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Galaxies


Contents

Types of Galaxies
Active Galaxies
Seyfert Galaxies
Radio Galaxies
Quasars
Extremely Red Objects (ERO)
Black Holes
Formation and Evolution of Galaxy
Theory of Spiral Arm Formation
The Milky Way
Black Hole at the Milky Way Center
Dark Matter in the Milky Way
Footnotes
References
Index

Types of Galaxies1

Composition

Galaxies are systems of stars, gas and dust (see for example the Sombrero galaxy in Figure 05-01a). They exist in a wide variety of shapes and sizes. The simplest classification scheme, which was devised by Edwin Hubble, recognizes 4 basic types - elliptical, spiral, barred spiral, and irregular and arranges them in a sequence called the "tuning fork" diagram.

Elliptical galaxies are denotes by the letter E followed by the number from 0 to 7 to indicate the degree of flattening of the observed elliptical shape. An E0 galaxy appears spherical, where as an E7 galaxy is markedly flattened. The viewing angle adds some complications into this kind of classification, an elongated ellipsoid would appear spherical if seen "end-on".

Figure 05-01a Composition
[view large image]

Small ellipticals are "dwarf" systems denoted by "dE". The giant ellipticals are designated as "cD". This class of galaxies usually does not contain much interstellar matter.

galaxy types

Spiral galaxies, denote by S, have a central nucleus surrounded by a flattened disc with the stars, gas, and dust organized into a pattern of spiral arms. They are categorized according to the size of the nuclear bulge, the tightness of the spiral pattern, and the degree of "patchiness" in their arms. S0 is the transitional type called lenticular galaxy. An "Sa" galaxy has a large central nucleus and tightly wound, relatively smooth, arms; an "Sb" galaxy has a somewhat smaller nucleus and less tight arms that often contain conspicuous HII regions and clusters of hot young stars; and an "Sc" galaxy has a relatively small nucleus and loosely wound "knotty" arms dominated by numerous HII regions and youthful clumps of stars. In barred spirals, denoted by "SB", the arms emerge from the ends of what looks like a rigid bar of luminous matter that straddles the nucleus.

Irregular galaxies, which have no obvious nucleus or ordered structure, are denoted by "Irr" and are broadly subdivided into "Irr I" and "Irr II". Irr I galaxies display evidence of recent or ongoing star formation (e.g., OB associations (young stars) and HII regions (luminous nebulas)); Irr II galaxies have a disturbed appearance, and their shapes seem to have been distorted by violent internal activity or by collisions or close encounters with other galaxies.

Figure 05-01b Samples of Galaxy Types [view large image]

The classification for the spirals is further subdivided into five luminosity classes: from I (most luminous) to V (least luminous). Figure 05-01b shows some real

galaxy types images for the different types of galaxies; while Figure 05-01c is a schematic diagram showing the side view of the elliptical galaxies and top view of the spiral galaxies. It is believed that a galaxy's type is determined by the amount of angular momentum it contains and the rate at which star formation has proceeded. Elliptical galaxies, and the spheroidal Population II halos of spirals, show little net systematic rotation. Their individual member stars and globular clusters move around their centers in random directions.

Figure 05-01c Types of Galaxies [view large image]

galaxy merger Where the overall angular momentum was small, and star formation proceeded rapidly (thereby mopping up most of the gas early on in the evolutionary process), the end result would be an elliptical dominated by older stars and containing little, if any, gas. Where the angular momentum was greater, the result would be a more flattened system. Where star formation proceeded relatively slowly, the gaseous component would settle into a flattened disclike distribution. The first generation of stars would form within the spheroidal system and the later generations within the flattened disc as observed in the spiral and lenticular galaxies. Dwarf galaxies are much smaller than ordinary galaxies. Because of their size, they have relatively low gravity and matter can escape from them more easily. This property, combined with the fact that dwarf galaxies are the most common type of galaxy in the universe, makes them very important in understanding how the universe was seeded with various elements billions of years ago, when galaxies were forming. Recently in 2005, it is suggested that merger of gas clouds may also played a role in creating different galaxy type. Where a large galaxy was formed by the merger of many small gas clouds, it prevented the formation of disk structure and developed to a large elliptical galaxy (see Figure 05-01d).

