Galaxy

<h2 id="etymology">Etymology</h2>
The word galaxy was borrowed via <a href="/facts/French_language/qe1DnaQh">French</a> and <a href="/facts/Medieval_Latin/gyLMjaCX">Medieval Latin</a> from the <a href="/facts/Greek_language/pzDd6eIz">Greek</a> term for the Milky Way, galaxías (kúklos) γαλαξίας (κύκλος)<a class="footnote-ref" id="fnref:14" href="#fn:14">14</a><a class="footnote-ref" id="fnref:15" href="#fn:15">15</a> 'milky (circle)', named after its appearance as a milky band of light in the sky.<a class="footnote-ref" id="fnref:16" href="#fn:16">16</a><a class="footnote-ref" id="fnref:17" href="#fn:17">17</a>
In the astronomical literature, the capitalised word "Galaxy" is often used to refer to the <a href="/facts/Milky_Way/ulF6lccN">Milky Way</a> galaxy, to distinguish it from the other galaxies in the <a href="/facts/Universe/XbfpnDmM">universe</a>. 
Galaxies were initially discovered telescopically and were known as <a href="/facts/Spiral_nebula/hRT2dtxJ">spiral nebulae</a>. Most 18th- to 19th-century astronomers considered them as either unresolved <a href="/facts/Star_cluster/Crs7Y6me">star clusters</a> or <a href="/facts/Extragalactic_astronomy/WtKKEWru">extragalactic</a> nebulae,: 220  but their true composition and natures remained a mystery. Observations using larger telescopes of a few nearby bright galaxies, like the <a href="/facts/Andromeda_Galaxy/MjmSLV6m">Andromeda Galaxy</a>, began resolving them into huge conglomerations of stars, but based simply on the apparent faintness and sheer population of stars, the true distances of these objects placed them well beyond the Milky Way. For this reason they were popularly called island universes. <a href="/facts/Harlow_Shapley/EBHMWFuP">Harlow Shapley</a> began to advocate for the term "galaxy" and against using "universes" and "nebula" for the objects but the very influential <a href="/facts/Edwin_Hubble/fpX3JlbJ">Edwin Hubble</a> stuck to nebulae. The nomenclature did not fully change in until Hubble's death in 1953.<a class="footnote-ref" id="fnref:18" href="#fn:18">18</a>

<h2 id="nomenclature">Nomenclature</h2>

Millions of galaxies have been catalogued, but <a href="/facts/List_of_galaxies/9PJtf6ld">only a few</a> have well-established names, such as the <a href="/facts/Andromeda_Galaxy/MjmSLV6m">Andromeda Galaxy</a>, the <a href="/facts/Magellanic_Clouds/WEspxUJl">Magellanic Clouds</a>, the <a href="/facts/Whirlpool_Galaxy/tah45nH8">Whirlpool Galaxy</a>, and the <a href="/facts/Sombrero_Galaxy/snMpBeCb">Sombrero Galaxy</a>. Astronomers work with numbers from certain <a href="/facts/List_of_astronomical_catalogues/LFtX59qs">catalogues</a>, such as the <a href="/facts/Messier_catalogue/YKz2MxzQ">Messier catalogue</a>, the NGC (<a href="/facts/New_General_Catalogue/qxfhfKAc">New General Catalogue</a>), the IC (<a href="/facts/Index_Catalogue/qxfhfKAc">Index Catalogue</a>), the CGCG (<a href="/facts/Catalogue_of_Galaxies_and_of_Clusters_of_Galaxies/C893NBVg">Catalogue of Galaxies and of Clusters of Galaxies</a>), the MCG (<a href="/facts/Morphological_Catalogue_of_Galaxies/DzaqHHfR">Morphological Catalogue of Galaxies</a>), the UGC (<a href="/facts/Uppsala_General_Catalogue/1kkIojqA">Uppsala General Catalogue</a> of Galaxies), and the PGC (<a href="/facts/Catalogue_of_Principal_Galaxies/G7KUmUQQ">Catalogue of Principal Galaxies</a>, also known as LEDA). All the well-known galaxies appear in one or more of these catalogues but each time under a different number. For example, <a href="/facts/Messier_109/PfvXkR2Y">Messier 109</a> (or "M109") is a spiral galaxy having the number 109 in the catalogue of Messier. It also has the designations NGC 3992, UGC 6937, CGCG 269–023, MCG +09-20-044, and PGC 37617 (or LEDA 37617), among others.<a class="footnote-ref" id="fnref:19" href="#fn:19">19</a> Millions of fainter galaxies are known by their identifiers in <a href="/facts/Sky_surveys/6BE1V8V6">sky surveys</a> such as the <a href="/facts/Sloan_Digital_Sky_Survey/MSHAk1RU">Sloan Digital Sky Survey</a>.<a class="footnote-ref" id="fnref:20" href="#fn:20">20</a>

<h2 id="observation-history">Observation history</h2>
<h3>Milky Way</h3>
Main article: <a href="/facts/Milky_Way/ulF6lccN">Milky Way</a>
<a href="/facts/Greek_philosophy/LWEkp8JX">Greek</a> philosopher <a href="/facts/Democritus/yTzsod3v">Democritus</a> (450–370 BCE) proposed that the bright band on the night sky known as the Milky Way might consist of distant stars.<a class="footnote-ref" id="fnref:21" href="#fn:21">21</a>
<a href="/facts/Aristotle/U2bDlBFW">Aristotle</a> (384–322 BCE), however, believed the Milky Way was caused by "the ignition of the fiery exhalation of some stars that were large, numerous and close together" and that the "ignition takes place in the upper part of the <a href="/facts/Atmosphere/oUpLaGRF">atmosphere</a>, in the <a href="/facts/Sublunary_sphere/ttYhpxtx">region of the World that is continuous with the heavenly motions</a>."<a class="footnote-ref" id="fnref:22" href="#fn:22">22</a> <a href="/facts/Neoplatonism/Tyq4uTG0">Neoplatonist</a> philosopher <a href="/facts/Olympiodorus_the_Younger/YElfIhfK">Olympiodorus the Younger</a> (c. 495–570 CE) was critical of this view, arguing that if the Milky Way was <a href="/facts/Sublunary/ttYhpxtx">sublunary</a> (situated between Earth and the Moon) it should appear different at different times and places on Earth, and that it should have <a href="/facts/Parallax/Gu8W21LP">parallax</a>, which it did not. In his view, the Milky Way was celestial.<a class="footnote-ref" id="fnref:23" href="#fn:23">23</a>
According to Mohani Mohamed, <a href="/facts/Astronomy_in_the_medieval_Islamic_world/hw8HxDHz">Arabian</a> astronomer <a href="/facts/Ibn_al-Haytham/Q5H9hm4J">Ibn al-Haytham</a> (965–1037) made the first attempt at observing and measuring the Milky Way's parallax,<a class="footnote-ref" id="fnref:24" href="#fn:24">24</a> and he thus "determined that because the Milky Way had no parallax, it must be remote from the Earth, not belonging to the atmosphere."<a class="footnote-ref" id="fnref:25" href="#fn:25">25</a> <a href="/facts/Persian_people/4GhM3jl2">Persian</a> astronomer <a href="/facts/Al-Biruni/4XbTzrYl">al-Biruni</a> (973–1048) proposed the Milky Way galaxy was "a collection of countless fragments of the nature of nebulous stars."<a class="footnote-ref" id="fnref:26" href="#fn:26">26</a> <a href="/facts/Al-Andalus/JTNmWTzP">Andalusian</a> astronomer <a href="/facts/Avempace/gG1Iq21r">Avempace</a> (d. 1138) proposed that it was composed of many stars that almost touched one another, and appeared to be a continuous image due to the effect of <a href="/facts/Refraction/S8kvSKzM">refraction</a> from sublunary material,<a class="footnote-ref" id="fnref:27" href="#fn:27">27</a><a class="footnote-ref" id="fnref:28" href="#fn:28">28</a> citing his observation of the <a href="/facts/Conjunction_(astronomy_and_astrology)/TgujumHI">conjunction</a> of Jupiter and Mars as evidence of this occurring when two objects were near.<a class="footnote-ref" id="fnref:29" href="#fn:29">29</a> In the 14th century, Syrian-born <a href="/facts/Ibn_Qayyim_al-Jawziyya/XdpWwkPM">Ibn Qayyim al-Jawziyya</a> proposed the Milky Way galaxy was "a myriad of tiny stars packed together in the sphere of the fixed stars."<a class="footnote-ref" id="fnref:30" href="#fn:30">30</a>

