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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 |
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. |
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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 |
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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] |
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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] |
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, quasars and extremely red objects (ERO) 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.
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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 galactic 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] |
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Figure 05-01f presents a unified view of the AGN. The basic ingredient consists of a central black hole surrounded by a dusty disk. The kind sporting a jet or two usually associates with strong radio emission; it includes quasar, and radio galaxy. While QSO and Seyfert galaxy belong to the radio quiet kind. Energy consumed by the jet and various forms of radiations is extracted from the in-falling gas cloud and the dusty torus - ultimately it is converted from the gravitational potential and angular momentum. The same kind of object presents a different aspect depending on the viewing angle of the observer. Figure 05-01g is an updated version of the AGN. It adds an accretion disk in between |
Figure 05-01f An Unified View of AGN |
Figure 05-01g Another Unified View of AGN |
the dust torus and the black hole and classifies the Seyfert galaxies into two types (see Figure 05-01g). While the EROs (Extremely Red Objects) are these kinds of objects further away in the early universe. |
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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 05-01i is an artist's illustration of the X-ray AGN. |
Figure 05-01i X-ray AGN [view large image] |
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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 05-02a shows a schematic diagram of the Schwarzschild geometry. |
Figure 05-02a Black Hole |
Figure 05-02b Worm Hole [view large image] |
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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 05-02c shows a model of the black hole. |
Figure 05-02c AGN Model [view large image] |
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Magnetohydrodynamics is the branch of physics dealing with the behavior of the combined system of magnet field and ionized gas at low density. A popular theoretical scenario applies such formulation to explain the relativistic jet(s) powered by the black hole. The study found that magnetic field lines are twisted into a helix (as shown in Figure 05-02d) by the differential rotation of matter in the accretion disk. Such field provide a force to expel the ionized particles in a collimated jet from the inner circumference of the accretion disk. The energy to maintain the process is derived from the braking action on the rotation of the disk. In this way, matter can slow down and eventually flow inward into the black hole. Figure 05-02e illustrates a mechanism to extract the spinning energy from a rotating black hole, wherein the surrounding ionized gas and the magnetic field act together to set up a voltage |
Figure 05-02d Magnetic Field and Jet [view large image] |
Figure 05-02e Rotating BH |
difference between the poles. This is similar to a battery driving electric current around to provide another source of energy for the outflowing jet(s). |
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much larger warm component (T=320K, red) is well resolved. The arrows indicate the 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 05-02f NGC4261 |
Figure 05-02g NGC1068 |
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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 05-02h is an artist's conception of a supermassive black hole with matter swirling into it. |
Figure 05-02h 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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A 2012 update on the supermassive black hole J1148+5251 reveals that while matter swirls inward from the accretion disk toward the black hole, intense radiation creates outflow of gas at the same time. The process is shown schematically in Figure 05-02i. The orange wavy lines represent photons emitted during the accretion process. Most of them escape the galaxy, but some imping on clouds of gas (blue) and the radiation pressure drives the gas out. The stars and dark are too heavy to be affected by the radiation. It is suggested the elliptical galaxies may lost their gas component in this way. The Milky Way has a mild imitation of such process in the form of the 30-kpc arms. |
Figure 05-02i BH Gas Outflow |