Figure 05-01d Development Pathways [view large image]

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Active Galaxies2

The types of galaxies in Figure 05-01b and c seems to be a good classification scheme for the nearby galaxies. However, there are other kinds of galaxies, which do not fit into such category. They seem to represent the galaxies in another phase of evolution. These special objects include Seyfert galaxies, radio galaxies, extremely red objects (ERO), and quasars in a rough order of ascending redshift (distance). Thanks to systematic surveys, the latest (2007) catalogs contain more than 13,000 quasars - a number that could eventually reach 100,000.

Black Hole in Galaxy By 2007, it is recognized that most galaxies other than dwarfs have central black holes. The idea is that black hole "seeds" either attracted matter into forming galaxies or formed within young galaxies in the early universe. This action produced quasars and explains why most quasars are extremely distant. As the black hole acquired more and more matter from galaxies' centers, the fuel became exhausted, so they slowly quieted down. Most galaxies in the recent universe have slumbering giants in their centers. They can be re-activated when interact with other galaxies, starbursts, or gas clouds falling into the central region. This scenario explains active galaxy nucleus (AGN) in the nearby universe. Study of such galaxies reveals that the more massive a galaxy's central bulge, the more massive its black hole. Figure 05-01e shows two deep field galaxies in both optical and infrared. The black holes are displayed prominently in the infrared images.

Figure 05-01e Black Hole in Galaxy [view large image]

X-ray AGN An international team of astronomers using NASA's Swift satellite and the Japanese/United States Suzaku X-ray observatory has discovered a new class of active galactic nuclei (AGN) in 2007. These objects are so heavily shrouded in gas and dust that virtually no light gets out. Only the high-energy X-rays can punch through such thick layer. These objects comprise about 20 percent of point sources in the X-ray background, a glow of X-ray radiation that pervades our Universe. It implies that there must be a large number of yet unrecognized obscured AGNs in the local universe. By missing this new class, previous AGN surveys were heavily biased, and thus gave an incomplete picture of how supermassive black holes and their host galaxies have evolved over cosmic history. Figure 05-01f is an artist's illustration of the X-ray AGN.

Figure 05-01f X-ray AGN [view large image]

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Seyfert Galaxies

A Seyfert is a spiral or barred-spiral galaxy with a bright compact nucleus. In short exposure images, the outer parts of the galaxy are not seen and the nucleus appears almost star-like, so that, in this respect, a Seyert nucleus resembles a quasar. Although not usually strong radio emitters, Seyfert nuclei radiate strongly over a wide range of wavelength producing strong gamma-ray emission up to 1 million ev. Its intensity peaks at an emission line near 450 nm They are less luminous than quasars,
Seyfert galaxy Face-on Seyfert galaxy Edge-on but are brighter than most normal spirals (about 100 times more luminous than the Milky Way). Across the spectrum, the tremendous brightness of Seyferts can change over periods of just days to months and Seyfert galaxies like NGC 7742 in Figure 05-02a are suspected of harboring massive black holes at their cores. Figure 05-02b shows the edge-on view of another Seyfert galaxy M106, which conveys an impression that matters

Figure 05-02a Seyfert Galaxy Face-on [view large image]

Figure 05-02b Seyfert Galaxy Edge-on [view large image]

are falling into a hole.


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Radio Galaxies

Radio Emission Radio galaxies are so named because they are powerful sources of radio emission that radiate much more strongly at radio wavelengths than do conventional galaxies as shown in the upper diagram of Figure 05-03. Whereas normal galaxies emit blackbody radiation, the radio emission is generated by a mechanism called synchrotron radiation. Cygnus A was the first radio galaxy identified in 1951. It is shown in the lower diagram of Figure 05-03. In a typical radio galaxy, most of the emission comes from two huge lobes located far beyond and on either side of the visible galaxy. The radio-emitting lobes are believed to be clouds of energetic charged particles that have been expelled from the nucleus of the central galaxy, the jets are streams of additional energetic particles, which have been accelerated in the nucleus and are surging outward toward the lobes, producing "hot spots" (represented by red colour) where they plow into the leading edges of the
Radio Emission lobes. This material typically spans a region of space five to ten times larger than the visible galaxy, and sometimes far larger than that. The overall luminosities can be up to several thousand times that of the Milky Way. Strong radio emissions are usually associated with elliptical galaxies - such as M87 (Virgo A) - or disturbed galaxies such as Centaurus A3. This kind of objects is sometimes referred to as AGN for Active Galaxy Nucleus. By superimposing the radio images taken by the Very Long Baseline Array (VLBA) to the gamma-ray sky map produced by the

Figure 05-03 Radio Galaxy

Large Area Telescope (LAT), astronomers are able to confirm that the gamma-ray emission from the core of AGN is associated with the radio jet.

