Survey
* Your assessment is very important for improving the workof artificial intelligence, which forms the content of this project
* Your assessment is very important for improving the workof artificial intelligence, which forms the content of this project
Globular Clusters and Galaxy Formation Duncan A. Forbes Centre for Astrophysics & Supercomputing, Swinburne University Collaborators - SAGES Project Mike Beasley (Swinburne) Jean Brodie (Lick Observatory) John Huchra (Harvard-Smithsonian) Markus Kissler-Patig (ESO) Soeren Larsen (Lick Observatory) Telescopes Globular Clusters • Bound homogeneous collections of ~105 M • All galaxies with MV < -15 have at least one globular, some have over 10,000 • They have a universal luminosity function which gives the Hubble constant accurate to 10% • Share the same star formation and chemical enrichment history as their host galaxy. • Provide a powerful and unique probe of galaxy formation. Two sub-populations Most (perhaps all) large galaxies reveal two distinct sub-populations of globular clusters. [Fe/H] V-I = -1.5 0.95 -0.5 1.15 Why study extragalactic GCs ? • The MW has only 140 known GCs, M31 has ~400, M87 has ~10,000 • The Local Group has no giant ellipticals • Probe to higher metallicity GCs • Same distance and reddening • No foreground stars in the GC spectra • Discover something new ! Extragalactic Globular Cluster Database: http://astronomy.swin.edu.au/dforbes Local Group GCs (D ~1 Mpc) 3-6m telescopes Photometry Spectra (V ~ 16) • CMD Morphology [0.1” ~ 0.4 pc] • Metallicities • Optical colours • Infrared colours • Abundances • Relative Ages • System Kinematics • Sizes Brodie & Huchra 1990, 1991 Virgo/Fornax GCs (D ~15 Mpc) 8-10m telescopes Photometry Spectra (V ~ 22) • Optical colours (~50) • Metallicities (~10) • Infrared colours (~4) • Abundance ratios (~6) • Sizes (~20) • Relative Ages (~6) [0.1” ~ 7 pc] • System Kinematics (~4) Milky Way Globular Cluster System Sub-populations: Metal-rich ~50 Metal-poor ~100 Bulge (RGC < 5 kpc) Old Halo (prograde) Thick disk (RGC > 5 kpc) Young Halo (retrograde) Young halo + 4 Sgr dwarf GCs = Sandage noise Milky Way Bulge Clusters The inner metal-rich GCs are: • spherically distributed • similar metallicity to bulge stars • similar velocity dispersion to bulge • follow the bulge rotation => associated with the bulge Minniti 1995 Bulge Clusters in M31 and M81 The inner metal-rich GCs are: • spherically distributed M31 M81 • similar metallicity to bulge stars M31 M81? • similar velocity dispersion to bulge M31 M81 • follow the bulge rotation M31 M81 The Sombrero Galaxy Metallicities Number of metal-rich GCs scale with the bulge Forbes, Brodie & Larsen 2001 Globular Clusters in M104 M104 M31 MW Sa Sb Sbc Metal-rich GCs 667 100 53 Bulge-to-total 0.80 0.25 0.19 Disk SN 4.2 0.21 0.19 Bulge SN 1.1 0.63 0.84 Hubble type The metal-rich GCs in M104 must be associated with the bulge not disk component. GCs in Spirals Inner metal-rich GCs in spirals are associated with the bulge not the disk. The number of bulge GCs scales with bulge luminosity (bulge SN ~1). Forbes, Brodie & Larsen 2001 The Elliptical Galaxy Formally Known as The Local Group M31+MW+M33+LMC+ SMC+... gE with MV = – 22.0 and N = 700 +/- 125 Universal luminosity function Local Group Elliptical Metallicity peaks at [Fe/H] = –1.55, –0.64 Ratio 2.5:1 SN = 1.1 -> 2.5 S + S -> gE with low SN Forbes, Masters, Minniti & Barmby 2000 Numbers, Specific Frequency • The bulge SN for spirals is ~ 1 • The total SN for field ellipticals is 1-3 (Harris 1991) • The fraction of red GCs in ellipticals is about 0.5 • The bulge SN for field ellipticals is ~1 => Spirals and field ellipticals have a similar number of metal-rich GCs per unit starlight. Luminosities A Universal Globular Cluster