Actual proof of the Milky Way consisting of many stars came in 1610 when the Italian astronomer <a href="/facts/Galileo_Galilei/98VT2z3v">Galileo Galilei</a> used a <a href="/facts/Optical_telescope/dVfBR10I">telescope</a> to study it and discovered it was composed of a huge number of faint stars.<a class="footnote-ref" id="fnref:31" href="#fn:31">31</a><a class="footnote-ref" id="fnref:32" href="#fn:32">32</a> In 1750, English astronomer <a href="/facts/Thomas_Wright_(astronomer)/zlfrX17L">Thomas Wright</a>, in his An Original Theory or New Hypothesis of the Universe, correctly speculated that it might be a rotating body of a huge number of stars held together by <a href="/facts/Gravitation/bqAN7DdQ">gravitational</a> forces, akin to the <a href="/facts/Solar_System/QIcLSazQ">Solar System</a> but on a much larger scale, and that the resulting disk of stars could be seen as a band on the sky from a perspective inside it.<a class="footnote-ref" id="fnref:33" href="#fn:33">33</a><a class="footnote-ref" id="fnref:34" href="#fn:34">34</a><a class="footnote-ref" id="fnref:35" href="#fn:35">35</a> In his 1755 treatise, <a href="/facts/Immanuel_Kant/vIxjdy6I">Immanuel Kant</a> elaborated on Wright's idea about the Milky Way's structure.<a class="footnote-ref" id="fnref:36" href="#fn:36">36</a> 
The first project to describe the shape of the Milky Way and the position of the Sun was undertaken by <a href="/facts/William_Herschel/SsruaBvq">William Herschel</a> in 1785 by counting the number of stars in different regions of the sky. He produced a diagram of the shape of the galaxy with <a href="/facts/Galactocentrism/cdpEM4j0">the Solar System close to the center</a>.<a class="footnote-ref" id="fnref:37" href="#fn:37">37</a><a class="footnote-ref" id="fnref:38" href="#fn:38">38</a> Using a refined approach, <a href="/facts/Jacobus_Kapteyn/GwwvINSR">Kapteyn</a> in 1920 arrived at the picture of a small (diameter about 15 kiloparsecs) ellipsoid galaxy with the Sun close to the center. A different method by <a href="/facts/Harlow_Shapley/EBHMWFuP">Harlow Shapley</a> based on the cataloguing of <a href="/facts/Globular_cluster/FL0EERJU">globular clusters</a> led to a radically different picture: a flat disk with diameter approximately 70 kiloparsecs and the Sun far from the centre.<a class="footnote-ref" id="fnref:39" href="#fn:39">39</a> Both analyses failed to take into account the <a href="/facts/Extinction_(astronomy)/rLNLDfe1">absorption of light</a> by <a href="/facts/Cosmic_dust/Uy6hlL29">interstellar dust</a> present in the <a href="/facts/Galactic_plane/4eaqfCIB">galactic plane</a>; but after <a href="/facts/Robert_Julius_Trumpler/akR1f6lp">Robert Julius Trumpler</a> quantified this effect in 1930 by studying <a href="/facts/Open_cluster/UodlJqcx">open clusters</a>, the present picture of the Milky Way galaxy emerged.<a class="footnote-ref" id="fnref:40" href="#fn:40">40</a>