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Extremely Red Objects (ERO)

The Hercules Deep Field provides a detailed view of hundreds of distant galaxies. One particular object called Extremely Red Object (ERO) is marked with the yellow box as shown in Figure 05-04a. This type of galaxies is generally faint in the visible light, but can be very bright in the infrared. The six images below show how different the same object can appear from visible blue light (left-most image), to well into the infrared (far-right). This object appears to have achieved its extreme red color because the bulk of its star formation has been reddened with a thick layer of dust. This galaxy is believed to lie about 9 billion
ERO Infrared Galaxies light years away, at a time when the universe was only a third of its present age. It is estimated that this galaxy has around 100 billion stars and may in fact be a very distant mirror -- an analog of our own Milky Way Galaxy in its formative years. Combining data over a period of 3 years obtained at UKIRT, astronomers in 2008 have produced an image containing over 100,000 galaxies (Figure 05-04b). Many of the faint red objects in the background (against a relatively

Figure 05-04a ERO
[view large image]

Figure 05-04b Infrared Galaxies [view large image]

nearby spiral galaxy) are massive galaxies at distances of over 10 billion light-years.

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Quasars

Quasar During the early 1960s, some radio sources were shown to coincide in position with objects that looked like stars. These became known as quasars (quasi-stellar radio source). It was later discovered that only about one in ten of these objects is a strong radio emitter, the radio-quiet type is named quasi-stellar object (QSO). The term quasar is still widely used to describe both kinds of objects. Figure 05-05a shows the quasar 3C273 (3C denotes the third Cambridge Catalogue of radio sources) discovered in 1962. The radio, optical, and X-ray images are displayed in the top from left to right. The lower picture is a drawing of a quasar. These objects have high redshift, some of which translate into distance well in excess of 10 billion light-years. In order to appear as bright as they do, quasars must be extremely luminous at more than ten thousands times the luminosity of the normal galaxies. Quasars radiate strongly over a wide range of wavelenghts, and although emission lines are present in

Figure 05-05a Quasar 3C273
[view large image]

their spectra, the overall spectrum is consistent with synchrotron emission. Their powerful energy sources are compact and variable, with some quasars varying

Blazar substantially in brightness over periods as short as a few days. Some has a jet (e.g, 3C273), or pair of jets emerging from their centers similar to the radio galaxies. There are many more high redshift quasars than low redshift ones. No known quasar has a redshift less than 0.06, and quasar numbers seem to be highest at redshifts of around 2-3. It follows that quasar activity must have been more prevalent among galaxies billions of years ago, when the universe was younger than it is now.

There is a class of objects called BL Lacertae objects or blazars (Figure 05-05b). They are star-like radio sources, similar in appearance to quasars, but with no obvious emission lines in their featureless spectra. They may be quasars seen almost end-on with the jet pointing to the line of sight. Astronomers divide blazars roughly into two groups: lower-energy, relatively nearby BL Lacertae objects and higher-energy, distant soruces. More than 1000 blazars have been catgaloged.

Figure 05-05b Blazar [view large image]

It is possible that redshift of the blazars may be masked by the approaching jet, which shifts the light to shorter wavelength.

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Black Holes4

Black Hole Worm Hole The concept of black hole has its origin in a solution of Einstein's General Relativity for a spherical object with mass M and radius R. If the mass collapses to a radius less than R = 2GM/c2, where G is the gravitational constant and c is the speed of light, then nothing (including light) can escape from inside this radius. It is called the event horizon or the Schwarzschild radius (named after the astrophysicist who solved the equation). Figure 05-06a shows a schematic diagram of the Schwarzschild geometry.

