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Galactic surveys 1: The giant spiral galaxy NGC 1365 – what we often think of as a “typical” galaxy. (ESO VLT) 2: The Small Magellanic Cloud, an irregular galaxy once thought to represent the faint end of the distribution of galaxy luminosities. (AAO) 3: The dwarf elliptical galaxy M32 superimposed on the disc of its giant neighbour M31, showing the contrast in sizes (INT image by David Malin). M32 has a truncated light distribution suggesting outer stars may have been stripped away by tidal forces. Small galaxies are New telescope technology and major sky surveys are finding more and more dwarf galaxies. Steve Phillipps discusses how this growing population may hold the clues to understanding a range of galaxy collisions and interactions. G alaxies are supposed to be huge aggregates of hundreds of billions of stars and have the spectacular appearance we see in “coffee table” books. Indeed, in the early days of extragalactic astronomy it was thought that most galaxies were of rather similar (large) luminosities. Specifically, Edwin Hubble (1936) and his contemporaries believed that the luminosity function (LF) of galaxies, that is the number of galaxies per unit volume of different luminosities, was a peaked, roughly Gaussian shaped curve. Known local galaxies spanned the range from the giant spiral M31 in Andromeda and our own galaxy, with luminosities of a few 1010 L (absolute magnitudes MV ≈ –21), through smaller irregular systems like the Small Magellanic Cloud (MV ≈ –17), down to the dwarf elliptical galaxy companion to M31, NGC 147, about 250 times less luminous than M31 itself (i.e. MV ≈ –15). This was a very much smaller range than seen for stars: even main sequence stars have a range of at least a factor 108, with the Sun (logarithmically speaking) somewhere near the middle. We might note though that the range of stellar masses is quite narrow, only around a factor 103. This galactic uniformity was disturbed in 1938 when Hubble’s great rival Harlow Shapley reported the discovery of two very faint Local Group galaxies, known as the Fornax and Sculptor dwarfs, after the constellations in whose direction they appear to lie. Strictly 6.6 speaking they were apparently first noted by Harvard College Observatory assistant astronomer Sylvia Mussells on plates taken by Shapley (see A&G 2003 45 1.18). Sculptor, in particular, was very much less luminous (by another factor ~100) than previously known galaxies – with modern distance estimates it has MV ≈ –10 – and these two were the first examples of dwarf spheroidal galaxies. They were discovered only because they were close enough for individual bright stars in them to be resolved – indeed, they are satellites of our own galaxy. Their averaged-out surface brightness (i.e. luminosity per unit area) would have been far too low to be detectable on the photographic emulsions available in the 1930s. Even at a dark site, the night sky brightness – due to a combination of airglow in our atmosphere, sunlight reflected off dust grains and the general stellar light in our galaxy, among other things – is an order of magnitude brighter than even the central regions of a dwarf spheroidal. Such dwarfs therefore suffer a problem generic to all low surface brightness galaxies, that is a poor contrast against the overall sky brightness. This difficulty is epitomized by the Fornax dwarf itself, which has a total magnitude around mV = 7.3. A star of this magnitude would be visible with a pair of binoculars, let alone a long photographic exposure on a large telescope. The arrival of dwarf spheroidals on the scene implied that galaxies could be much more Abstract Galaxies are not always giant collections of billions of stars. Since the 1930s, when Harlow Shapley discovered the first dwarf spheroidal galaxies, technology has allowed the detection of ever fainter galaxies in our immediate neighbourhood. Our galaxy is now known to have a whole retinue of very small satellite galaxies, the lowest luminosity examples of which can hardly outshine one massive star. Some galaxies appear to be getting physically smaller. Evidence for this is found in the streams of stars detected around our galaxy and elsewhere and in galaxies that appear to have had their outer regions truncated. Recent surveys of galaxy clusters have revealed another new class of object, the ultra-compact dwarfs. Though no less