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On 28 March 2011, the Swift satellite designed to look for gamma-ray bursts (GRBs) detected a burst with unusually long duration of more than a month. The new source, called Swift J164449.3+573451, is now believed to be generated by the tidal disruption of a star moving too close to a black hole. The left portion in Figure 05-02j shows the level of X-ray flux recoded by various detectors over the past 20 years with observational duration indicated by horizontal bars. The data indicate the gradual buildup of intensity until it suddenly flared up more than 200 times in few hours. The right portion in the same diagram is the follow-up to show the flux variation for the first 7 weeks of the most recent observation. Time interval of the variation (in luminosity) can be used to calculate the size of the source since each part of |
Figure 05-02j Black Hole Cannibalism [view large image] |
the source would have to be in contact with others on such a time scale t to coordinate the variations; thus the size r c t. For the most rapid variability of t 100 s, r 3x1012 cm, which is about 50 time bigger than the Sun and about 1/2 the size of Mercury's orbit. |
rc2/2G
107 Msun, which is in close agreement with the estimate from the relationship between the black hole mass and galactic bulge luminosity. The unusually high luminosity may be related to the onset of relativistic jet pointing to the direction of observation and moving at a velocity of 99.5% of the speed of light.![]() |
In another 2011 report, the jet from M87 has been observed in great detail with the Very Long Baseline Array (VLBA), which has resolution 400 times finer than the HST. Since black hole is not a clean eater, about half of the food (the in falling star) is left behind in the accretion disk close to the black hole. Interaction of the rotating "crumbs" and magnetic field produces the jet. The observation finds a jet of high-energy particles starts as a broad flow at |
Figure 05-02k M87 Jet |
a distance about 14 to 23 times the Schwarzschild radius of the black hole. The jet becomes more cylindrical and faster with distance from the black hole. Figure 05-02k (a) is a schematic diagram showing different sections of the jet that have different particle densities observed at |
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M87 used to hold the title of harbouring the most massive black hole with a mass of 6.3x109 Msun. The record was broken in 2011 with the detection of 2 super massive black holes in NGC 3842 (within the Abell 1367 cluster) and NGC 4889 (within the Coma cluster) both with a mass of about 1010 Msun. These giant galaxies all sit at the bottom of the cluster's gravitational potential well collecting a lot |
Figure 05-02l Black Hole Correlations |
Figure 05-02m Black Hole Formation [view large image] |
of the material falling inward. Estimate of black hole mass depend on either the measurement of stellar (or gas, or maser emission from molecular clouds etc.) velocity |
or V-band galactic bulge luminosity Lv. The data points usually fall on (or near) a straight line of a logarithmic plot (see the formula for the solid black line in Figure 05-02l, b). However, the super massive black holes doesn't seem to follow such relationship (Figure 05-02l, a and b). The deviation is explained by proposing that the super massive black hole was formed by merger of black holes while the lighter variety was grown by accretion of cold gas (Figure 05-02m). BTW, the BCG (in Figure 05-02l) is the abbreviation of Brightest Cluster Galaxies, and MW denotes Milky Way.![]() |
presented astronomers with a problem to explain how could it be created so soon and so big? It is known that the acquisition of material by the black hole is always balanced by ejection of some of the in-falling matter. It has been calculated that a black hole sucking in matter continuously at its maximal rate would double its mass Mbh every 50x106 years, i.e., Mbh=M0x277/5~ 4x104M0, where M0 is the initial mass. This is too slow for a seed |
Figure 05-02n Supermassive Black Hole [view large image] |
black hole of stellar mass to grow into billion-sun in 770x106 years (Figure 05-02o,a). |
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Two different theories has been proposed to resolve the problem. They all try to make the basic component from solar-mass black hole to middleweight one with mass of 105 to 2x106 Msun, i.e., to bump up M0. One theory suggests that black hole at the center of a star cluster could grow quickly enough to middleweight seed hole (Figure 05-02o,b). The other one involves collapse of primordial gas cloud (Figure 05-02o,c). The former scenario predicts more leftover middleweight seed holes to survive into the present age. Since only a few hundred such holes among 2x105 galaxies have been found so far, it seems that the odd is against the bottom-up version at least for now (see also related observation in Baby Galaxy). |
Figure 05-02o Supermassive Black Hole Formation |
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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 05-03a are suspected of harboring massive black holes at their cores. Figure 05-03b shows the edge-on view of another Seyfert galaxy M106, which conveys an impression that matters are falling into a hole. |