Figure 05-06a Black Hole
[view large image]

Figure 05-06b Worm Hole [view large image]

It is known as the embedding diagram. The two dimensional circles are slices of three dimensional spheres (of the same radius) - the hyperspace. The verticle axis denotes the "stretch" of space in the radial direction. The slope of the curve can be considered as representing the curvature of the space. It is flat (or zero) at the outer edge and becomes infinity at the Schwarzschild radius. This pictorial representation is very similar to a rubber sheet stretched by a rock. The shape of the region inside the horizon is somewhat arbitrary. It is only known that everything plunges inevitably to the central singularity once passing over the horizon. In a more realistic drawing the event horizon would be placed far below the diagram at infinity. The complete Schwarzschild geometry consists of a black hole, a white hole, and two singularities connected at their horizons by a worm hole as shown in Figure 05-06b. A white hole is a black hole running backwards in time. Just as black holes swallow things irretrievably, so do white holes spit them out. White holes cannot exist, since they violate the second law of thermodynamics by allowing some time reversal events such as reassembling a broken glass back to its original whole. The white hole geometry outside the horizon represents another Universe. The worm hole joining the two separate singularities is known as the Einstein-Rosen bridge, but even if it can somehow be generated, it would be unstable and pinch off immediately. Therefore, only the black hole geometry is applicable to the physical world.

Black Hole It is believed that every quasar, active galactic nucleus, and even normal galactic nucleus contains a black hole with a mass of between ten million to several billion solar masses at its core. The difference in appearance is related to the intensity of the activity. Since galaxies rotate, matter falling toward the central black hole will form a rapidly spinning disk of gas - an accretion disk - rather than falling directly into the hole. Kinetic energy released by in-falling matter, and frictional effects within the accretion disk, raise the temperature of the nner parts of the disk to enormous values and provide plenty of energy to power AGN's on all scales from Seyferts to quasars. By a process that is still not fully understood but seems to be related to rotating black hole, the central engine accelerates streams of charged particles to very high speeds. The inner rim of the accretion disk, together with surrounding gas and magnetic fields, forms a nozzle that confines the outward flow of energetic particles into narrow streams that shoot out perpendicularly to the plane of the disk. Figure 05-07a shows a model of the black hole.

Figure 05-07a AGN Model [view large image]

Figure 05-07b is a HST (Hubble Space Telescope) image of NGC4261, which is a radio galaxy. The image strongly suggests that it is a black hole fitting the description of the theoretical model. Infrared observation of NGC1068 in 2004 was able to resolve the inner region down to a few parsec. Figure 05-07c penetrates the dusty central region and shows the structures on arcsec scales. The picture on the right is a model for the nucleus of NGC1068. It contains a central hot component (dust temperature > 800K, yellow) marginally resolved along the source axis. Its finite width and the dashed circle indicate the currently undetermined extent. The much larger warm component (T=320K, red) is well resolved. The arrows indicate the
Black Hole NGC4261 Black Hole NGC1068 projected orientation of the two interferometer baselines and the angular resolution L/2B, where L is the wavelength and B is the projected baseline. The image shows that the active galactic nuclei are arranged like a thick doughnut. This model requires a continuous injection of kinetic energy to maintain such cloud system. The mechanism is currently unknown; thus a better understanding of the physics of these spectacular objects is needed.

Figure 05-07b NGC4261
[view large image]

Figure 05-07c NGC1068
[view large image]

The quasar 3C273 is a 2-billion-solar-mass black hole encircled by a doughnut of gas (accretion disk) and with two gigantic jets shooting out along the spinning axis. The Schwrzschild radius for this object is about 6x109 km. Such supermassive black hole can be created while matter is still at quite low density (~ 10-3 gm/cm3). Since the tidal force at the event horizon of a black hole is inversely proportional to the square of its mass, its effect on a space visitor would be un-noticeable, although he would soon be in dire trouble as he plunges irrevocably toward the central singularity. However for a stationary observer, it takes an infinitely long time for the asronaut to approach the event horizon (due to gravitational time dilation) and the view of the asronaut would gradually disappear (due to gravitational red shift of light). The effect on the astronaut visiting a stellar black hole (mini-quasar) would be more violent due to the drastic increase of the tidal force.
Black Hole 2 In a November, 2004 announcement by NASA, a black hole catalogued as SDSSp J1306 appears to be about one billion times as massive as the sun. It is 12.7 billion light-years away. A similarly massive and distant black hole was studied in the same year with the European Space Agency's XMM-Newton X-ray satellite. The object, SDSSp J1030, is 12.8 billion light-years away. These two results seem to indicate that the way supermassive black holes produce X-rays has remained essentially the same from a very early date in the universe. How such massive and energetic structures formed so quickly (only after one billion years of the big bang) remains a major puzzle for scientists. Mergers of smaller galaxies and their black holes may have played a role. Researchers suspect that black hole formation and galaxy development go largely hand-in-hand, but they cannot say which comes first. Figure 05-07d is an artist's conception of a supermassive black hole with matter swirling into it.

