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Galaxy Ecology The role of galaxy environment in determining the star formation history of the universe Michael Balogh ICC, University of Durham Galaxy Ecology 1. Motivation: cosmological context of observations 2. The local universe: 2dF and Sloan surveys 3. Low mass clusters and groups at intermediate redshift 4. Clusters and groups at z~1 and beyond Galaxy Ecology 1. Motivation: cosmological context of observations 2. The local universe: 2dF and Sloan surveys Bob Nichol, Chris Miller, Percy Gomez (CMU), Ann Zabludoff (Arizona), Tomo Goto (CMU, Tokyo), Vince Eke, Richard Bower (Durham), Ian Lewis (Oxford) and many others… 3. Low mass clusters and groups at intermediate redshift 4. Clusters and groups at z~1 and beyond Galaxy Ecology 1. Motivation: cosmological context of observations 2. The local universe: 2dF and Sloan surveys 3. Low mass clusters and groups at intermediate redshift Richard Bower, Roger Davies, Ian Smail, Simon Morris, Dave Wilman (Durham), John Mulchaey, Gus Oemler (Carnegie) 4. Clusters and groups at z~1 and beyond Galaxy Ecology 1. Motivation: cosmological context of observations 2. The local universe: 2dF and Sloan surveys 3. Low mass clusters and groups at intermediate redshift 4. Clusters and groups at z~1 and beyond Fumiaki Nakata, Ian Smail, Richard Bower (Durham) Taddy Kodama, Ichi Tanaka, Toru Yamada (NAOJ) Motivation: Two questions: 1. Why does star formation decline? 2. What physical mechanisms operate in dense environments? Why Does Star Formation Stop? Steidel et al. 1999 SFR ~ (1+z)1.7 (Wilson, Cowie et al. 2002) A) Internal? i.e. gas consumption and “normal” aging B) External? Hierarchical build-up of structure inhibits star formation Galaxy clusters: the end of star formation? Abell 2390 (z~0.23) 3.6 arcmin R image from CNOC survey (Yee et al. 1996) Ha in Abell 2390 Balogh & Morris 2000 3.6 arcmin CNOC: Galaxy populations Measurements of [OII] emission line for galaxies in 15 clusters and the surrounding field at z~0.3 [OII] closely related to star formation rate (SFR) Showed that average SFR within the virialised regions of clusters is much lower than in lower density regions Balogh et al. 1997, ApJ 488, L75 Ha in Rich Clusters at z~0.3 LDSS++ with nod and shuffle sky subtraction, on AAT (Field) Star formation rate is low in all clusters observed Couch et al. 2001 ApJ 549, 820 Balogh et al. 2002 MNRAS, 335, 110 Tying star formation to structure growth Press-Schechter plot of dark matter mass evolution Groups Clusters Normalised to 1011 Mo Clusters are negligible; but groups dominate and evolve strongly Thus, can environmental processes be responsible for SFR evolution? Additional physics? 1. Ram-pressure stripping (Gunn & Gott 1972) 2. Collisions / harassment (Moore et al. 1995) 3. “Strangulation” (Larson et al. 1980; Balogh et al. 2000) Additional physics? 1. Ram-pressure stripping (Gunn & Gott 1972) 2. Collisions / harassment (Moore et al. 1995) 3. “Strangulation” (Larson et al. 1980; Balogh et al. 2000) short timescale Quilis, Moore & Bower 2000 Additional physics? 1. Ram-pressure stripping (Gunn & Gott 1972) 2. Collisions / harassment (Moore et al. 1995) 3. “Strangulation” (Larson et al. 1980; Balogh et al. 2000) important in groups? Additional physics? 1. Ram-pressure stripping (Gunn & Gott 1972) 2. Collisions / harassment (Moore et al. 1995) 3. “Strangulation” (Larson et al. 1980; Balogh et al. 2000) long timescale Timescales Numerical model of infall rate + assumed decay rate of star formation => radial gradient in SFR Radial gradients in CNOC clusters suggest t ~2 Gyr Suppressed star formation within several Mpc of cluster centre! What environment is responsible? Balogh, Navarro & Morris 2000 Diaferio et al. 2001 The local Universe: Going beyond cluster cores… The 2dFGRS and SDSS 1. 