Figure 05-03a Seyfert Galaxy Face-on [view large image] |
Figure 05-03b Seyfert Galaxy Edge-on [view large image] |
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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 05-04. 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 05-04. 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 lobes. |
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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 Large Area Telescope (LAT), |
Figure 05-04 Radio Galaxy |
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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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 their spectra, the overall spectrum is consistent with synchrotron |
Figure 05-05a Quasar 3C273 |
emission. Their powerful energy sources are compact and variable, with some quasars |
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varying 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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image containing over 100,000 galaxies (Figure 05-06b). Many of the faint red objects in the background (against a relatively nearby spiral galaxy) are massive galaxies |
Figure 05-06a ERO |
Figure 05-06b Infrared Galaxies [view large image] |
Figure 05-06c Hot DOG |
at distances of over 10 billion light-years. |
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In August 2009 the rejuvenated Hubble Telescope took an infrared deep field image (Figure 05-07a). It shows many small galaxies with redshift of up to 8.5 corresponding to 13.1 billion light years from us or about 600 million years after the Big Bang. Their size and mass are about 1/20 and 1/100 of those of the Milky Way respectively. Although detected in the near infrared region of the spectrum, they are intrinsically blue (before the redshift) - meaning that they may be |
Figure 05-07a Furthest Galaxies [view large image] |
Figure 05-07b Furthest Cluster of Galaxies [view large image] |
deficient in heavier elements, i.e., made with primordial matter, and as a result, quite free of the dust that reddens light through scattering. The discovery of these galaxies so near the |
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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" as shown 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. 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" as shown in the lower half of Figure |
Figure 05-08a BH, Initial Formation [view large image] |
Figure 05-08b BH, Supermassive |
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 |
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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 motion of the particles. Thus only large scale fluctuations survive to the |
Figure 05-08c Power Spectrum for Density Fluctuation |
present epoch. Structure forms first large scale objects which fragment into smaller objects. |
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carbon, oxygen and iron into the void at tremendous speeds. By the remarkably young age 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 |
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Galaxies used to be considered as "island universes" that formed in the distant past and have since evolved in isolation from their surroundings. Such concept was replaced by the hierarchical growth scenario, which enrols galaxy interactions, collisions and mergers to shape the mature galaxies in the current epoch. Lately in the 2010s, observations reveal that the decline in galaxy formation is not matched by the decrease of atomic hydrogen - only half of the latter has been consumed by the galaxies. The latest explanation proposes that the hydrogen fuel is supplied by ionized hydrogen in the intergalactic environment. Such novel idea is supported by the recent (2013) detection of neutral hydrogen in space between the Andromeda and Triangulum galaxies. The detection of 21 cm radio emission from neutral hydrogen is much easier although the neutral variety is only about 1% of the ionized one. The new discovery adds one more element into the process of galaxy assembly. |
Figure 05-08e Galactic Mass Assembly [view large image] |
Figure 05-08e is the numerical simulation of galaxy formation and evolution, in which green denotes higher ionized hydrogen density and black is lower (a-c are zoom in views). |
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After the initial phase of galaxy formation, there was an era of cosmic fireworks: galaxies collided and merged (see Figure 05-08f), 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 transitted from a small number of bright objects to a large number of dimmer ones. Computer simulations |
Figure 05-08f Simulation of Galactic Merger [view large image] |
suggest that such shift may be a direct consequence of cosmic expansion. |
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will decline drametically. As the cosmic expansion continues, the dwarf galaxies - which hold only a 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 05-08g shows the evolution subsequent to the initial phase. Figure 05-08h shows another evolutuon simulation with cold dark matter. |