<h3>Distinction from other nebulae</h3>
A few galaxies outside the Milky Way are visible on a dark night to the <a href="/facts/Naked_eye/ePEIa0lK">unaided eye</a>, including the <a href="/facts/Andromeda_Galaxy/MjmSLV6m">Andromeda Galaxy</a>, <a href="/facts/Large_Magellanic_Cloud/7VYAehNa">Large Magellanic Cloud</a>, <a href="/facts/Small_Magellanic_Cloud/jg9s2YCl">Small Magellanic Cloud</a>, and the <a href="/facts/Triangulum_Galaxy/etLCCGhP">Triangulum Galaxy</a>. In the 10th century, Persian astronomer <a href="/facts/Abd_al-Rahman_al-Sufi/qzc2hHfl">Abd al-Rahman al-Sufi</a> made the earliest recorded identification of the Andromeda Galaxy, describing it as a "small cloud".<a class="footnote-ref" id="fnref:41" href="#fn:41">41</a> In 964, he probably mentioned the Large Magellanic Cloud in his <a href="/facts/Book_of_Fixed_Stars/8aMMc7EN">Book of Fixed Stars</a>, referring to "Al Bakr of the southern Arabs",<a class="footnote-ref" id="fnref:42" href="#fn:42">42</a> since at a <a href="/facts/Declination/5X4S4k9u">declination</a> of about 70° south it was not visible where he lived. It was not well known to Europeans until <a href="/facts/Ferdinand_Magellan/DgNLv567">Magellan</a>'s voyage in the 16th century.<a class="footnote-ref" id="fnref:43" href="#fn:43">43</a><a class="footnote-ref" id="fnref:44" href="#fn:44">44</a> The Andromeda Galaxy was later independently noted by <a href="/facts/Simon_Marius/yb54huCF">Simon Marius</a> in 1612.<a class="footnote-ref" id="fnref:45" href="#fn:45">45</a>
In 1734, philosopher <a href="/facts/Emanuel_Swedenborg/QE3Pcl8U">Emanuel Swedenborg</a> in his Principia speculated that there might be other galaxies outside that were formed into galactic clusters that were minuscule parts of the universe that extended far beyond what could be seen. These views "are remarkably close to the present-day views of the cosmos."<a class="footnote-ref" id="fnref:46" href="#fn:46">46</a>
In 1745, <a href="/facts/Pierre_Louis_Maupertuis/AcFjlBhh">Pierre Louis Maupertuis</a> conjectured that some <a href="/facts/Nebula/hG6coklY">nebula</a>-like objects were collections of stars with unique properties, including a <a href="/facts/Relativistic_jets/QYerB8R3">glow exceeding the light</a> its stars produced on their own, and repeated <a href="/facts/Johannes_Hevelius/JJSooIep">Johannes Hevelius</a>'s view that the bright spots were massive and flattened due to their rotation.<a class="footnote-ref" id="fnref:47" href="#fn:47">47</a>
In 1750, <a href="/facts/Thomas_Wright_(astronomer)/zlfrX17L">Thomas Wright</a> correctly speculated that the Milky Way was a flattened disk of stars, and that some of the nebulae visible in the night sky might be separate Milky Ways.<a class="footnote-ref" id="fnref:48" href="#fn:48">48</a><a class="footnote-ref" id="fnref:49" href="#fn:49">49</a>

Toward the end of the 18th century, <a href="/facts/Charles_Messier/dTokW7Yy">Charles Messier</a> compiled a <a href="/facts/Messier_object/YKz2MxzQ">catalog</a> containing the 109 brightest celestial objects having nebulous appearance. Subsequently, William Herschel assembled a catalog of 5,000 nebulae.<a class="footnote-ref" id="fnref:50" href="#fn:50">50</a> In 1845, <a href="/facts/William_Parsons,_3rd_Earl_of_Rosse/bPQ37rMF">Lord Rosse</a> examined the nebulae catalogued by Herschel and observed the spiral structure of <a href="/facts/Whirlpool_Galaxy/tah45nH8">Messier object M51</a>, now known as the Whirlpool Galaxy.<a class="footnote-ref" id="fnref:51" href="#fn:51">51</a><a class="footnote-ref" id="fnref:52" href="#fn:52">52</a>
In 1912, <a href="/facts/Vesto_M._Slipher/ewBeHwIC">Vesto M. Slipher</a> made spectrographic studies of the brightest spiral nebulae to determine their composition. Slipher discovered that the spiral nebulae have high <a href="/facts/Doppler_shift/bzrK1BKf">Doppler shifts</a>, indicating that they are moving at a rate exceeding the velocity of the stars he had measured. He found that the majority of these nebulae are moving away from us.<a class="footnote-ref" id="fnref:53" href="#fn:53">53</a><a class="footnote-ref" id="fnref:54" href="#fn:54">54</a>
In 1917, <a href="/facts/Heber_Doust_Curtis/KaGog5aI">Heber Doust Curtis</a> observed nova <a href="/facts/S_Andromedae/cDoSrkRh">S Andromedae</a> within the "Great <a href="/facts/Andromeda_(constellation)/PN2eI1WI">Andromeda</a> Nebula", as the Andromeda Galaxy, <a href="/facts/Messier_object/YKz2MxzQ">Messier object</a> <a href="/facts/Andromeda_Galaxy/MjmSLV6m">M31</a>, was then known. Searching the photographic record, he found 11 more <a href="/facts/Nova/H1GcmKXT">novae</a>. Curtis noticed that these novae were, on average, 10 <a href="/facts/Magnitude_(astronomy)/f4FbscJu">magnitudes</a> fainter than those that occurred within this galaxy. As a result, he was able to come up with a distance estimate of 150,000 <a href="/facts/Parsec/SwSsk57J">parsecs</a>. He became a proponent of the so-called "island universes" hypothesis, which holds that spiral nebulae are actually independent galaxies.<a class="footnote-ref" id="fnref:55" href="#fn:55">55</a>
In 1920 a debate took place between <a href="/facts/Harlow_Shapley/EBHMWFuP">Harlow Shapley</a> and <a href="/facts/Heber_Curtis/KaGog5aI">Heber Curtis</a>, the <a href="/facts/Great_Debate_(astronomy)/aF4mJfJe">Great Debate</a>, concerning the nature of the Milky Way, spiral nebulae, and the dimensions of the universe. To support his claim that the Great Andromeda Nebula is an external galaxy, Curtis noted the appearance of dark lanes resembling the dust clouds in the Milky Way, as well as the significant Doppler shift.<a class="footnote-ref" id="fnref:56" href="#fn:56">56</a>
In 1922, the <a href="/facts/Estonia/PVjB16TI">Estonian</a> astronomer <a href="/facts/Ernst_%C3%96pik/DYT6Pmpx">Ernst Öpik</a> gave a distance determination that supported the theory that the Andromeda Nebula is indeed a distant extra-galactic object.<a class="footnote-ref" id="fnref:57" href="#fn:57">57</a> Using the new 100-inch <a href="/facts/Mount_Wilson_Observatory/pYrLP2uH">Mt. Wilson</a> telescope, <a href="/facts/Edwin_Hubble/fpX3JlbJ">Edwin Hubble</a> was able to resolve the outer parts of some spiral nebulae as collections of individual stars and identified some <a href="/facts/Cepheid_variable/WQXaAFmW">Cepheid variables</a>, thus allowing him to estimate the distance to the nebulae: they were far too distant to be part of the Milky Way.<a class="footnote-ref" id="fnref:58" href="#fn:58">58</a> In 1926 Hubble produced a classification of <a href="/facts/Galaxy_morphological_classification/AGbMJ9Dp">galactic morphology</a> that is used to this day.<a class="footnote-ref" id="fnref:59" href="#fn:59">59</a><a class="footnote-ref" id="fnref:60" href="#fn:60">60</a>

<h3>Multi-wavelength observation</h3>
See also: <a href="/facts/Observational_astronomy/PKgYt9PX">Observational astronomy</a>