luminous than other dwarf galaxies, their physical sizes, of order 20 pc, are far below anything previously seen. They are reminiscent of the nuclei of dE,N type galaxies and may well be descended from them via some destructive processes within galaxy clusters. varied than hitherto believed. As Shapley (1943) himself put it, “two misty patches have put us in a fog”. In the 1950s Fritz Zwicky proposed an alternative view. Zwicky was famous for usually having an alternative view and in this case it was that – as with most things astronomical, from stars to meteorites – there should be a steady increase in numbers towards smaller December 2004 Vol 45 Galactic surveys 4: The Fornax dwarf spheroidal galaxy, first reported by Harlow Shapley in 1938. (UKST) 5: The very faint and diffuse Carina dwarf spheroidal was first seen in 1977 on the UKST plate reproduced here. 6: And IX, the most recently discovered of M31’s companions and the lowest luminosity galaxy currently known. (INT image from Zucker et al. 2004 ApJ) growing smaller objects. Support for this view, with the LF rising at the faint end, soon came from Kiang (1961) and others, from consideration of local galaxies, and from George Abell (1962) for galaxies in clusters. Subsequent work has confirmed this in general terms, though the slope of the faint end of the LF remains a contentious issue. This is primarily because of the strong selection effects biasing us against including low luminosity, low surface brightness objects in galaxy catalogues or other galaxy samples. A similar effect had been seen for stars; the apparently brightest stars seen in the sky include a preponderance of stars much brighter than the Sun, but a volume-limited sample of nearby stars reveals that most stars are really considerably less luminous than the Sun. As we have seen, for dwarf galaxies this effect is compounded by their low surface brightnesses. Unsurprisingly then, further detections of very small and/or low luminosity galaxies remained confined to the local universe, indeed to the Local Group of galaxies. Further examples of dwarf spheroidals were discovered in the 1950s by Harrington and Wilson in the Palomar Schmidt Sky Surveys. Again these were immediate companions (satellites) of our own galaxy, less than 200 kpc away and even smaller and fainter than Fornax. Indeed, Wilson’s (1955) Ursa Minor and Draco dwarf spheroidals were even fainter than Sculptor and remained the faintest known galaxies for many years. By 1977, when Russell Cannon, Tim Hawarden and Sue Tritton discovered the remarkably inconspicuous Carina dwarf spheroidal on a plate taken for the UK Schmidt Telescope (UKST) southern sky survey, our December 2004 Vol 45 galaxy had acquired the correct fairy-tale complement of seven dwarfs as companions. Carina itself has a luminosity 5 × 105 L and an effective radius (i.e. the radius containing half of its total light) about 250 pc. The galactic satellite with the lowest luminosity is still the Ursa Minor system (MV ≈ –8.5, L ≈ 2 × 105 L), while the dwarf satellite with the lowest surface brightness (as judged from star counts) is probably Draco (equivalent to 26.3B magnitudes per square arc second, or 2 L/pc2 at the centre). However, the physically smallest of our galaxy’s dwarf companions is Leo II with an effective radius re ≈ 170 pc. It is more luminous than the likes of Draco or Carina because of its rather higher surface brightness. (Excellent surveys of the properties of the galaxy’s dwarf satellites are given by Irwin and Hatzidimitriou [1995], Mateo [1998] and van den Bergh [2000].) We should also note that M31 has its own retinue of satellites. For many years the only ones known were the quite moderate brightness dwarf ellipticals M32, NGC 205, NGC 185 and the fainter NGC 147. And I, II and III were discovered by Sydney van den Bergh in 1972, but M31 still lagged the galaxy in terms of the number of companions until quite recently. (The galaxy now has 12 known satellites, including the Magellanic Clouds.) There was always the suspicion that this shortfall might be due to the greater difficulty of detecting faint dwarfs at the distance of M31 (≈ 800 kpc) and the last few years has seen the addition of And V up to And IX (the proposed And IV is now thought not to be a genuine galaxy). And IX, which was detected only in the last year (Zucker et al. 2004) is probably of even lower luminosity than the Ursa Minor dwarf, with