Figure 05-08g Evolution History [view large image] |
Figure 05-08h Evolution Simulation [view large image] |
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This finding is consistent with the progression of mass among the types of galaxy as shown in Figure 05-08i, 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 05-08i 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 |
m = 0.26 and 
= 0.74.| 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. |
| < 0.05 | > 25 | First stars, supernovea. | Formation of black holes, production of heavy elements. |
| < 0.6 | > 8.0 | Protogalaxies. | Protogalaxies drew in matter. |
| < 1.3 | > 4.70 | Baby galaxies. | Galaxies took shape. |
| < 3.8 | > 1.75 | Quasar, supermassive black holes. | Galaxies collided and merged, bursts of star formation. |
| < 7.2 | > 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. |
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13.0 billion years). |
Figure 05-08k Evolution of Galaxies [view large image] |
The lookback time T (in billions of years) is computed from the red shift z by the formula: T 13.7 x [1 - (1 + z)-3/2]. Figure 05-08l shows an updated cosmic timeline as appears in the September 2012 issue of Astronomy. |
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Figure 05-08l Cosmic Timeline [view large image] |
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These objects emit strong ultraviolet light (from newborn stars and exploding supernovae), have low metal content, and are in the form of amorphous blob. The galaxy's gas contains just 2% of the Sun's abundance of heavy elements, or metals - the most pristine galactic gas seen since the big bang (star-forming regions in the Milky Way contain 100 to 200 more of these elements than the baby galaxy). This kind of astronomical objects is thought to exist more than 10 billion years ago (a few billion years after the Big Bang). Such nearby baby galaxies probably started out as a small gas cloud in a relatively empty region of space. It grew very slowly until, after nearly 13 billion years, it had enough density to form stars. The images on top of Figure 05-09a compares the mature and newborn galaxies in visible and ultraviolet lights. The lower image is the baby galaxy I Zwicky 18, at a distance of only 45 million light years. The galaxy's proximity allowed Hubble's eagle-eyed Advanced Camera for Surveys to resolve |
Figure 05-09a Baby Galaxy |
a few thousand of its estimated 20,000 stars. The stars' colour and brightness suggest that none are more than 500 million years old. More HST observations in 2008 indicate that star formation in I Zwicky 18 began at least one billion - and perhaps up to 10 billion |
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Another baby galaxy in the early universe has been detected in 2005. It is located at a point about 800 million years after the Big Bang. It has a mass eight times that in the Milky Way. The discovery was surprising, since astronomers have long theorized that galaxies form when stars gradually cluster together, with small galaxies preceding bigger galaxies. Now the new evidence suggests that the process of galaxy formation started really very early on. This galaxy, known as HUDF-JD2 was found by researchers using NASA's Hubble and Spitzer space telescopes. It is the smaller red object in Figure 05-09b. Other survey found massive | |
Figure 05-09b HUDF-JD2 |
galaxies originated 700 million years after the Big Bang, whereas the supposedly old dwarf galaxies showed the most recent bouts of star formation just 4 billion years ago. Theoretical consideration also suggests that the proto-galaxies in the early universe may have fizzled out |
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Report from Hubble Ultra Deep Field in 2011 shows the oldest galaxy (to date) 13.2 billion light years from Earth or 480 million after the Big Bang at a redshift of about 8 (Figure 05-09c). In contrast to the 60 or so galaxies detected in a period roughly 650 million years after the Big Bang, this lone object indicates large galaxies rapidly built up from smaller ones in a short span fewer than 200 million years, and the rate of star formation increased tenfold. This discovery raises a puzzle about not enough sources to re-ionize the neutral hydrogen in this epoch. Further observations with Hubble and the JWST will be needed to clear up the discrepancy. |
Figure 05-09c Oldest Galaxy |
An article in Nature Online 13 April 2012 reports that another very old galaxy was found at a red shift of 9.6 - about 490 million years after the Big Bang. Its age is no more than 200 million years and has only 1% the mass of the Milkway. By lucky coincidence, it locates right behind a galactic |
m = 0.26 and 
= 0.74, the age of the universe corresponding to z = 9.6 is about 450 million years, while it is about 600 million years for z = 8. These values are at variance with the ages quoted above. Those numbers are also contradictory with each others.