Advances in astronomy have always been driven by technology. After centuries of success in <a href="/facts/Optical_astronomy/bbfzMHAn">optical astronomy</a>, recent decades have seen major progress in other regions of the <a href="/facts/Electromagnetic_spectrum/24LARvFY">electromagnetic spectrum</a>.<a class="footnote-ref" id="fnref:61" href="#fn:61">61</a>
The <a href="/facts/Cosmic_dust/Uy6hlL29">dust</a> present in the interstellar medium is opaque to visual light. It is more transparent to <a href="/facts/Far_infrared_astronomy/jwjIFDYB">far-infrared</a>, which can be used to observe the interior regions of giant molecular clouds and <a href="/facts/Bulge_(astronomy)/cjJ0LFan">galactic cores</a> in great detail.<a class="footnote-ref" id="fnref:62" href="#fn:62">62</a> Infrared is also used to observe distant, <a href="/facts/Redshift/Qfl4VjDF">red-shifted</a> galaxies that were formed much earlier. Water vapor and <a href="/facts/Carbon_dioxide/xGzpppEp">carbon dioxide</a> absorb a number of useful portions of the infrared spectrum, so high-altitude or space-based telescopes are used for <a href="/facts/Infrared_astronomy/WEmAadyf">infrared astronomy</a>.<a class="footnote-ref" id="fnref:63" href="#fn:63">63</a>
The first non-visual study of galaxies, particularly active galaxies, was made using <a href="/facts/Radio_astronomy/TdjF4LgL">radio frequencies</a>. The Earth's atmosphere is nearly transparent to radio between 5 <a href="/facts/Hertz/6Wshj5qm">MHz</a> and 30 GHz. The <a href="/facts/Ionosphere/mT9tTBE5">ionosphere</a> blocks signals below this range.<a class="footnote-ref" id="fnref:64" href="#fn:64">64</a> Large radio <a href="/facts/Interferometry/X3E1SsQT">interferometers</a> have been used to map the active jets emitted from active nuclei.
<a href="/facts/UV_astronomy/X4Y86Wg7">Ultraviolet</a> and <a href="/facts/X-ray_astronomy/KAQ6WxgQ">X-ray telescopes</a> can observe highly energetic galactic phenomena. Ultraviolet flares are sometimes observed when a star in a distant galaxy is torn apart from the tidal forces of a nearby black hole.<a class="footnote-ref" id="fnref:65" href="#fn:65">65</a> The distribution of hot gas in galactic clusters can be mapped by X-rays. The existence of supermassive black holes at the cores of galaxies was confirmed through X-ray astronomy.<a class="footnote-ref" id="fnref:66" href="#fn:66">66</a>

<h3>Modern research</h3>

In 1944, <a href="/facts/Hendrik_C._van_de_Hulst/CKc332Up">Hendrik van de Hulst</a> predicted that <a href="/facts/Microwave/HmVSN31Y">microwave</a> radiation with <a href="/facts/Hydrogen_line/fQaWCT2t">wavelength of 21 cm</a> would be detectable from interstellar atomic <a href="/facts/Hydrogen/BoYHjl0J">hydrogen</a> gas;<a class="footnote-ref" id="fnref:67" href="#fn:67">67</a> and in 1951 it was observed. This radiation is not affected by dust absorption, and so its Doppler shift can be used to map the motion of the gas in this galaxy. These observations led to the hypothesis of a rotating <a href="/facts/Barred_spiral_galaxy/cntSCFX4">bar structure</a> in the center of this galaxy.<a class="footnote-ref" id="fnref:68" href="#fn:68">68</a> With improved <a href="/facts/Radio_telescope/SxIXUowL">radio telescopes</a>, hydrogen gas could also be traced in other galaxies.
In the 1970s, <a href="/facts/Vera_Rubin/wKHXHVIp">Vera Rubin</a> uncovered a discrepancy between observed galactic <a href="/facts/Galaxy_rotation_curve/YJyb1Jy3">rotation speed</a> and that predicted by the visible mass of stars and gas. Today, the galaxy rotation problem is thought to be explained by the presence of large quantities of unseen <a href="/facts/Dark_matter/y5HgX55N">dark matter</a>.<a class="footnote-ref" id="fnref:69" href="#fn:69">69</a><a class="footnote-ref" id="fnref:70" href="#fn:70">70</a>
Beginning in the 1990s, the <a href="/facts/Hubble_Space_Telescope/NQeIf0vw">Hubble Space Telescope</a> yielded improved observations. Among other things, its data helped establish that the missing dark matter in this galaxy could not consist solely of inherently faint and small stars.<a class="footnote-ref" id="fnref:71" href="#fn:71">71</a> The <a href="/facts/Hubble_Deep_Field/Auz98FQg">Hubble Deep Field</a>, an extremely long exposure of a relatively empty part of the sky, provided evidence that there are about 125 billion (1.25×1011) galaxies in the observable universe.<a class="footnote-ref" id="fnref:72" href="#fn:72">72</a> Improved technology in detecting the <a href="/facts/Electromagnetic_spectrum/24LARvFY">spectra</a> invisible to humans (radio telescopes, infrared cameras, and <a href="/facts/X-ray_astronomy/KAQ6WxgQ">x-ray telescopes</a>) allows detection of other galaxies that are not detected by Hubble. Particularly, surveys in the <a href="/facts/Zone_of_Avoidance/xcrH3whk">Zone of Avoidance</a> (the region of sky blocked at visible-light wavelengths by the Milky Way) have revealed a number of new galaxies.<a class="footnote-ref" id="fnref:73" href="#fn:73">73</a>
A 2016 study published in <a href="/facts/The_Astrophysical_Journal/jSYn0eez">The Astrophysical Journal</a>, led by <a href="/facts/Christopher_Conselice/znTsuNG4">Christopher Conselice</a> of the <a href="/facts/University_of_Nottingham/PR8osn19">University of Nottingham</a>, analyzed many sources of data to estimate that the observable universe (up to z=8) contained at least two trillion (2×1012) galaxies, a factor of 10 more than are directly observed in <a href="/facts/Hubble_Space_Telescope/NQeIf0vw">Hubble</a> images.<a class="footnote-ref" id="fnref:74" href="#fn:74">74</a>: 12 <a class="footnote-ref" id="fnref:75" href="#fn:75">75</a> However, later observations with the <a href="/facts/New_Horizons/G5XTU5DK">New Horizons</a> space probe from outside the <a href="/facts/Zodiacal_light/HqQjsaox">zodiacal light</a> observed less cosmic optical light than Conselice while still suggesting that direct observations are missing galaxies.<a class="footnote-ref" id="fnref:76" href="#fn:76">76</a><a class="footnote-ref" id="fnref:77" href="#fn:77">77</a>

<h2 id="types-and-morphology">Types and morphology</h2>
See also: <a href="/facts/Galactic_bulge/cjJ0LFan">Galactic bulge</a>, <a href="/facts/Central_massive_object/bkNq2nzR">Central massive object</a>, <a href="/facts/Active_galactic_nucleus/qT1owvXz">Active galactic nucleus</a>, and <a href="/facts/Galaxy_morphological_classification/AGbMJ9Dp">Galaxy morphological classification</a>