Luminosity Function MV Ellipticals –7.33 +/- 0.04 1.36 +/- 0.03 Spirals –7.46 +/- 0.08 1.21 +/- 0.05 Ho = 74 +/- 7 km/s/Mpc GCLF Ho = 72 +/- 8 km/s/Mpc HST Key Project Harris 2000 Sizes For Sp S0 E cD the GCs reveal a size– colour trend. The blue GCs are larger by ~20%. This trend exists for a range of galaxy types and galactocentric radii. Larsen et al. 2001 Metallicities All large (bulge) galaxies reveal a similar GC metallicity distribution. All ( MV < –15 ) galaxies, reveal a population of GCs with [Fe/H] ~ –1.5. The WLM galaxy has one GC, [Fe/H] = –1.52 age = 14.8 Gyrs (Hodge et al. 1999). Metallicity vs Galaxy Mass Blue GCs <2.5 V–I ~ 0.95 Pregalactic ? Red GCs ~4 Spirals fit the trend Forbes, Larsen & Brodie 2001 Metallicity vs Galaxy Mass Red GC relation has similar slope to galaxy colour relation. Red GCs and galaxy stars formed in the same star formation event. Forbes, Larsen & Brodie 2001 Colour - Colour Galaxy and GC colours from the same observation. The red GCs and field stars have a very similar metallicity and age. Also NGC 5128 (Harris et al. 1999) Bulge C-T1 colour Forbes & Forte 2001 Spatial Distribution Red GCs are centrally concentrated, have similar azimuthal and density profile to the `bulge’ light. Blue GCs are more extended. Does the blue GC density profile follow the X-ray/halo profile ? Ellipticals Blue Halo Red `Bulge’ Red ? Spirals Halo Bulge Disk Summary from Photometry Blue GCs = halo common to all galaxies [Fe/H] ~ –1.5 constant colour Pregalactic ? Red GCs = bulge [Fe/H] ~ –0.5 colour varies with galaxy mass formed in same event as bulge stars NGC 1399 NGC 1399 GC Ages ~3.5hrs on Keck 10m blue Hß error = +/- 0.2 to 0.3 A 1.6 Gyr NGC 1399 2.3 Gyr -2.2 < [Fe/H] < 0.3 ages ~ 12 Gyrs red 12 Gyr (some young GCs) Caveat: BHBs LRIS spectra, 2hrs Abundance Ratios High S/N spectra of GCs in ellipticals suggests that all GCs have supersolar alpha abundance ratios, eg [Mg/Fe] ~ +0.3 (similar to the MW). Supersolar ratios indicate the dominance of SN II vs SN Ia products in the GC-forming gas. This is due to: • short time formation timescale • IMF skewed to high mass stars => important chemical evolution clues [Note: Maraston etal 2001 found solar ratio protoGCs in the ongoing merger NGC7252] System Kinematics M49 M49 red low ~ galaxy blue high , rotate M87 red ~ blue, rotate No general trends Zepf etal. 2000 GC Formation Scenarios • Mergers of spirals (Ashman & Zepf 1992) • Two-phase collapse (Forbes, Brodie & Grillmair 1997) • In situ plus accretion (Cote, Marzke & West 1998) Merger Model Ashman & Zepf 1992 Merger Model Merger Model Meanwhile, 10 billion years later... Merger Model Multi-phase collapse model Pre-galactic Phase Galactic DormantPhase Phase clumpy collapse of additional gas collapse star formation gas cloud stopped by SNII formation of metal-rich formation of metalglobulars and bulge gas reheated by SNIa poor globulars stars and a gas cools few halo stars T=0 T=2 Forbes, Brodie & Grillmair 1997 Multi-phase collapse model Mike Beasley Duncan Forbes Ray Sharples Carlton Baugh • Merging of Dark Matter halos using Monte-Carlo method yielding ‘Merger Trees’. • Gaseous fragments form some metal-poor stars and GCs before the main galaxy. • Gaseous pre-galactic fragments may merge/collapse forming a burst of stars that results in an elliptical galaxy. The bulk of stars are formed in this burst. • Hot gas cools onto the elliptical galaxy, forming a cold gas disk over time and hence a spiral galaxy. Merger Tree Simply taking a fraction of the stars formed in the model produces a skewed, unimodal distribution in V-I. [Fe/H] Assuming that the efficiency is dependent upon the SFR (e.g. Larsen 2000) produces a sharper unimodal peak. Truncating the blue GC formation at high-redshift produces a