an absolute magnitude MV ≈ –8.3, though this is still somewhat uncertain. And IX was discovered as an excess in projected stellar density in the Sloan Digital Sky Survey (SDSS) data just 2.6° (a projected distance of 34 kpc) from the centre of M31. Allowing for the contribution of fainter, unseen stars, the central surface brightness also seems to be the lowest yet recorded, at 26.8 V magnitudes per square arc second (less than 1 L /pc2). M32 remains the oddest of the companions, though, because of its high central surface brightness but comparatively small size. In some ways it looks like a “chopped down” version of a giant galaxy and it has been hypothesized that it may represent just the central remnant of a once much bigger galaxy that lost most of its outer stars via gravitational tidal effects as it passed close by M31. If we could reverse our viewpoint and look at our galaxy from Andromeda, we might see a rather similar situation. In 1997 Rodrigo Ibata, Gerry Gilmore and Mike Irwin discovered a coherent stream of stars in nearly the same direction as, but moving at different radial velocities to, those in the galactic centre region. This was identified as a companion galaxy to our own, actually plunging through the galaxy’s disc on the opposite side to the Sun and only 12 kpc from the centre. A huge plume of stars trails (and precedes) the Sagittarius dwarf spheroidal (as it became known), clear “smoking gun” evidence for the tidal destruction of satellite galaxies. As the loss of stars is preferentially from the less tightly bound outer regions, we can anticipate that Sagittarius will end up looking like a rather small remnant of its former self. 6.7 Galactic surveys 7: The Sagittarius is currently plunging through the galaxy’s disc, on the opposite side to where the Sun lies. The huge trail of tidally removed stars can be seen projecting nearly at right angles to the galactic plane in this star count plot. (From Majewski et al. 2003 ApJ) 8: The nucleated dwarf elliptical FCC 303 in the Fornax Cluster, at ground-based resolution. (UKST) Interestingly, the supposed galactic globular cluster M54 (discovered in 1770!) turns out to be associated with the Sagittarius dwarf and it has been suggested that it may be its nucleus. Another stream, but with little evidence for any surviving core, has recently been discovered and named the Canis Major dwarf. Returning to the detection of dwarf galaxies as such, improved photographic technology in the 1980s made it possible to detect very low luminosity galaxies at greater distances, for example in the Virgo and Fornax Clusters around 16–20 Mpc away. Studies of Virgo by Allan Sandage, Bruno Binggeli and Gustav Tammann, and of Fornax by Sandage and Harry Ferguson, revealed many low surface brightness objects looking just like Local Group dwarf ellipticals (though some contain central nuclei), dwarf irregulars and even dwarf spheroidals, the numbers implying a quite steeply rising LF. However, at the really low luminosity end we are relying on statistics (more objects per unit area in the cluster direction than away from the cluster) and on circumstantial evidence (whether they look like previously known dwarfs) rather than any direct, individual identification as a cluster dwarf. The same is true, perhaps even to a greater extent, with the more modern CCDbased studies of both these nearby clusters and more distant ones, since it becomes increasingly difficult to distinguish a nearby very faint dwarf from very distant normal luminosity galaxies that merely look faint (e.g. Driver et al. 1999, Trentham and Hodgkin 2002). Even if we can identify the usual types of dwarf, there is also the possibilty of low luminosity galaxies that do not look like those found in the Local Group. A way around both of these problems is to obtain individual distances to candidate dwarfs in the direction of a cluster. This is most easily achieved by measuring redshifts. A problem with this is clearly the potentially large number of galaxies that must be checked. However, technology has again come to our aid in the last 6.8 decade with the development of multi-object spectroscopy. With the “2 degree Field” (2dF) spectrograph on the Anglo-Australian Telescope, for instance, we can now obtain spectra for 400 objects simultaneously. This has enabled the present generation of huge galaxy redshift surveys, such as 2dFGRS with 220 000 redshifts (Colless