or entropy) and mass Buote & Humphrey 11 A SPECIAL ERA IN X-RAY ASTRONOMY ChandraXMM-Newton 1 arcsec resolutionHigh sensitivity due to high effective area, i.e. more photons SUZAKU Low and stable background NFW a good fit to the mass profile c-M relation is consistent with no variation in c and with the gentle decline with increasing M expected from CDM ( = 0.03, P05). Vikhlinin et al Pointecouteau et al Clusters X-ray results THE PROJECT Improve significantly the constraints on mass profiles and c-M relation by analyzing a wider mass range with many more systems, in particular obtaining accurate mass constraints on relaxed systems with M M sun There were very few constraints on groups scale (10 13 M M sun ) In Gastaldello et al we selected a sample of 16 objects in the 1-3 keV range from the XMM and Chandra archives with the best available data RESULTS After accounting for the mass of the hot gas, NFW + stars is the best fit model MKW 4 NGC 533 STARS GAS DM RESULTS No detection of stellar mass due to poor sampling in the inner 20 kpc or localized AGN disturbance A 2717 RESULTS No detection of stellar mass due to poor sampling in the inner 20 kpc or localized AGN disturbance NGC 5044 Buote et al. 2002 RESULTS NFW + stars best fit model Not all the objects require stellar mass, due to poor sampling in the inner 20 kpc or localized AGN disturbance. Stellar M/L in K band for the objects with best available data is 0.57 0.21, in reasonable agreement with SP synthesis models ( 1) Adopting more complicated models, like introducing AC or N04 did not improve the fits. AC produces too low stellar mass-to- light ratios c-M relation for groups We obtain a slope = 0.076, c decreases with M at the 3 level THE LOCAL X-RAY c-M RELATION Buote, Gastaldello et al. 2007: c-M relation for 39 systems ranging in mass from ellipticals to the most massive galaxy clusters ( ) x M sun. A power law fit requires at high significance (6.6) that c decreases with increasing M (slope 0.026) Normalization and scatter consistent with relaxed objects THE LOCAL X-RAY c-M RELATION WMAP 1 yr Spergel et al. 2003 THE LOCAL X-RAY c-M RELATION WMAP 3yr Spergel et al. 2006 GAS FRACTIONS GASTALDELLO ET AL (see also Sun+09) CLUSTERS GROUPS THE PERSEUS CLUSTER Fabian+11 THE PERSEUS CLUSTER Fabian+11 THE PERSEUS CLUSTER Fabian+11 Fabian et al. 2003 NGC 5044 Gastaldello+09 (using J. Sanders binning code) See also results from longer Chandra observation (David+09) NGC 5044 Gastaldello+09 NGC 5044 CAON ET AL Gastaldello+09 DUST IN NGC 5044 TEMI, BRIGHENTI & MATHEWS m PAH NGC 5044 Gastaldello+09 BLACK : X-ray FILAMENT box #2 RED: X-ray FILAMENT box #7 COLD FRONTS IN CLUSTERS IN MERGING CLUSTERSIN RELAXED CLUSTERS Markevitch & Vikhlinin 07 COLD FRONTS IN CLUSTERS Ascasibar & Markevitch 06 SLOSHING CFs IN CLUSTERS Ascasibar & Markevitch 06 COLD FRONTS IN CLUSTERS Markevitch & Vikhlinin 07 HOW ABOUT GROUPS ? EXAMPLES IN MERGING SYSTEMS, e.g. NGC 1404 IN FORNAX (Machacek+05) SLOSHING CFs IN NGC 5044 Gastaldello+09 z=0.009 kT=1.2 keV SLOSHING CFs IN NGC 5044 Gastaldello+09 z=0.009 kT=1.2 keV SLOSHING CFs IN NGC 5044 Gastaldello+09 SLOSHING CFs IN NGC 5044 Gastaldello+09 z=0.009 kT=1.2 keV COMPARISON W/ SIMULATIONS SLOSHING IN PERSEUS Simionescu+12 EXCESS IN NGC 5044 SLOSHING CFs IN IC 1860 Gastaldello+13 arXiv: z=0.022 kT=1.4 keV SLOSHING CFs IN IC 1860 z=0.022 kT=1.4 keV Gastaldello+13 arXiv: SLOSHING CFs IN IC 1860 PECULIAR VELOCITIES AND PERTURBERS AM 06 MENDEL+08 STUDY OF 111 MEMBERS: PECULIAR VELOCITY OF 156 km/s WRT THE MEAN VELOCITY Z-score: 4.8 PECULIAR VELOCITIES AND PERTURBERS: NGC 5044 DETECTION OF A SUBSTRUCTURE (99.9 %) AT 1.4 Mpc