bimodaldistribution. V-I GC Colour Diversity After correcting for magnitude incompleteness and limited areal coverage, the model can reproduce the diversity of GC colour distributions seen with HST (eg Larsen etal. 2001) GC Number vs Host Galaxy Luminosity The model galaxies (small circles) are well matched to the observations (red symbols). The purple line shows constant GC formation efficiency. A Massive Elliptical Age ‘peak’ of blue GCs is a result of truncation at high redshift. Ages of red GCs show a greater range and appear ‘bursty’. Old ages and particularly bimodal metallicity distributions lead to bimodal colour distributions. Model What drives SN ? The plot shows model galaxies (blue), data (red) and the spiralspiral merger model of Bekki etal. (green). High SN galaxies are associated with large numbers of blue GCs, not red GCs as expected in spiralspiral mergers. Evolution in SN For most ellipticals there is very little evolution in SN in the last ~10 Gyrs. In the low luminosity elliptical, SN increases from 4.5 to 4.7 as the result of a major merger 4 Gyrs ago. MB = -22.0 MB = -20.4 SN of young ellipticals Galaxy Merger Age SN NGC3156 1 Gyr 0.3 NGC1700 2 Gyr 1.4 -> 2 NGC6702 2 Gyr 2.3 -> 4 NGC1316 3 Gyr 1.5 -> 2 NGC3610 3 Gyr 1.1 Old ellipticals have SN ~ 3 (field) to 6 (cluster) GC Metallicity vs Mass The red model GCs, are generally consistent with the data, but do not have the same slope. The blue model GCs behave similarly to the red GCs, but with less scatter. GC Age Predictions Age The mean age of red GCs shows a strong dependence on dark matter halo velocity (mass). log The model predicts that low-L and field galaxies have younger red GCs. N Age NGC 1399 NGC 1399 GC Ages ~3.5hrs on Keck 10m blue Hß error = +/- 0.25 A 1.6 Gyr NGC 1399 2.3 Gyr -2.2 < [Fe/H] < 0.3 ages ~ 12 Gyrs red 12 Gyr (some young GCs) LRIS spectra, 2hrs Observational Summary • The inner metal-rich GCs in the Milky Way and other spirals have a bulge (not disk) origin. • The GC systems of spirals and ellipticals show remarkable similarities. • Blue and red GCs have similar ages ~12 Gyrs (but red GCs could be younger by 2-4 Gyrs) • Some very young (~2 Gyrs) GCs have been found in `old’ ellipticals. • Blue and red GCs have [Mg/Fe] ~ +0.3. • Red GCs trace elliptical galaxy star formation. Model Predictions Our model (Beasley etal. 2002) of GC formation in a Hierarchical Universe assumes truncation of blue GCs at z = 5, and predicts: • SN is determined at early epochs; late stage mergers have little effect on SN • Blue GCs formed ~12 Gyrs ago in all ellipticals. • Red GCs have a mean age of ~8-10 Gyrs in field and low luminosity ellipticals. • In general: spirals and ellipticals have similar GC systems. Future Developments • HST+ACS U-band and 8m wide-field K-band imaging studies (eg Puzia etal) • Age structure within the red GCs (eg Beasley etal) • Nature of the new large (Reff ~ 10 pc) red low luminosity (MV ~ -6) clusters (eg Brodie & Larsen) • Importance of stripped nucleated dE (eg Bekki etal) • HST+ACS CMDs for Local Group GCs (eg Rich etal) • Halo mass estimates: GC kinematics vs X-rays • Better SSP grids (eg BHBs, AGB, supersolar) Formation Timeline 12 Gyrs Blue GCs form in metal-poor gaseous fragments with little or no knowledge of potential well. Halo formation. 8-11 Gyrs Clumpy collapse/merger of gaseous fragments form metal-rich red GCs and `bulge’ stars. Late epoch mergers of Sp + Sp (low SN) E Time http://astronomy.swin.edu.au/dforbes Number per unit Starlight McLaughlin (1999) proposed a universal GC formation efficiency = MGC / Mgas + Mstars = 0.26 % Mgas = current Xray gas mass Ntot ~ L 2 = 0.2% NGC 5128 Reveals a mostly metal-rich halo, which has similar metallicity to the metal-rich globular clusters. Harris etal 1999