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universe, i.e., about 2x1054 gm. In the early epoch, this much of the baryonic matter were mostly neutral hydrogen atoms, which can be measured in the absorption spectrum known as "Lyman alpha forest". It seems that around 5 billion years after the Big Bang, the balance in the book keeping of baryonic mass had gone awry with the full-blown formation of galaxies. Auditing of the various kinds of galactic components (such as stars, stellar remnants, neutral gas, ionized gas, |
Figure 05-09d WHIM Detection |
Figure 05-09e WHIM Replenishment |
dust, planets, ...) through measuring the different forms of electromagnetic radiation reveals that the total amounts to only 1/10 of the initial inventory. Where is the rest? |
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In 2013, computer study of dwarf galaxies reveals that cold dark matter such as WIMP would produce a simulation too dense for the real things. Hot dark matter such as neutrinos move too fast to settle down into compact structures like galaxies. Only the warm dark matter such as the sterile neutrinos plus disturbance from supernova explosions would generate galaxies of just the right density (Figure 05-09f). This work seems to be in good agreement with the detection of WHIM as mentioned above. |
Figure 05-09f Warm Dark Matter |
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The formation of the spiral patterns is still a mystery because the simple model of differential rotation (rotational speed varies with distance) would produce tightly wound spirals (within 500 million years) in contrary to observation. A generally accepted mechanism for producing the spiral structure involves wave of excess density (density wave10) that gently travels around the galaxy compressing gas in its wake. This compressed gas triggers star formation and helps to explain why we see the concentration of bright young stars and clusters in the spiral arms. Figure 05-10a is a schematic model illustrating the action of a density wave, which causes stars and interstellar gas and dust to bunch up |
Figure 05-10a Density Wave |
temporarily, with the spiral arm being the result of a temporary compression of material. The mechanism for the generation of density wave is unclear, but it is thought to be similar to the traffic jam on highway (see Figure 05-10a). |
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The original density wave soon ran into the difficulty of energy dissipation by setting up shock waves in the interstellar gas. Complex mechanism was proposed to resolve the problem without much success. This unsatisfying state of affairs changed only in the 1980s and 1990s when gas is included into the simulations. Since gas constitutes only a few percent of the mass of spiral galaxies, it was not taken into account in previous modeling. It turns out that the gas has a disproportionate dynamical role. As soon as gas is included into the simulation, it produces a rich variety of galactic morphologies. The torque exerted by the stellar bar acts as a giant stirrer, continuously driving a spiral structure in the gas. The spiral did not fade away as it had in earlier simulations. It also |
Figure 05-10b Reinvigoration [view large image] |
explains the presence of dust lanes on the leading edge of spiral arms, the high rate of star formation in galactic center, and the refueling of the central black hole. Figure 05-10b shows the cycles of reinvigoration by the accretion of intergalactic gas into the system starting from an initial disk of stars, gas, and dust. |
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of the ellipses. Spiral wave arises when the ellipses move in unison but are not perfectly aligned; each ellipse is slightly skewed compared with its neighbors. The density of stars is highest where the ellipses crowd together as shown in diagram c. Diagram d shows the barred spiral pattern when orbits near the center of the galaxy are aligned but those farther out are skewed. It is thought that the alignment is caused by spontaneous gravitational instability. Because gravity in |
Figure 05-10c Wave Patterns |
Figure 05-10d Wave Anatomy |
galaxies is not a fixed external force but a product of the stars themselves, waves can be self-reinforcing. The process starts when stellar |
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There are about 4x1010 galaxies in the universe. Among this multitude of galaxies, 34% are spirals, 20% are ellipticals, and 54% are irregular. We happen to live in an ordinary spiral galaxy called the Milky Way. On a clear night and with the aid of long exposure time, it appears like a silvery river across the sky as shown in Figure 05-11. It is a view |
Figure 05-11 View from Death Valley |
Figure 05-12 All Sky View [large image] |
Figure 05-13a NGC7331 |
looking from inside the galactic disk. The all sky (panoramic) view in different regions of the electromagnetic spectrum is shown in Figure 05-12 (in false colours). If we could fly |