Figure 05-07d Supermassive Black Hole [view large image]

In 2009, radio observations of 4 early galaxies (1 to 2 billion years after the Big Bang) including J1148+5251 shows that the mass ratio of central bulge to black hole is about 10 times smaller than the more recent data indicating the black hole probably came first.

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Formation and Evolution of Galaxy5,6

Galaxy Formation Protogalaxies The most accepted view on the formation and evolution of large scale structure is that it was formed as a consequence of the growth of primordial fluctuations by gravitational instability. Galaxies can form in a "bottom up" process in which smaller units merge and form larger units. It is referred to as the "Inside-out Theory" or "Merger" in the upper half of Figure 05-08a. In the present epoch, large concentrations of galaxies (clusters of galaxies) are still in the process of assembling.

Figure 05-08a Initial Formation [view large image]

Figure 05-08b Proto-
galaxies [large image]

The opposing view is the "top down" process in which large clump breaks up into smaller units. It is referred to as the

"Outside-in Theory" in the lower half of Figure 05-08a. The figure also shows the kind of objects the NGST (Next Generation Space Telescope) will detect according to the two opposing theories. The "bottom up" theory have been given a boost in 2008 by the first ever detection of the infant protogalaxies (artist's view in Figure 05-08b) with an unprecedented 92-hour session on the European Southern Observatory's Very Large Telescope. These protogalaxies were irregularly shaped and with low star-formtion rates, but the stars that did form were massive and consequently exploded as supernovae. The image shows a group of protogalaxies in the process of merging.
Density Fluctuation The difference between the "bottom up" (inside-out) and "top down" (outside-in) point of view is related to whether the universe is composed with cold dark matter (CDM, slow moving) or hot dark matter (HDM, fast moving). In the former scenario there is fluctuation in the power spectrum over a wide range of physical scales as shown in Figure 05-08c. It increases with smaller scales, therefore structure formed first with small objects, which then merge to form ever larger structures. This is called ``bottom up'' structure formation. The observations strongly favour this scenario over its competitor: ``top down'' structure formation. The proto-typical ``top down'' scenario is structure formation in a universe dominated by hot dark matter. Hot dark matter cannot support fluctuations on small length scales - they are washed out with the rapid

Figure 05-08c Power Spectrum for Density Fluctuation

motion of the particles. Thus only large scale fluctuations survive to the present epoch. Structure forms first large scale objects which fragment into smaller objects.

The early universe was a barren wasteland of hydrogen, helium, and a touch of lithium, containing none of the elements necessary for life as we know it. From those primordial gases were born giant stars a few hundred times as massive as the Sun, burning their fuel at such a prodigious rate that they lived for only about 3 million years before exploding. Those explosions spewed elements like carbon, oxygen and iron into the void at tremendous speeds. By the remarkably young age
Protogalaxy Evolution of 275 million years, the universe was substantially seeded with metals thrown off by exploding stars. That seeding process was aided by the structure of the infant universe, where small protogalaxies less than one-millionth the mass of the Milky Way clustered together into vast filamentary structures. Giant stars form at the intersections of these great filaments of primordial hydrogen, forming the nuclei of the first galaxies - the protogalaxies (Figure 05-08d). The small sizes and distances between those protogalaxies allowed an individual supernova to rapidly seed a significant volume of star forming space. New simulations show that the first, "greatest generation" of stars spread incredible amounts of such heavy elements like carbon, oxygen and iron across thousands of light-years of space, thereby seeding the cosmos with the stuff of life.

Figure 05-08d Protogalaxy Evolution
[view large image]

Merger Simulation After the initial phase of galaxy formation, there was an era of cosmic fireworks: galaxies collided and merged (see Figure 05-08e), powerful black holes in quasars sucked in huge whirlpools of gas, and stars were born in unrivaled profusion. The activity of star formation peaked about four to six billion years. Since then galactic mergers became much less common, the gargantuan black holes were replaced by numerous moderate ones, star formation continued but mostly in the low mass variety. In other words, the contents of the universe have transited from a small number of bright

Figure 05-08e Simulation of Galactic Merger [view large image]

objects to a large number of dimmer ones. Computer simulations suggest that such shift may be a direct consequence of cosmic expansion.

