cluster really a galaxy? IGPP Seminar talk, June 26, 2008 Work in progress: ESO Conference, Munich, July 21-25, 2008 “Chemical Evolution of Dwarf Galaxies and Stellar Clusters”
- a small sphere - roughly 160 globulars (GCs) in the Milky Way - 90% lie within 100,000 light-years (0.5r stellar halo) - single age (old !13 Gyr), single (low) metallicity populations (all stars form at the same time) - Very little or no HI gas and dust (stars + stellar winds drive out gas) - M/L ratios ≈ 1 (unlike galaxies - NO DARK MATTER) - typical effective radii of r e = 3-5 pc Back seat bandits: Omega Centauri (ωCen) - old (12 Gyr), massive (5 x 106 M¤) - metallicity spread (several generations of stars) core of a tidally stripped dwarf galaxy? - contains a 4 x 105 M¤ BH (Gemini observations) M15 : massive and most dense GC (core collapse), probably contains a central black hole.
mass of the MW - roughly 460 GCs Back seat bandits: Mayall/G1 : - massive (10 x 106 M¤) x2 mass of ωCen - metallicity spread (several generations of stars) core of a tidally stripped dwarf galaxy? - large ellipticity Mayall II is named after Nicholas U. Mayall and O.J. Eggen in 1953. Sidney van den Bergh named it G1 in 1977.
d=20 Mpc, 30’~183 kpc) - NGC1399: v =1425 kms-1 (top right) is the central galaxy. - The first compact object to be discovered is near NGC1404 (v=1947 kms-1) and has v =1591±36 kms-1. Intracluster GCs? The first hints… 1996: (Minniti et al. 1996). Small survey of NGC1399 globular clusters Object near NGC1404s identified as a very compact dwarf galaxy: V=18.5, (V- I) = I.48 1999: (Hilker et al. 1999) Images a large number of Fornax galaxies. Two compact objects are spectroscopically confirmed to be cluster members. “..can be explained by a a very bright GC or a compact elliptical like M32. Another explanation may be that these represent the nuclei of dwarf elliptical galaxies.” Image: CTIO 4m MOSAIC (g’,r’,i’), Karick, Gregg & Drinkwater
et al. 2002) Extremely luminous star clusters formed in galaxy interactions. (Fellhauer & Kroupa 2002, Maraston et al. 2004) Remnant nuclei of dE,Ns or low luminosity spirals which have been tidally disrupted or “threshed” during passages close to the central cluster galaxy, NGC1399. (“UCDs”: Bekki et al. 2001, 2003) Extreme cases of known galaxies. (e.g. dE,Ns with very faint halos) Highly compact galaxies formed in the early Universe? (Blanchard et al. 1992, Tegmark et al. 1997) - is there an upper mass limit for normal GCs? - are the ICOs single age and metallicity like MW GCs? - do the ICOs fall on the L ∝ σ 1/4 relation or is there are turnover point? - smooth radial distribution? - ICOs should be more concentrated than dEs - requires low σ, radial orbits and very compact cores ωCen, M22, G1? - ICOs should be more metal rich? - mixed ages? W3? Possible explanations for IGCs
UCDs and a comparison Fornax Cluster dE,N, FCC303 (Drinkwater et al. 2003) UCD profiles are well fitted by King and de Vaucouleurs R1/4 law profiles. Effective radii range from, r e = 10-22 pc. UCD3, the most luminous UCD, required a 60 pc scale length exponential halo. FCC303 (dE,N) has an 8 pc core and a 300 pc halo. FCC303 UCD1 UCD2 UCD3 UCD4 UCD5 Galactic GCs have typical effective radii of r e = 3-5 pc. The most compact normal dwarf galaxies in the Virgo Cluster have scale lengths of 160 pc.
of 5 UCDs and a comparison dE,N, FCC303 (Drinkwater et al. 2003 & Evstigneeva et al. 2007) Velocity dispersions range from, σ = 24 - 37 km s-1 considerably higher than Galactic GCs. UCDs lie well off the GC: L ∝ σ1.7 relation in a previously unoccupied region, but on an extrapolation of the elliptical galaxy: L ∝ σ4 Faber-Jackson relation. Combining the HST data, mass-to-light ratios range from M/L ~ 2 - 4 solar masses. The largest GCs in M31 have M/L ~ 1-2 solar masses. The location of the UCDs and dE,Ns supports the “galaxy threshing” model (Bekki et al. 2001, 2003). A normal dE,N halo, accounting for ~98% of the dE,Ns luminosity is tidally stripped, reducing the total luminosity by a factor of 100 but barely changing the central velocity dispersion. Over time this disruption contributes diffuse stellar material to the ICM. The surviving nuclei are dispersed into intra cluster space or added to the envelopes of brighter galaxies where they can masquerade as stars.
5 UCDs and FCC303 (Gregg 2008., in prep) Observations taken in September 2003 Short exposures but good S/N. 6Å resolution. UCD2 and UCD6 both have stronger Ca II H absorption than Ca II K, indicating a younger, ~1-3 Gyr stellar component. UCD1 has strong Mg, Hb absorption as well as a strong CN feature, similar to NGC1399. This suggests that it may have started out as a larger more metal rich stellar system.
1786 Å (GALEX) Near UV: 1771 - 2831 Å (GALEX) - hand wavy explanation: UV light traces star formation - the UV light of an integrated population is an effective age indicator and can be used to break the well known “age-metallicity” degeneracy. HOW? - the far UV is sensitive to the excess UV emission produced by EXTREME (Teff > 15,000K) horizontal branch stars (EBH). This “UV-excess” is observed in many early-type (elliptical) galaxies. Elliptical galaxies and large spiral bulges exhibit this excess for λ < 2000A by stars with T~22,000K WHY? - EBH population is governed mainly by envelope mass-loss processes on the RGB and by the helium abundance, which in-turn is sensitive to the age and metal abundance of stars.
(5 x 106 M¤) - metallicity spread (several generations of stars) core of a tidally stripped dwarf galaxy? - contains a 4 x 105 M¤ BH (Gemini observations) Double MS - large variation in He abundance - large enrichment parameter (>90, ~2 for MW stars) - larger number of “hot” stars - large FUV flux Canonical Old SP models: For a given metallicity, the Universe needs to be ~3-5 Gyr older than WMAP. i.e. normal level of He enrichment Would take longer to output the Observed UV flux.
the Milky Way - 90% lie within 100,000 light-years (0.5r stellar halo) - single age (old !13.2), single (low) metallicity populations (all stars form at the same time) - Very little or no HI gas and dust (stars + stellar winds drive out gas) - M/L ratios ≈ 1 (NO DARK MATTER) - typical effective radii of r e = 3-5 pc The rest of the Milky Way do not exhibit the same FUV-excess seen in ωCen. Neither do the M31 Globulars
66 GCs with STIS (NUV+FUV) and optical photometry. - distinct UV-optical properties compared to MW and M31 GCs. - the most metal rich are near solar and overlap the local E galaxy sample in terms of their Mg2 line indices.