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away from the Milkyway and look back, the view would be similar to the spiral galaxy NGC 7331 as depicted in Figure 05-13a. Similar in size to our own Milky Way, spiral galaxy NGC 7331 lies about 50 million light-years away toward the constellation Pegasus. It contains a mixture of young stars in the bluer regions and an older population in the yellowish center. The total mass of NGC 7331 and the Milky Way is estimated to be several 1011 solar mass. The first painting featuring a prominent MilkyWay is probably the "Flight into Egypt" of the holy family by Adam Elsheimer in 1609 (see Figure 05-13b). In the Middle Ages, it is called the "Jacob's Ladder" leading |
Figure 05-13b Milkyway, Artist's View [view large image] |
to heaven in his dream. The MilkyWay was also known as "Silvery River" in other folklore. |
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Milky Way can draw on to make new stars. An August 2008 report from the Sloan Digital Sky Survey indicates that there are many stellar streams crisscrossing the Milky Way halo. They are the stars torn from disrupted satellite galaxies that have merged with the Milky Way. Figure 05-15a is a theoretical model of a galaxy like the Milky Way showing many trails of stars . The region shown is about 1 million light-years on a side; the Sun is just 25,000 light-years from the center of the galaxy and would appear close to the center of this picture. |
Figure 05-14 Milky Way Neighborhood [large image] |
Figure 05-15a Milky Way Streams [view large image] |
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The disk of the Milky Way8 exhibits a spiral structure, which shows up in the distribution of objects populating the disk component. These objects include, the HI regions of neutral hydrogen atoms, the population I objects such as young stars, diffuse star-forming nebulae9, H II regions of ionized hydrogen atoms and open star clusters. These population I objects are very young, in contrast to the very old population II objects in the Milky Way's Halo (globular clusters and old stars, including older planetary nebulae). The arms of the Milky Way, at least near the solar neighborhood in our Galaxy, are typically named for the constellations where more prominent parts of them are situated. The solar system is trundleing around at nearly 200 km/sec in the Local or Orion Arm - a spur in between the more substantial Sagittarius and Perseus arms. The Milky Way is now known as a barred spiral. The evidence, at first indirect, began to accumulate in 1975: stars and gas tracked in the middle of the Milky Way did not follow the orbits they would if the spiral pattern |
Figure 05-15b Barred Milky Way [view large image] |
reached all the way in. Recent surveys of the sky in near-infrared light have revealed the bar directly and dispelled the remaining doubts (Figure 05-15b). |
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specks throughout the picture are individual Milky Way stars. The new data also reveal a structure different from the traditional view. It finds that the Milky Way is a barred spiral with only two major arms - the Scutum-Centaurus and Perseus arms. They contain the greatest densities of both young, bright stars, and older, so-called red-giant stars. The two minor arms, Sagittarius and Norma, are filled with gas and pockets of young stars. The solar system lies near a small, partial arm called the Orion Arm, or Spur |
Figure 05-15c Milky Way, |
Figure 05-15d Latest Version [large image] |
(see an artist's rendition in Figure 05-15d). While most of the arms are spiraling inward to the center, the 3 kpc arms are expanding at speed more than 50 km/sec. |
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Top View : 1. Galactic Center - A super-massive black hole of 4 million solar mass is sitting at the center. It is about 8 kpc from Earth. 2. Galactic Bar - It is a region about 8.6 kpc long, where stars orbit in narrow elliptical instead of circular paths. 3. Central Molecular Zone - This zone contains dense, turbulent gas that gives rise to new stars at a higher rate than more outlying regions. It is about 7.4 kpc across. 4. Spiral Arm - When orbiting stars and gas enter the arms, they slow down and bunch up triggering star birth. 5. Gas Flow - The gas entering a spiral arm deflects slightly toward the galactic center, where it fuels star birth. 6. Spiral Flow - The movement of gas, dust, and stars forms a spiral pattern, which indicates a "sink" (the black hole) at the galactic center. |
Figure 05-16a Milky Way Components |
Side View : |
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12. Bubbles and Beams - It was discovered by NASA's Fermi Gamma-ray Space Telescope in 2010 that there are pairs of gamma-ray bubbles and beams emanating up and down from the Milky Ways's center out to a distance of 27000 light-years (Figure 05-16b, by artist's impression). These features indicate that the Milky Way was much more active not long ago. The beams likely resulted from hot matter squeezing through the |
Figure 05-16b Bubbles and Beams from Milky Way Center |
Figure 05-16c Centaurus A [view large image] |
magnetic field in the galactic center while the bubbles probably formed from the push of material spewing from the central black hole. |