et al. 2001), or the SDSS with plans for one million redshifts (York et al. 2000). However, taking redshifts for all the galaxies we see down to some magnitude limit solves only half the problem – that is, we can tell which of the candidate faint galaxies really are in the cluster not the background. But at the distance of Virgo and Fornax, the nearest clusters, 200 pc subtends only 2″. Given the blurring effect of the atmosphere, (“seeing”) a small dwarf at these distances will be virtually unresolved and will certainly appear pretty much like any other image 2″ in radius, regardless of any true differences in structure. Any even smaller objects will not only be indistinguishable from background galaxies, but also will look like unresolved stellar images in ordinary groundbased imaging. They will, therefore, not be included in galaxy redshift surveys at all. The only way out of this impasse is the extreme one of taking spectra for all the objects in the direction of the cluster, regardless of whether they look like galaxies or not. This has a very large overhead since at the magnitudes generally accessible to the large surveys (say down to mB ~ 20), stars outnumber galaxies by a sizeable factor. Nevertheless, again taking advantage of multi-object spectroscopy it is possible to undertake an “all-object” survey of a cluster area. The Fornax Cluster Spectroscopic Survey (Phillipps 1997, Drinkwater et al. 2000a) set out to do just this. It covers some 9 square degrees of sky which contains about 10 000 objects between mB = 16.5 and mB = 20. The large majority are stars or background galaxies, with a selection of cluster galaxies thrown in. Given the magnitude limits and the distance to Fornax, the latter are all dwarf galaxies. In fact, we would expect many more dwarf galaxies down to our magnitude limit than appear in the 2dF sample, but many of the candidates are of too low a surface brightness for a spectrum to be measurable. However, the exciting discovery came at the other extreme. Six of the objects classified as “stars” in the input catalogues (created by scanning UKST photographic plates with the APM machine in Cambridge) turned out to have redshifts that placed them clearly at the distance of the cluster. Despite luminosities of several million L (–13.5 < MB < –11), these had to be dwarf cluster members with sizes no more than 100 pc or so (Drinkwater et al. 2000b, Phillipps et al. 2001). Threshing, shredding and harassment In fact, Hubble Space Telescope imaging showed them to be even smaller, with half light radii around 20 pc, almost – but, crucially, not quite – as small as globular clusters (which have re ≈ 5 pc). In addition, higher resolution spectroscopy from the ESO Very Large Telescope and from the Keck Telescope indicated velocity dispersions around 25 km s–1, also intermediate between the values for known dwarf galaxies and globular clusters. This was clearly a previously untenanted area of parameter space, making these a whole new species of small stellar system, which we christened ultra-compact dwarfs (UCDs; Phillipps et al. 2001, Drinkwater et al. 2003). Their origin may be debated, of course. They could be merely the extreme, most massive end of the distribution of globular clusters, but the brighter UCDs are 10 times more luminous than the brightest globular clusters seen around our galaxy. They also seem to have somewhat larger mass-to-light ratios. They could be a totally new type of dwarf galaxy formed early in the development of structure in the universe along with the other dwarf types. Or they could be a new variety descended from a different galaxy type, perhaps via some of the destructive mechanisms we discussed above for December 2004 Vol 45 Galactic surveys 9: The Fornax Cluster showing the positions of the ultra-compact dwarfs (UCDs) discovered during our Fornax Cluster Spectroscopic Survey. High-resolution HST images of five of the UCDs are shown, along with an image of the nucleus of FCC 303 (c.f. figure 8). The UCDs are comparable in size to this nucleus and about 1000 times smaller than NGC 1365, also a member of the Fornax Cluster, seen in figure 1. (Image by M Hilker and A Karlick [Fornax Cluster Spectroscopic Survey team]; original images from the Curtis Schmidt and HST) M32 and the Sagittarius dwarf spheroidal. One of these goes by the name of “threshing” (there are also “shredding” and “harassment” among others) and invokes the