Galaxies come in three main types: ellipticals, spirals, and irregulars. A slightly more extensive description of galaxy types based on their appearance is given by the <a href="/facts/Hubble_sequence/LXD95esK">Hubble sequence</a>. Since the Hubble sequence is entirely based upon visual morphological type (shape), it may miss certain important characteristics of galaxies such as <a href="/facts/Star_formation/SMyfVDY6">star formation</a> rate in <a href="/facts/Starburst_galaxy/EV0wM4Rs">starburst galaxies</a> and activity in the cores of <a href="/facts/Active_galaxy/qT1owvXz">active galaxies</a>.<a class="footnote-ref" id="fnref:78" href="#fn:78">78</a>
Many galaxies are thought to contain a supermassive black hole at their center. This includes the Milky Way, whose core region is called the <a href="/facts/Galactic_Center/TI4MwWwM">Galactic Center</a>.<a class="footnote-ref" id="fnref:79" href="#fn:79">79</a>

<h3>Ellipticals</h3>
Main article: <a href="/facts/Elliptical_galaxy/1PUchrj1">Elliptical galaxy</a>
The Hubble classification system rates elliptical galaxies on the basis of their ellipticity, ranging from E0, being nearly spherical, up to E7, which is highly elongated. These galaxies have an <a href="/facts/Ellipsoid/pe9vm0Sh">ellipsoidal</a> profile, giving them an elliptical appearance regardless of the viewing angle. Their appearance shows little structure and they typically have relatively little <a href="/facts/Interstellar_medium/mokU0WEz">interstellar matter</a>. Consequently, these galaxies also have a low portion of <a href="/facts/Open_cluster/UodlJqcx">open clusters</a> and a reduced rate of new star formation. Instead, they are dominated by generally older, more <a href="/facts/Stellar_evolution/Qa4vAGmn">evolved stars</a> that are orbiting the common center of gravity in random directions. The stars contain low abundances of heavy elements because star formation ceases after the initial burst. In this sense they have some similarity to the much smaller <a href="/facts/Globular_cluster/FL0EERJU">globular clusters</a>.<a class="footnote-ref" id="fnref:80" href="#fn:80">80</a>

<h4>Type-cD galaxies</h4>

The <a href="/facts/List_of_largest_galaxies/9PJtf6ld">largest galaxies</a> are the <a href="/facts/Type-cD_galaxy/1n0mMurr">type-cD galaxies</a>.
First described in 1964 by a paper by Thomas A. Matthews and others,<a class="footnote-ref" id="fnref:81" href="#fn:81">81</a> they are a subtype of the more general class of D galaxies, which are giant elliptical galaxies, except that they are much larger. They are popularly known as the supergiant elliptical galaxies and constitute the largest and most luminous galaxies known. These galaxies feature a central elliptical nucleus with an extensive, faint halo of stars extending to megaparsec scales.<a class="footnote-ref" id="fnref:82" href="#fn:82">82</a> The profile of their surface brightnesses as a function of their radius (or distance from their cores) falls off more slowly than their smaller counterparts.<a class="footnote-ref" id="fnref:83" href="#fn:83">83</a>
The formation of these cD galaxies remains an active area of research, but the leading model is that they are the result of the mergers of smaller galaxies in the environments of dense clusters, or even those outside of clusters with random overdensities.<a class="footnote-ref" id="fnref:84" href="#fn:84">84</a> These processes are the mechanisms that drive the formation of fossil groups or fossil clusters, where a large, relatively isolated, supergiant elliptical resides in the middle of the cluster and are surrounded by an extensive cloud of X-rays as the residue of these galactic collisions. Another older model posits the phenomenon of <a href="/facts/Cooling_flow/7HotuHJy">cooling flow</a>, where the heated gases in clusters collapses towards their centers as they cool, forming stars in the process,<a class="footnote-ref" id="fnref:85" href="#fn:85">85</a> a phenomenon observed in clusters such as <a href="/facts/Perseus_Cluster/t3scp0Sg">Perseus</a>,<a class="footnote-ref" id="fnref:86" href="#fn:86">86</a> and more recently in the <a href="/facts/Phoenix_Cluster/fAQulz61">Phoenix Cluster</a>.<a class="footnote-ref" id="fnref:87" href="#fn:87">87</a>

<h4>Shell galaxy</h4>

A shell galaxy is a type of elliptical galaxy where the stars in its halo are arranged in concentric shells. About one-tenth of elliptical galaxies have a shell-like structure, which has never been observed in spiral galaxies. These structures are thought to develop when a larger galaxy absorbs a smaller companion galaxy—that as the two galaxy centers approach, they start to oscillate around a center point, and the oscillation creates gravitational ripples forming the shells of stars, similar to ripples spreading on water. For example, galaxy <a href="/facts/NGC_3923/aG6CAX0y">NGC 3923</a> has over 20 shells.<a class="footnote-ref" id="fnref:88" href="#fn:88">88</a>

<h3>Spirals</h3>
Main articles: <a href="/facts/Spiral_galaxy/hRT2dtxJ">Spiral galaxy</a> and <a href="/facts/Barred_spiral_galaxy/cntSCFX4">Barred spiral galaxy</a>

Spiral galaxies resemble spiraling <a href="/facts/Pinwheel_(toy)/74YR2yIw">pinwheels</a>. Though the stars and other visible material contained in such a galaxy lie mostly on a plane, the majority of mass in spiral galaxies exists in a roughly spherical halo of <a href="/facts/Dark_matter/y5HgX55N">dark matter</a> which extends beyond the visible component, as demonstrated by the universal rotation curve concept.<a class="footnote-ref" id="fnref:89" href="#fn:89">89</a>
Spiral galaxies consist of a rotating disk of stars and interstellar medium, along with a central bulge of generally older stars. Extending outward from the <a href="/facts/Bulge_(astronomy)/cjJ0LFan">bulge</a> are relatively bright arms. In the Hubble classification scheme, spiral galaxies are listed as type S, followed by a letter (a, b, or c) which indicates the degree of tightness of the spiral arms and the size of the central bulge. An Sa galaxy has tightly wound, poorly defined arms and possesses a relatively large core region. At the other extreme, an Sc galaxy has open, well-defined arms and a small core region.<a class="footnote-ref" id="fnref:90" href="#fn:90">90</a> A galaxy with poorly defined arms is sometimes referred to as a <a href="/facts/Flocculent_spiral_galaxy/M6jtYBlR">flocculent spiral galaxy</a>; in contrast to the <a href="/facts/Grand_design_spiral_galaxy/0TIMfSS2">grand design spiral galaxy</a> that has prominent and well-defined spiral arms.<a class="footnote-ref" id="fnref:91" href="#fn:91">91</a> The speed in which a galaxy rotates is thought to correlate with the flatness of the disc as some spiral galaxies have thick bulges, while others are thin and dense.<a class="footnote-ref" id="fnref:92" href="#fn:92">92</a><a class="footnote-ref" id="fnref:93" href="#fn:93">93</a>