MENDEL+08. OR NGC 5054 (DAVID+09). PECULIAR VELOCITIES AND PERTURBERS: NGC 5044 cz = 2733 km/s cz = 1658 km/s PECULIAR VELOCITIES AND PERTURBERS: NGC 5044 cz = 2733 km/s cz = 1658 km/s PECULIAR VELOCITIES AND PERTURBERS: NGC 5044 BUZZONI+12 PECULIAR VELOCITIES AND PERTURBERS: IC1860 STUDY OF 81 MEMBERS AVAILABLE IN NED: PECULIAR VELOCITY OF 11350 km/s (Z-score significant at the 2.3 level) WRT THE MEAN VELOCITY PECULIAR VELOCITIES AND PERTURBERS: IC1860 PRESENCE OF SUBSTRUCTURES AT A MARGINAL LEVEL 96% PECULIAR VELOCITIES AND PERTURBERS: IC1860 V PEC OF BCGs COZIOL+09: A large fractions of BCGs have significant peculiar velocity. This has one immediate consequence, which is that most clusters harboring a dominant galaxy are not dynamically relaxed VAN DEN BOSCH+05: The brightest galaxy in a dark matter halo is expected to reside at rest at the centre of the halo. In this paper, we test this `Central Galaxy Paradigm' (CGP) using group catalogues extracted from the Two-Degree Field Galaxy Redshift Survey (2dFGRS) and the Sloan Digital Sky Survey (SDSS). We show that the CGP is only consistent with the data in haloes with M < M sun, while in more massive haloes the data indicate a non-zero offset between the brightest galaxy and the satellites. This indicates that either central galaxies reside at the minimum of the dark matter potential, but that the halo itself is not yet fully relaxed, or, that the halo is relaxed, but that the central galaxy oscillates in its potential well. V PEC OF BCGs Van den Bosch+05 RADIO EMISSION: NGC 5044 GMRT RADIO DATA AT 610 MHz David+09 RADIO EMISSION: NGC 5044 GMRT RADIO DATA AT 235 MHz David+09 RADIO EMISSION: NGC 5044 GMRT RADIO DATA AT 235 MHz David+09 RADIO EMISSION: IC 1860 ABSENCE OF EXTENDED 1.4 GHz EMISSION (DUNN+10) RADIO EMISSION: IC 1860 GMRT RADIO DATA AT 325 MHz. EMISSION AT THESE SCALES INDICATES VERY STEEP SPECTRUM. RADIO EMISSION ZuHone+13 IMAGE SEPARATION DISTRIBUTION OF SL OGURI 2006 GALAXY GROUPS POOR CLUSTERS WITH IMAGE SEPARATION IN THE RANGE 6-16 HAVE BEEN SCARCELY REPORTED IMAGE SEPARATION DISTRIBUTION OF SL OGURI 2006 NO 6-15 IMAGE SEPARATION LENSES IN THE CLASS SURVEY (PHILLIPS+01, McKEAN10) SL2S GROUPS INITIAL SAMPLE OF 13 OBJECTS, A SUBSAMPLE OF THE SL2S BASED ON MULTI-COLOUR CFHTLS, IDEAL TO DETECT SL FEATURES AND FOLLOW-UP HUBBLE IMAGING (z = ) LUMINOSITY MAPS BASED ON LIGHT DISTRIBUTION OF ELLIPTICALS HAVE FOR SOME OBJECTS COMPLICATED SHAPE. WEAK LENSING SIGNAL DETECTED FOR 6 GROUPS SL2S GROUPS X-RAY FOLLOW-UP CLEARLY DIFFICULT BECAUSE WE ARE TARGETING LOW FLUX OBJECTS, HOWEVER MORE MASSIVE OBJECTS THAN PREVIOUS STUDIES (E.G., LARGEST IMAGE SEPARATION IN FASSNACHT+08 IS CLASS B WITH R E = 2.5) XMM SNAPSHOTS OF 5-10 ks TO SECURE FLUXES FOR DEEPER CHANDRA OBSERVATION. ENOUGH PHOTONS FOR MORPHOLOGY AND POSSIBLY TEMPERATURE SL2SJ z = 0.30 (PHOT) STRAIGHT ARC BETWEEN THE TWO GALAXIES SL R E = 6.8 SL2SJ TWO GROUPS DETECTED, THE N-ONE CONSISTENT WITH THE ELONGATION IN LUMINOSITY CONTOURS. THE S-ONE ASSOCIATED WITH THE LENS HAS A TEMPERATURE CONSISTENT WITH A POOR CLUSTER kT = 3.4 0.6 keV SL2SJ CLEARLY EXTENDED SOURCE (r c = 150 60 kpc, 34 13, = 0.58 0.12) SL2SJ z = STRAIGHT ARC BETWEEN THE TWO GALAXIES SL R E = 6.830.15 SL2SJ JUST A POINT SOURCE DETECTED, HOWEVER VERY SHALLOW XMM EXPOSURE (5 KS) SL2SJ z = EXTENDED STELLAR HALO FOR CENTRAL GALAXY SL R E = 7.500.81 SL2SJ RATHER REGULAR X-RAY EMISSION TEMPERATURE OF KT=3.60.4 SL2SJ CLEARLY EXTENDED SOURCE SL2SJ z = MULTIPLE IMAGES (SOUTHERN ARC MAYBE NOT ASSOCIATED) SL R E = 7.3 0.5 SL+WL+GALAXY DYNAMICS (VERDUGO+11) UNIMODAL NFW W/ c_200 = 6.00.6 AND M_200 1.0 x REPRODUCES WELL ALL THE