tidal stripping of the outer stars from a former nucleated dwarf elliptical (dE,N) galaxy as it passes through the central regions of the cluster, past the first ranked (most massive) central cluster member (NGC 1399 in the case of Fornax). This may leave only the nucleus itself orbiting the centre of the cluster. Support for this sort of mechanism has come from the more recent detection (Jones et al. 2004) of very similar UCDs in the middle of the Virgo Cluster, in the region around M87, but not in the outskirts of clusters. If UCDs are indeed such remnants then we might expect their distribution of masses or luminosities to follow that of the nuclei of dE,Ns. This appears to peak at luminosities much lower than those of the original UCDs (around MB = –9), so a deeper search could be expected to reveal many more UCDs. Another search in Fornax, again using 2dF but targeting stellar-looking objects a magnitude fainter than before, did turn up a population of fainter cluster members (Drinkwater et al. 2004), but there were even more of them than expected: 46, in fact. On further consideration, though, it is clear that we are now in the magnitude range where we will also pick up the bright globular clusters around the central cluster galaxy NGC 1399 (which was already known to have a large population of globulars). Thus telling apart large globulars from small UCDs becomes problematic, if indeed they are December 2004 Vol 45 two independent types of object at all. (Coming the other way, there have been suggestions [e.g. Meylan et al. 2001] that the galaxy’s largest “globular cluster”, ω Cen, may really be the remnant of a former galaxy, too.) The distribution of the spectroscopically confirmed faint UCD candidates does, in fact, suggest two populations of objects as some are closely clustered around NGC 1399 itself (as are its globulars, of course), while the others appear to be spread throughout the central regions of the cluster, like the brighter UCDs. If at least some of the new objects are faint UCDs then, judging by the previous HST imaging, we might expect them to be the physically smallest galaxies yet detected. Clearly our view of the contents of the universe has changed dramatically since Shapley’s “two misty patches” came on the scene. It is now evident that low luminosity/low mass galaxies in fact outnumber their more spectacular giant cousins. However, the factor by which they do so – often called the dwarf-togiant ratio – remains to be settled. Not only is there a large population of diffuse, hard to see, low surface brightness dwarfs out there, but now we have to contend with compact, high surface brightness dwarfs masquerading as stars, as well. Regardless of the fine detail, the existence – and large numbers – of the varied types of dwarf galaxy are already providing us with vital clues and constraints on both the original formation mechanisms for galaxies and the dynamical, evolutionary processes that take place during their lifetimes. The humble dwarf is no longer to be ignored! ● 10: An illustration of a computer simulation of the destruction (“threshing”) of a nucleated dwarf (such as that in the upper inset) to produce an ultracompact dwarf (as in the lower inset). The trail of tidally stripped debris is superimposed on an image of the Fornax Cluster. (Created by U Queensland Communications for the Fornax Cluster Spectroscopic Survey team. Simulation by K Becker) Steve Phillipps is a reader in astrophysics at the University of Bristol. Acknowledgments. The author would like to thank his colleagues on the Fornax Cluster Spectroscopic Survey and especially those involved in the UCD work, Michael Drinkwater, Bryn Jones, Michael Gregg, Kenji Bekki, Warrick Couch, Katya Evstigneeva, Harry Ferguson, Michael Hilker, Russell Jurek, Arna Karick, Quentin Parker, Rodney Smith and Terry Bridges. References Abell G 1962 in Problems in Extragalactic Research (McMillan, NY). Cannon R D et al. 1977 MNRAS 180 81. Colless M et al. 2001 MNRAS 328 1039. Drinkwater M J et al. 2000a A&A 355 915. Drinkwater M J et al. 2000b PASA 17 227. Drinkwater M J et al. 2003 Nature 423 519. Drinkwater M J et al. 2004 PASA in press. Driver S P et al. 1998 MNRAS 301 369. Ferguson H and Sandage A 1988 AJ 96 1520. Harrington R G and Wilson A G 1950 PASP 62 118. Hubble E P 1936 The Realm of the Nebulae (Yale University Press, New Haven). 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