In spiral galaxies, the spiral arms do have the shape of approximate <a href="/facts/Logarithmic_spiral/4rwkxL7B">logarithmic spirals</a>, a pattern that can be theoretically shown to result from a disturbance in a uniformly rotating mass of stars. Like the stars, the spiral arms rotate around the center, but they do so with constant <a href="/facts/Angular_velocity/2n8JljAT">angular velocity</a>. The spiral arms are thought to be areas of high-density matter, or "<a href="/facts/Density_wave_theory/SkR3bARs">density waves</a>".<a class="footnote-ref" id="fnref:94" href="#fn:94">94</a> As stars move through an arm, the space velocity of each stellar system is modified by the gravitational force of the higher density. (The velocity returns to normal after the stars depart on the other side of the arm.) This effect is akin to a "wave" of slowdowns moving along a highway full of moving cars. The arms are visible because the high density facilitates star formation, and therefore they harbor many bright and young stars.<a class="footnote-ref" id="fnref:95" href="#fn:95">95</a>

<h4>Barred spiral galaxy</h4>
A majority of spiral galaxies, including the <a href="/facts/Milky_Way/ulF6lccN">Milky Way</a> galaxy, have a linear, bar-shaped band of stars that extends outward to either side of the core, then merges into the spiral arm structure.<a class="footnote-ref" id="fnref:96" href="#fn:96">96</a> In the Hubble classification scheme, these are designated by an SB, followed by a lower-case letter (a, b or c) which indicates the form of the spiral arms (in the same manner as the categorization of normal spiral galaxies). Bars are thought to be temporary structures that can occur as a result of a density wave radiating outward from the core, or else due to a <a href="/facts/Galactic_tide/0X0cJblB">tidal interaction</a> with another galaxy.<a class="footnote-ref" id="fnref:97" href="#fn:97">97</a> Many barred spiral galaxies are active, possibly as a result of gas being channeled into the core along the arms.<a class="footnote-ref" id="fnref:98" href="#fn:98">98</a>
Our own galaxy, the <a href="/facts/Milky_Way/ulF6lccN">Milky Way</a>, is a large disk-shaped barred-spiral galaxy<a class="footnote-ref" id="fnref:99" href="#fn:99">99</a> about 30 kiloparsecs in diameter and a kiloparsec thick. It contains about two hundred billion (2×1011)<a class="footnote-ref" id="fnref:100" href="#fn:100">100</a> stars and has a total mass of about six hundred billion (6×1011) times the mass of the Sun.<a class="footnote-ref" id="fnref:101" href="#fn:101">101</a>

<h4>Super-luminous spiral</h4>
Recently, researchers described galaxies called super-luminous spirals. They are very large with an upward diameter of 437,000 light-years (compared to the Milky Way's 87,400 light-year diameter). With a mass of 340 billion solar masses, they generate a significant amount of ultraviolet and mid-infrared light. They are thought to have an increased star formation rate around 30 times faster than the Milky Way.<a class="footnote-ref" id="fnref:102" href="#fn:102">102</a><a class="footnote-ref" id="fnref:103" href="#fn:103">103</a>

<h3>Other morphologies</h3>
<ul><li><a href="/facts/Peculiar_galaxy/pd810k2m">Peculiar galaxies</a> are galactic formations that develop unusual properties due to tidal interactions with other galaxies.
<ul><li>A <a href="/facts/Ring_galaxy/1uyJ4KoF">ring galaxy</a> has a ring-like structure of stars and interstellar medium surrounding a bare core. A ring galaxy is thought to occur when a smaller galaxy passes through the core of a spiral galaxy.<a class="footnote-ref" id="fnref:104" href="#fn:104">104</a> Such an event may have affected the <a href="/facts/Andromeda_Galaxy/MjmSLV6m">Andromeda Galaxy</a>, as it displays a multi-ring-like structure when viewed in <a href="/facts/Infrared/44XdJNcc">infrared</a> radiation.<a class="footnote-ref" id="fnref:105" href="#fn:105">105</a></li></ul></li>
<li>A <a href="/facts/Lenticular_galaxy/UuG7XJYf">lenticular galaxy</a> is an intermediate form that has properties of both elliptical and spiral galaxies. These are categorized as Hubble type S0, and they possess ill-defined spiral arms with an elliptical halo of stars<a class="footnote-ref" id="fnref:106" href="#fn:106">106</a> (<a href="/facts/Barred_lenticular_galaxy/UuG7XJYf">barred lenticular galaxies</a> receive Hubble classification SB0).</li>
<li><a href="/facts/Irregular_galaxy/P95rRpYR">Irregular galaxies</a> are galaxies that can not be readily classified into an elliptical or spiral morphology.
<ul><li>An Irr-I galaxy has some structure but does not align cleanly with the Hubble classification scheme.</li>
<li>Irr-II galaxies do not possess any structure that resembles a Hubble classification, and may have been disrupted.<a class="footnote-ref" id="fnref:107" href="#fn:107">107</a> Nearby examples of (dwarf) irregular galaxies include the <a href="/facts/Magellanic_Clouds/WEspxUJl">Magellanic Clouds</a>.<a class="footnote-ref" id="fnref:108" href="#fn:108">108</a></li></ul></li></ul>
<ul><li>A <a href="/facts/Dark_galaxy/Ja0gWgLT">dark</a> or "ultra diffuse" galaxy is an extremely-low-luminosity galaxy. It may be the same size as the Milky Way, but have a visible star count only one percent of the Milky Way's. Multiple mechanisms for producing this type of galaxy have been proposed, and it is possible that different dark galaxies formed by different means.<a class="footnote-ref" id="fnref:109" href="#fn:109">109</a> One candidate explanation for the low luminosity is that the galaxy lost its star-forming gas at an early stage, resulting in old stellar populations.<a class="footnote-ref" id="fnref:110" href="#fn:110">110</a><a class="footnote-ref" id="fnref:111" href="#fn:111">111</a></li></ul>
<h3>Dwarfs</h3>
Main article: <a href="/facts/Dwarf_galaxy/TKS7W9tA">Dwarf galaxy</a>
Despite the prominence of large elliptical and spiral galaxies, most galaxies are dwarf galaxies.<a class="footnote-ref" id="fnref:112" href="#fn:112">112</a> They are relatively small when compared with other galactic formations, being about one hundredth the size of the Milky Way, with only a few billion stars. <a href="/facts/Blue_compact_dwarf/TKS7W9tA">Blue compact dwarf</a> galaxies contains large clusters of <a href="/facts/OB_star/npDSPUhp">young, hot, massive stars</a>. Ultra-compact dwarf galaxies have been discovered that are only 100 parsecs across.<a class="footnote-ref" id="fnref:113" href="#fn:113">113</a>
Many dwarf galaxies may orbit a single larger galaxy; the Milky Way has at least a dozen such satellites, with an estimated 300–500 yet to be discovered.<a class="footnote-ref" id="fnref:114" href="#fn:114">114</a>
Most of the information we have about dwarf galaxies come from observations of the <a href="/facts/Local_group/rAr5xEzF">local group</a>, containing two spiral galaxies, the Milky Way and Andromeda, and many dwarf galaxies. These dwarf galaxies are classified as either <a href="/facts/Irregular_galaxy/P95rRpYR">irregular</a> or <a href="/facts/Dwarf_elliptical_galaxy/YAFNrdSc">dwarf elliptical</a>/<a href="/facts/Dwarf_spheroidal_galaxy/g791E8ly">dwarf spheroidal galaxies</a>.<a class="footnote-ref" id="fnref:115" href="#fn:115">115</a>
A study of 27 Milky Way neighbors found that in all dwarf galaxies, the central mass is approximately 10 million <a href="/facts/Solar_mass/j6Auhku8">solar masses</a>, regardless of whether it has thousands or millions of stars. This suggests that galaxies are largely formed by <a href="/facts/Dark_matter/y5HgX55N">dark matter</a>, and that the minimum size may indicate a form of <a href="/facts/Warm_dark_matter/bbql6u4H">warm dark matter</a> incapable of gravitational coalescence on a smaller scale.<a class="footnote-ref" id="fnref:116" href="#fn:116">116</a>