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It is found recently that the central black hole invariably comprises about 0.5% of the mass of the stars in the spheroid of the galaxies. This is referred to as the Magorrian relation, the same relationship is also applicable to the black holes in some globular clusters. A galaxy's spheroid is the round central bulge in a spiral galaxy, or the whole galaxy with an elliptical. It seems that once the black hole reaches a particular maximum mass, it would shut off its own growth by forcing orbits of surrounding stars to become more circular. This keeps them out of the black hole's powerful grip. If this process happened commonly, most galaxies |
Figure 05-16f Sagittarius |
must have undergone a bright quasarlike phase in their youth, when the central black hole was growing by ingesting material and producing quasarlike symptoms. |
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The development of a central black hole may be an unavoidable part of a galaxy's formation and evolution. The black hole at the Milky Way center is located at SgrA* toward a point in the constellation Sagittarius (Figure 05-16f). It shows no sign of motion, has a mass of 3.7 million suns, its size is smaller than the solar system and is in a much quieter phase comparing to the AGN's or quasars. The upper portion of Figure 05-17a shows a 400 by 900 light-years mosaic of Chandra X-ray images toward the central region of the Milky Way. It reveals thousands of white dwarf stars, neutron stars, and black holes bathed in an incandescent fog of multimillion-degree gas. The supermassive black hole at the Milky Way center is located inside the bright white patch at the center of the image. The colors indicate X-ray energy bands - red (low), green (medium), and blue (high). The lower part of Figure 05-17a is a blow-up of the central region. It shows four (A-D) of the large number of variable x-ray sources - likely black holes or neutron stars in binary star systems - swarming around the Milky Way's central supermassive black hole. While four sources may not make a swarm, these all lie within only three light-years of Sgr A* (the bright source just above C). Repeated gravitational interactions with other stars are thought to cause |
Figure 05-17a Milky Way Center, SgrA* |
the system near the black hole to spiral inward toward the Galactic Center. |
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In 2005, the Chandra X-ray Observatory discovered more than 50 massive stars (with mass = 30 - 50 MSun) in a big dust ring around the central black hole of the Milky Way at less than a light year's distance (Figure 05-17b). According to the standard model for star formation, gas clouds from which stars form should have been ripped apart by tidal forces from the supermassive black hole. Evidently, the gravity of a dense disk of gas around Sagittarius A* offsets the tidal forces and allows stars to form. Since there are no low mass stars in this region, it strongly suggests that the massive stars must have formed where we see them now - around the black hole. They would not be members of star cluster migrating from a more distant location.The discovery may also explain the large amounts of heavy elements such as oxygen and iron observed in the disks of supermassive black holes. |
Figure 05-17b Massive Stars near the BH [view large image] |
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movie in infrared light detailing how stars in the central light-year of our Galaxy have moved over a period of eight years. The yellow mark at the image center represents the location of Sgr A*. Motion of S2 |
Figure 05-17c BH at MW Center [view large image] |
Figure 05-17d Stars near BH [view large image] |
Figure 05-17e S2 Orbit Arount BH |
around the black hole is plotted in Figure 05-17e. |
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It is reported in November 2005 that compact radio source at wavelength of 3.5 mm from gas in a region just 8 light minutes (~1.44x1013 cm) across, centered on the Milky Way black hole, was measured by the Very long Baseline Array, which is a system of ten radio telescopes scattered across the United States. Figure 05-17f shows a super-resolution image with a circular beam of 0.2 mas (major axis size) from which an east-west elongated structure can be seen. The Schwarzschild radius Rs is 1.2 x 1012 cm according to the latest estimated value for |
Figure 05-17f Radio SgrA* [view large image] |
Figure 05-17g BH Shadow [view large image] |
the mass of the central black hole (~ 4 x 106 Msun). Thus, the size of the unresolved beam (the circle) is 2.5 Rs with the black hole just hidden inside. A 2007 measurement at a wavelength |
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horizon of a black hole completely absorbs emissions from matter behind when viewed from Earth. The result is a darker circle that could be seen in a sufficiently high-resolution image. The tendency of photons to be flung around the black hole in the direction of its rotation brings about an event-horizon shadow that is off-center, to the right in this picture. A brighter ring around the shadow is formed by light rays, which are strongly deflected by the gravitational pull of the black hole without being absorbed by it. The real image of a black hole has been captured sitting at the center of the face-on spiral galaxy NGC1097 (Figure 05-17h). It is a view looking down from the top. Matter |
Figure 05-17h NGC1097 |