As the universe expands, galaxies become more separated and merger become rarer. Furthermore, as the gas surrounding galaxies grows hotter and more diffuse, it does not gravitationally collapse as readily into the galaxy's potential well. A few billion years from now, the smaller galaxies that are active today will have consumed much of their fuel, and the total cosmic output of radiation will decline drametically. As the cosmic expansion continues, the dwarf galaxies - which hold only a
Galaxy Evolution Simulation few million stars each but are the most numerous type of galaxy in the universe - will become the primary hot spots of star formation. Inevitably, though, the universe will darken, and its only contents will be the fossils of galaxies from its past. Figure 05-08f shows the evolution subsequent to the initial phase. Figure 05-08g shows another evolutuon simulation with cold dark matter.

Figure 05-08f Evolution History [view large image]

Figure 05-08g Evolution Simulation [view large image]

It seems that galaxy formation is a very complicated process involving star-forming history, merger history, mass, size, angular momentum, and external environment. But research in 2008 indicates that the mass is the only dominant factor in determining the properties of individual galaxies. A sample of roughly 200 galaxies has been selected from a large, blind sky survey for neutral hydrogen (HI) emission using the hydrogen spectral line at a wavelength of 21 cm. For each galaxy in the catalogue, they measured a number of quantities: 1. the total hydrogen mass; 2. the width of the hydrogen spectral line; 3. the redshift; 4. the inclination with respect to the line of sight; 5. two radii, containing 50% and 90% of the light, respectively; and 6. the optical luminosity in four different colour bands. It is found that the six independent components that they use to describe the galaxies in their sample are all correlated with each other and with a single principal component — the galaxy's mass.
Mass Range of Galaxies This finding is consistent with the progression of mass among the types of galaxy as shown in Figure 05-08h, where the dwarf galaxies are in the lowest mass range of 107 - 108 Msun, the mass of irregular galaxies is in between 108 - 1010 Msun, the range for spiral galaxies is

Figure 05-08h Mass Range of Galaxies [view large image]

1010 - 1012 Msun, while the giant elliptical galaxies is in the range 1012 - 1013 Msun. The mass ranges form a continuous sequence without overlapping. Thus, if the mass of the
galaxy is known, the type would follow according to Figure 05-08h. It is not that straight forward conversely, for if we know the type of the galaxy there is a range of mass within that type.

A single observation in 2009 discovered that elliptical galaxies seem to expand in size from epoch as early as 3 billion years after the Big Bang to present day. However, the mass of such elliptical galaxies remains constant in contradiction to the scaling relationship between mass and effective radius re for nearby galaxies (Figure 05-08i). The picture on the left of the Figure
Elliptical Galaxy shows very compact galaxies evolved to bigger, more diffuse objects and became more abundant. Diagram on the right depicts the scaling relationship for nearby galaxies (the black dots) and the high redshift galaxy 1255-0 (at z = 2.186 in red symbol, dynamical mass refers to mass obtained from velocity dispersion of the stars). Current theory predicts that galaxies evolve according to the scaling law perhaps by merger (the blue arrow). The new observation implies another path as shown by the red arrow.

Figure 05-08i Evolution of Elliptical Galaxy

Further research is required to confirm the atypical observation. It remains to be seen whether we need conventional or novel explanations for the evolution of elliptical galaxies.



Table 05-01 summarizes the evolutionary sequence. The time epoch t is computed from the relation with the red shift z:
t = 13.7x109/(1+z)3/2 years, which is derived from the standard cosmology model in flat space.

Epoch (109 years) Red- shift Astronomical Objects Activities
~ 0.38
x 10-3
~ 1090 Cosmic Microwave Background Radiation Transparent to light.
< 0.38
x 10-3
> 1090 None. Dark age.
< 0.1 > 25 First stars, supernovea. Formation of black holes, production of heavy elements.
< 0.5 > 8.0 Protogalaxies. Protogalaxies drew in matter.
< 1.0 > 4.70 Baby galaxies. Galaxies took shape.
< 3.0 > 1.75 Quasar, supermassive black holes. Galaxies collided and merged, bursts of star formation.
< 6.0 > 0.73 ERO (extremely luminous galaxies). Rate of star formation peaked at ~ 5 x 109 year.
< 13.7 > 0 AGN; elliptical, spiral, & irregular galaxies. Small # of bright objects replaced by large # of dimmer ones.
>>13.7 Dwarf galaxies... ... galaxies will disappear with the evaporation of matter.

Table 05-01 Evolution of Galaxies