CONSTRAINTS SL2SJ EVIDENCE FOR A SINGLE HALO: FIT A SINGLE HALO IN SL, NO OPTICAL SUBSTRUCTURE (MUNOZ+11, IN PREP) X-RAY EXTENDED BUT NOT ENOUGH COUNTS FOR SPECTRAL INFORMATION SL2SJ z = BIMODAL LUMINOSITY DISTRIBUTION (TWO DISTRINCT SUBGROUPS FROM SPECTROSCOPY WITH A VELOCITY DIFFERENCE OF 1200 km/s, MUNOZ+13). PERTURBED LENSING CONFIGURATION WHICH REQUIRES EXTERNAL MASS (LIMOUSIN+10) SL R E = 5.5 0.1 SL2SJ ELONGATED X-RAY EMISSION TEMPERATURE OF KT=2.70.4 SL2SJ CLEARLY EXTENDED SOURCE (r c = 128 56 kpc, 26 11, = 0.52 0.07) SL2SJ : THE BULLET GROUP SEPARATION BETWEEN X-RAY GAS AND GALAXIES THE BULLET GROUP SEPARATION BETWEEN THE X-RAY PEAK AND THE GALAXY ASSOCIATED WITH THE LENS OF 22 (109 Kpc) WHY LOOKING FOR BULLETS ? Galaxies (5%) Intra-cluster medium (ICM) Thermal plasma X-rays (10-30%) Dark Matter Gravitational potential 1E THE BULLET CLUSTER MARKEVITCH+04 CONSTRAINTS ON DM SELF- INTERACTION CROSS SECTION RANDALL+08 BABY BULLET (MACS J0025) BRADA+08 SHAN+10 SL2S J08544 BULLETTICITY MASSEY+11 BULLETTICITY Measurement of a statistical signal using lensing (Euclid) and X-ray surveys (EROSITA) BULLETTICITY MASSEY+11 BULLETTICITY FORERO-ROMERO+11 CONCLUSIONS Mass constraints for X-ray bright groups derived from good quality Chandra and XMM data can be of the same quality as obtained for hot, massive clusters. This crucial mass regime has provided the crucial evidence of the decrease of c with increasing M. Gas fraction reveal a more dramatic effect of feedback on these low mass scale The group environment is a nice environment to study the effect of sloshing Lensing groups will play an increasing role in the future with large area surveys Concentrations for relaxed halos are larger by 10% compared to the whole population (Jing 2000, Wechsler 2002, Maccio 2006). They show also smaller scatter ( logc 0.10) Wechsler et al Selection Effects AWM4 AND AGN FEEDBACK Gastaldello+08, see also OSullivan+05, Giacintucci+08 AWM4 AND AGN FEEDBACK Gastaldello+08 Its also a fossil system (Zibetti+08) AWM4 AND AGN FEEDBACK Inspired by Donahue+05 AWM4 AND AGN FEEDBACK Bauer+05 CC NCC CC NCC De Grandi & Molendi 01 EVERY RADIO BCG HAS A COOL CORE (?) Sun+09 X-RAY CORONAE Sun+09Abell 3627 AWM4 AND AGN FEEDBACK Gastaldello+08 Sun+09 AWM4 AND AGN FEEDBACK Cavagnolo+08 X-RAY SYSTEMATICS 1.HYDROSTATIC EQUILIBRIUM 2.MULTIPHASE GAS/PROJECTION EFFECTS IN CORES 3.DISCRETE SOURCES IN Es 4.BKG SUBTRACTION 5.DEPROJECTION AND FITTING PROCEDURES Chandra inner regions XMM outer regions NGC 533 DATA ANALYSYS DATA ANALYSIS Chandra is crucial in the inner region where a steep temperature gradient is present When data are available, we use Chandra in the core and XMM in the outer regions MULTI T UNRESOLVED POINT SOURCES BKG SUBTRACTION Bkg subtraction always crucial of course because of low surface brightness but different respect to clusters: particle background is not so crucial, important are the galactic components (and SWCX, we should routinely check for it, e.g. Carter & Sembay 08) We completely model the various bkg components (e.g. Lumb et al. 2002), exploiting the fact that the source component, mainly characterized by the Fe-L shell, is clearly spectrally separated from the other bkg components BKG MODELLING NGC 5044 offset Buote et al. 2004 DATA ANALYSIS NGC 1550 Projection of the 3D and T thus obtained to the results from spectral analysis, including the radial variation of the plasma emissivity (T,Z Fe ). Using an onion peeling deprojection (e.g., Fabian et al. 1981) gives consistent results with the above method Spectroscopic like T problem (e.g., Mazzotta et al. 2004). Folding through responses : no systematic effects