is falling in from bars of stars and gas. The black hole is surrounded by hot gas and bright stars. This mysterious object is completely obscure by the jet stream (in green color) shooting out toward the viewing direction. |
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of massive, young stars (white and blue). Farther out are clouds and curtains of interstellar dust, which reflect the light from flares occurring when gas falls into the black hole. The region is also home to some very young, very dense star clusters (the blue stars at the upper left). |
Figure 05-17i Milky Way Center [view large image] |
Figure 05-17j Objects near BH |
Figure 05-17k MW Center, Star Tracks [view large image] |
Another artist's rendition in Figure 05-17j depicts the various objects and processes near a massive black hole. |
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Figure 05-17l Milkyway Centre Zoom In [view large image] |
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Figure 05-17l depicts a sequence of images to zoom in to the centre of the Milky Way utilizing the penetration power of different kinds of electromagnetic wave. The size of the region or object is indicted for each frame. Figure 05-17m is a blowup of frame # 3 in Figure 05-17l with radio image in red, X-ray image in blue. It shows the radio arc jutting straight out from the Galactic plane and a zoom in view of the Arches, which is the most compact cluster of stars known in the Milky Way. One hypothesis holds that the Radio Arc and the Arches have such geometrical shapes because they contain hot plasma flowing along lines of constant magnetic field. Images from the Chandra X-ray Observatory appear to show this plasma colliding with a nearby cloud of cold gas. The black hole at the Galactic center is hidden inside the bright radio structure. |
Figure 05-17m Radio Arc |
The insert at the lower right is imaged at 20 cm (purple) with the NRAO Very Large Array, tracing H II regions that are illuminated by hot, massive stars, supernova remnants, and synchrotron emission. Emission at 1.1 mm (orange) was observed |
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On July 2012 NASA's Nuclear Spectroscopic Telescope Array (NuSTAR) has captured the flare up of X-ray during a period of 2 days at SgrA* (see time-lapse images on the right of Figure 05-17o). Such event is interpreted as the sign of material falling into the black hole. In this case the material could be gas from a nearby supernova remnant. The X-ray image at the center of the picture has been converted to visual colors with blue for 10 - 30 kev, green for 7 - 10 kev, and red for 3 - 7 kev. The time series shows X-ray energies between 3 - 30 kev corresponding to a temperature of about 100 million oC. |
Figure 05-17o X-ray from SgrA* [view large image] |
NuSTAR is a space-based X-ray telescope operating in the range of 5 to 80 keV. It was successfully launched on 13 June 2012. Its primary scientific goals are to conduct a deep survey for black holes a billion times more massive than the sun, |
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The halo is a spherical cloud of thinly scattered stars and globular clusters. It is the largest component of the Milky Way, extending to radius of about 100 kpc. It contains very little dust or gas. No star formation currently takes place there. This means that the halo contains very few young stars. Most of the halo stars are, in fact, 10 - 14 billion years, which is very close to the age of the galaxy itself. Halo stars are extreme Population II stars. They are very old, have very low metal content, and move in randomly tipped, elliptical orbits. The motion of objects in the Milky Way is not consistent with the amount of luminous matter, which is not enough to confine these objects inside the Milky Way boundary. The problem can be reconciled if a lot of dark matter still remains in the halo - the original clump of mass - while the |
Figure 05-18 Dark Matter Halo |
cooling of the hydrogen allows ordinary matter to contract, and settled into the disk. |
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of galaxies are essentially all dark matter. Figure 05-18 shows an "artist's impression" of a dark halo surrounding an almost edge-on disk galaxy. Figure 05-16f shows the dark matter distribution extends to 100 kpc. The rotation curve in Figure 05-19 provides a very convincing evidence for the pervasive presence of dark matter in the galactic halo (such as shown in M74). It is a plot of the rotational velocity of an object in the galactic plane versus distance to the center. From observations of starlight alone, the rotational velocity would be expected to fall towards the edge (dashed line). In fact the curve flattens (solid line), suggesting that galaxy is surrounded by a halo of unseen, dark matter. |
Figure 05-19 Rotation Curve [view large image] |
See more about the gamma-ray sky of the Milky Way in the Appendix. |
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1. For a star with mass m moving around the black hole the gravitational attraction must be balanced by the centrifugal repulsion: G m M / r2 = m v2 / r, from which M = r v2 / G where G = 6.67 x 10-8cm3/sec2-gm is the gravitational constant. |
Figure 05-20 [vli] Circular Motion |
= 1o =
/180 = 0.0175 radian, then the distance s covered by the star in t = 8 years = 8 x 3.15 x 107 sec is given by:
= 0.875 x 1016cm