2dF Galaxy redshift survey: • • spectra and redshifts for 220 000 nearby galaxies only photographic plate photometry 2. Sloan digital sky survey: • • goal is spectra for 1 million galaxies, with digital photometry (ugriz) First data release contains 186 240 galaxies 2dFGRS/SDSS Part I: 2dF clusters A1620 Rvir Data for 17 Abell-like clusters Covers velocity dispersions 500 km/s - 1100 km/s Region out to > 20 Rvir extracted from the survey Star formation rate measured from Ha 1 degree (data extracted over ~7 deg field) Lewis, Balogh et al. 2002 MNRAS 334, 673 2dFGRS/SDSS Part I: 2dF clusters Normalised star formation rate measured from Ha in 17 nearby clusters Field Critical density: ~group scales Identified a critical density of ~1 Mpc-2, where environmental effects become important This corresponds to low density groups in the infall regions of clusters Lewis, Balogh et al. 2002 MNRAS 334, 673 2dFGRS/SDSS Part I: 2dF clusters Field SFR-Density Relation Field Field Lewis et al. 2002 MNRAS 334, 673 2dFGRS/SDSS Part I: 2dF clusters Field SFR-Density Relation c.f. Morphology-Density Relation R>2 Rvirial Field Field Lewis et al. 2002 MNRAS 334, 673 Star Formation Rate (Mo/yr) 2dFGRS/SDSS Part II: SDSS Field 75th percentile 75th percentile Median Field median Gomez et al. (2003) Galaxy Surface Density (Mpc-2) 2dFGRS/SDSS Part III: Groups Compare groups with clusters and the field: does the large-scale environment play any role? 2dFGRS/SDSS Part III: Groups 2dFgrs Based on a friends-offriends algorithm (Eke et al., in prep) Effective at finding small groups with s«500 km/s SDSS Different algorithm, includes colour information (Miller et al. in prep). Effective at finding more massive groups 2dFGRS/SDSS Part III: Groups SFR of galaxies as a function of group velocity dispersion ● 2dFGRS ● SDSS Mean SFR appears to be suppressed in all galaxy associations at z=0! There is a trend with group mass, but this is due to the different distributions of local densities… Balogh et al., in prep Field 2dFGRS/SDSS Part III: Groups 75th %-tile Field Field Median Red hatched region: all galaxies (~30 000) White lines: groups with indicated s Balogh et al., in prep Luminosity dependence Balogh et al., in prep Does any environment enhance star formation? Close pairs in the SDSS ds~(Dv/250)2+(Dr/100)2 Dv~100 km/s Dr~50 kpc Balogh et al., in prep Close pairs in SDSS groups ds~(Dv/250)2+(Dr/100)2 Dv~100 km/s Dr~50 kpc Balogh et al., in prep Groups at z~0.4 Outskirts of Clusters at z~0.4 Subaru image Abell 851 at z=0.41 30 arcmin Kodama et al. 2001 Outskirts of Clusters at z~0.4 Kodama et al. 2001 Critical density where red sequence first appears. Scrit~4 Mpc-2 Corresponds to density of infalling groups, well outside of cluster Star formation in groups at z=0.2-0.5 1. Low-Lx Clusters at z=0.25 • • Factor ~10 less massive than CNOC clusters HST imaging, extensive ground-based spectroscopy 2. CNOC2 groups at z=0.45 • • Spectroscopy with LDSS-2 on Magellan 6.5-m Goal is complete group membership to M*+1 Low Lx Clusters at z~0.25 Cl0841 z=0.24 s=390 Cl0849 z=0.23 s=750 Cl1701 z=0.24 s=590 Cl1702 z=0.22 s=370 Cl0818 z=0.27 s=630 Cl0819 z=0.23 s=340 Cl1309 z=0.29 s=640 Cl1444 z=0.29 s=500 Lx ~ 1043 - 1044 ergs/s, ~ 10 X less massive than CNOC Morphology-density relation at z~0.25 Some evidence that disk galaxies are more common in groups than clusters, for a given local density. Low Lx (groups) The same is not true of star formation rates, however… High Lx (clusters) Balogh et al. 2002 ApJ 566, 123 Star Formation in Low-Lx Clusters Balogh et al. 1997 Spectroscopy for 172 cluster members Mr< -19 (h=1) SFR from [OII] emission line Distributions of massive and low-mass clusters are identical! Therefore, there must be a population of diskdominated galaxies with low SFR… Balogh et al. (2002) MNRAS, 337, 256 Disks Without Star Formation Cl 1309 id=83 z=0.2934 [OII] B/T = 0.39 Wo (OII)=-2.64.0 Wo (Hd)=3.8 2.1 3” HST Image Disks Without Star