<h2 id="variants">Variants</h2>
<h3>Interacting</h3>
Main article: <a href="/facts/Interacting_galaxy/zKSVoN8f">Interacting galaxy</a>

Interactions between galaxies are relatively frequent, and they can play an important role in <a href="/facts/Galaxy_formation_and_evolution/uAPtXxr4">galactic evolution</a>. Near misses between galaxies result in warping distortions due to <a href="/facts/Galactic_tide/0X0cJblB">tidal interactions</a>, and may cause some exchange of gas and dust.<a class="footnote-ref" id="fnref:117" href="#fn:117">117</a><a class="footnote-ref" id="fnref:118" href="#fn:118">118</a>
Collisions occur when two galaxies pass directly through each other and have sufficient relative momentum not to merge. The stars of interacting galaxies usually do not collide, but the gas and dust within the two forms interacts, sometimes triggering star formation. A collision can severely distort the galaxies' shapes, forming bars, rings or tail-like structures.<a class="footnote-ref" id="fnref:119" href="#fn:119">119</a><a class="footnote-ref" id="fnref:120" href="#fn:120">120</a>
At the extreme of interactions are galactic mergers, where the galaxies' relative momentums are insufficient to allow them to pass through each other. Instead, they gradually merge to form a single, larger galaxy. Mergers can result in significant changes to the galaxies' original morphology. If one of the galaxies is much more massive than the other, the result is known as <a href="/facts/Interacting_galaxy/zKSVoN8f">cannibalism</a>, where the more massive larger galaxy remains relatively undisturbed, and the smaller one is torn apart. The Milky Way galaxy is currently in the process of cannibalizing the <a href="/facts/Sagittarius_Dwarf_Elliptical_Galaxy/9IfJCbtl">Sagittarius Dwarf Elliptical Galaxy</a> and the <a href="/facts/Canis_Major_Dwarf_Galaxy/uQjxtxef">Canis Major Dwarf Galaxy</a>.<a class="footnote-ref" id="fnref:121" href="#fn:121">121</a><a class="footnote-ref" id="fnref:122" href="#fn:122">122</a>

<h3>Starburst</h3>
Main article: <a href="/facts/Starburst_galaxy/EV0wM4Rs">Starburst galaxy</a>

Stars are created within galaxies from a reserve of cold gas that forms giant <a href="/facts/Molecular_cloud/5jEwCJxs">molecular clouds</a>. Some galaxies have been observed to form stars at an exceptional rate, which is known as a starburst. If they continue to do so, they would consume their reserve of gas in a time span less than the galaxy's lifespan. Hence starburst activity usually lasts only about ten million years, a relatively brief period in a galaxy's history. Starburst galaxies were more common during the universe's early history,<a class="footnote-ref" id="fnref:123" href="#fn:123">123</a> but still contribute an estimated 15% to total star production.<a class="footnote-ref" id="fnref:124" href="#fn:124">124</a>
Starburst galaxies are characterized by dusty concentrations of gas and the appearance of newly formed stars, including massive stars that ionize the surrounding clouds to create <a href="/facts/H_II_region/oDXMyTE1">H II regions</a>.<a class="footnote-ref" id="fnref:125" href="#fn:125">125</a> These stars produce <a href="/facts/Supernova/Pfo2J23l">supernova</a> explosions, creating expanding <a href="/facts/Supernova_remnant/tYboe2n4">remnants</a> that interact powerfully with the surrounding gas. These outbursts trigger a chain reaction of star-building that spreads throughout the gaseous region. Only when the available gas is nearly consumed or dispersed does the activity end.<a class="footnote-ref" id="fnref:126" href="#fn:126">126</a>
Starbursts are often associated with merging or interacting galaxies. The prototype example of such a starburst-forming interaction is <a href="/facts/Messier_82/qDN2z3EI">M82</a>, which experienced a close encounter with the larger <a href="/facts/Messier_81/p91h990c">M81</a>. Irregular galaxies often exhibit spaced knots of starburst activity.<a class="footnote-ref" id="fnref:127" href="#fn:127">127</a>

<h3>Radio galaxy</h3>
Main article: <a href="/facts/Radio_galaxy/mya88npd">Radio galaxy</a>