Formation [OII] Cl 1444 id=78 z=0.2899 B/T = 0.42 Wo (OII)=3.5 2.7 Wo (Hd)=4.9 1.3 3” HST Image Disks Without Star Formation Cl 0818 id=58 z=0.2667 [OII] B/T = 0.19 Wo (OII)=-9.6 7.8 Wo (Ha)=22.1 11.6 Wo (Hd)=2.0 3.6 3” HST Image Ha Disks Without Star Formation Cl 0841 id=20 z=0.2372 [OII] B/T = 0.42 Wo (OII)=-0.2 1.2 Wo (Ha)=-1.4 0.6 Wo (Hd)=0.0 0.6 3” HST Image Ha CNOC2 Groups 1. Identified a sample of groups from original survey (Carlberg et al. 2001 ApJ 552, 427) 2. Properties of these groups can be directly compared with low redshift counterparts from 2dFgrs and SDSS 3. Durham involvement: follow-up observations with Magellan to gain higher completeness confirming complete samples of group members using LDSS-2 CNOC2 Groups at z~0.45 Deep spectroscopy with LDSS-2 on Magellan 1 (~30 groups) Infrared (Ks) images from INGRID Combined with CNOC2 multicolour photometry and spectroscopy, we can determine group structure, dynamics, stellar mass, and star formation history. LDSS2 on Magellan [OII] [OII] 30 CNOC2 groups at z~0.45 20 10 15 Within ~1 Mpc of group centre, galaxy SFR is low relative to surrounding field 5 Compare with z=0 data to establish evolution of the “critial” density 0 Mean EW [OII] (Å) 25 Preliminary result for 7 groups 0 0.5 1.0 1.5 2.0 2.5 Distance from centre (Mpc) Wilman et al. in prep. CNOC2 Groups at z~0.45 Preliminary results based on only 12 CNOC2 groups Have observed >30 groups to date Preliminary results for 13 Balogh et al. groups show excess star 1997 formation in groups, compared with rich clusters. But is this due to differences in density distributions? Wilman et al. in prep Implications? Implications: SFR Evolution Scrit (z~0) ~ 1 Mpc-2 (Lewis et al. 2002) Scrit (z~0.4) ~ 4 Mpc-2 (Kodama et al. 2001, corrected) Critical density -0.6 0.6 1.6 Implications: SFR Evolution Global SFR evolves as (1+z)1.7 So increases by ~70% between z=0 and z=0.4 This is consistent with an unevolving SFR-density correlation if most of the mass in Universe at z~0.4 is below Scrit However, nature of SF must be different at z~1 Implications: SFR Evolution Global SFR evolves as (1+z)1.7 So increases by ~70% between z=0 and z=0.4 70% increase? This is consistent with an unevolving SFR-density correlation if most of the mass in Universe at z~0.4 is below Scrit However, nature of SF must be different at z~1 Implications: Physical mechanisms Ram-pressure stripping Strangulation Galaxy interactions Implications: Physical mechanisms not important in groups Ram-pressure stripping Strangulation Galaxy interactions Implications: Physical mechanisms Ram-pressure stripping Strangulation no dependence on s Galaxy interactions Clusters and Groups at z~1 Groups at z > 1 1. Deep multicolour (VRi′z′JKs) images of Lynx and Q1335+28 (z=1.2). 2. Proposals to observe high redshift radio galaxies and radio-loud quasars: known to reside in dense environments • • IRIS2 narrow band Ha and [OIII] at z=2.3 GMOS/FORS2 narrow band filter + grism Ha and [OII] spectroscopy at z=1.4, 1.47, 2.3 Lynx clusters: z=1.2 Subaru VRi’z’ INGRID JKs Y (arcmin) Identified 7 groups around the clusters from photometric redshifts. GMOS spectroscopy pending X (arcmin) Nakata et al. (2002) Groups around the Lynx clusters Group at z=1.27, ~3 Mpc from main cluster GR3 CMR is present, perhaps with more scatter and fewer bright galaxies CL1 CL2 Nakata et al. in prep Groups around the Lynx clusters M*clus ~ 20.13 M*group ~ 21.80 Nakata et al. in prep Overdensities around HizRG z=1.44 z=1.59 Best et al. 2003 Conclusions 1. Clusters and groups have a large impact on galaxy star formation rates at the present day 2. Bright galaxies have little density dependence; trends driven by faintest galaxies 3. Observations just consistent with explanation of global SFR evolution to z~0.4 as due to growth of clustering 4. Most likely physical mechanism for transformation is galaxy-galaxy interactions.