A <a href="/facts/Radio_galaxy/mya88npd">radio galaxy</a> is a galaxy with giant regions of radio emission extending well beyond its visible structure. These energetic radio lobes are powered by jets from its <a href="/facts/Active_galactic_nucleus/qT1owvXz">active galactic nucleus</a>.<a class="footnote-ref" id="fnref:128" href="#fn:128">128</a> Radio galaxies are classified according to their <a href="/facts/Fanaroff%E2%80%93Riley_classification/rjmFVNvD">Fanaroff–Riley classification</a>. The FR I class have lower radio luminosity and exhibit structures which are more elongated; the FR II class are higher radio luminosity. The correlation of radio luminosity and structure suggests that the sources in these two types of galaxies may differ.<a class="footnote-ref" id="fnref:129" href="#fn:129">129</a>
Radio galaxies can also be classified as giant radio galaxies (GRGs), whose radio emissions can extend to scales of megaparsecs (3.26 million light-years). <a href="/facts/Alcyoneus_(galaxy)/5wg4Aesz">Alcyoneus</a> is an FR II class low-excitation radio galaxy which has the largest observed radio emission, with lobed structures spanning 5 <a href="/facts/Parsec/SwSsk57J">megaparsecs</a> (16×106 <a href="/facts/Light-year/IGc5NdQb">ly</a>). For comparison, another similarly sized giant radio galaxy is <a href="/facts/3C_236/lxpG1IBT">3C 236</a>, with lobes 15 million light-years across. It should however be noted that radio emissions are not always considered part of the main galaxy itself.<a class="footnote-ref" id="fnref:130" href="#fn:130">130</a>
A giant radio galaxy is a special class of objects characterized by the presence of radio lobes generated by <a href="/facts/Astrophysical_jet/QYerB8R3">relativistic jets</a> powered by the central galaxy's <a href="/facts/Supermassive_black_hole/BcuTx8Q5">supermassive black hole</a>. Giant radio galaxies are different from ordinary radio galaxies in that they can extend to much larger scales, reaching upwards to several megaparsecs across, far larger than the diameters of their host galaxies.<a class="footnote-ref" id="fnref:131" href="#fn:131">131</a>
A "normal" radio galaxy do not have a source that is a supermassive black hole or monster neutron star; instead the source is <a href="/facts/Synchrotron_radiation/mTsSKmRz">synchrotron radiation</a> from relativistic electrons accelerated by supernova. These sources are comparatively short lived, making the radio spectrum from normal radio galaxies an especially good way to study star formation.<a class="footnote-ref" id="fnref:132" href="#fn:132">132</a>

<h3>Active galaxy</h3>
Main article: <a href="/facts/Active_galactic_nucleus/qT1owvXz">Active galactic nucleus</a>

Some observable galaxies are classified as "active" if they contain an active galactic nucleus (AGN).<a class="footnote-ref" id="fnref:133" href="#fn:133">133</a> A significant portion of the galaxy's total energy output is emitted by the active nucleus instead of its stars, dust and <a href="/facts/Interstellar_medium/mokU0WEz">interstellar medium</a>. There are multiple classification and naming schemes for AGNs, but those in the lower ranges of luminosity are called <a href="/facts/Seyfert_galaxy/N7T3SleM">Seyfert galaxies</a>, while those with luminosities much greater than that of the host galaxy are known as quasi-stellar objects or <a href="/facts/Quasar/HS96328l">quasars</a>. Models of AGNs suggest that a significant fraction of their light is shifted to far-infrared frequencies because optical and UV emission in the nucleus is absorbed and remitted by dust and gas surrounding it.<a class="footnote-ref" id="fnref:134" href="#fn:134">134</a>
The standard model for an <a href="/facts/Active_galactic_nucleus/qT1owvXz">active galactic nucleus</a> is based on an <a href="/facts/Accretion_disc/8zJXshat">accretion disc</a> that forms around a <a href="/facts/Supermassive_black_hole/BcuTx8Q5">supermassive black hole</a> (SMBH) at the galaxy's core region. The radiation from an active galactic nucleus results from the <a href="/facts/Gravitational_energy/SJpNw6G5">gravitational energy</a> of matter as it falls toward the black hole from the disc.<a class="footnote-ref" id="fnref:135" href="#fn:135">135</a><a class="footnote-ref" id="fnref:136" href="#fn:136">136</a> The AGN's luminosity depends on the SMBH's mass and the rate at which matter falls onto it.
In about 10% of these galaxies, a diametrically opposed pair of <a href="/facts/Astrophysical_jet/QYerB8R3">energetic jets</a> ejects particles from the galaxy core at velocities close to the <a href="/facts/Speed_of_light/sKSQwdNx">speed of light</a>. The mechanism for producing these jets is not well understood.<a class="footnote-ref" id="fnref:137" href="#fn:137">137</a>

<h4>Seyfert galaxy</h4>
Main article: <a href="/facts/Seyfert_galaxy/N7T3SleM">Seyfert galaxy</a>
Seyfert galaxies are one of the two largest groups of active galaxies, along with quasars. They have quasar-like nuclei (very luminous, distant and bright sources of electromagnetic radiation) with very high surface brightnesses; but unlike quasars, their host galaxies are clearly detectable.<a class="footnote-ref" id="fnref:138" href="#fn:138">138</a> Seen through a telescope, a Seyfert galaxy appears like an ordinary galaxy with a bright star superimposed atop the core. Seyfert galaxies are divided into two principal subtypes based on the frequencies observed in their spectra.<a class="footnote-ref" id="fnref:139" href="#fn:139">139</a>

<h4>Quasar</h4>
Main article: <a href="/facts/Quasar/HS96328l">Quasar</a>
Quasars are the most energetic and distant members of active galactic nuclei. Extremely luminous, they were first identified as high redshift sources of electromagnetic energy, including radio waves and visible light, that appeared more similar to stars than to extended sources similar to galaxies. Their luminosity can be 100 times that of the Milky Way.<a class="footnote-ref" id="fnref:140" href="#fn:140">140</a> The nearest known quasar, <a href="/facts/Markarian_231/MS2jytBU">Markarian 231</a>, is about 581 million light-years from Earth,<a class="footnote-ref" id="fnref:141" href="#fn:141">141</a> while others have been discovered as far away as <a href="/facts/UHZ1/2W7somgC">UHZ1</a>, roughly 13.2 billion light-years distant.<a class="footnote-ref" id="fnref:142" href="#fn:142">142</a><a class="footnote-ref" id="fnref:143" href="#fn:143">143</a> Quasars are noteworthy for providing the first demonstration of the phenomenon that <a href="/facts/Gravitational_lens/LmxzvLs8">gravity can act as a lens for light</a>.<a class="footnote-ref" id="fnref:144" href="#fn:144">144</a>

<h4>Other AGNs</h4>
<a href="/facts/Blazar/gtIlQjQ5">Blazars</a> are believed to be active galaxies with a <a href="/facts/Relativistic_jet/QYerB8R3">relativistic jet</a> pointed in the direction of Earth. A <a href="/facts/Radio_galaxy/mya88npd">radio galaxy</a> emits radio frequencies from relativistic jets. A unified model of these types of active galaxies explains their differences based on the observer's position.<a class="footnote-ref" id="fnref:145" href="#fn:145">145</a>
Possibly related to active galactic nuclei (as well as <a href="/facts/Starburst_(astronomy)/wMNJJwQX">starburst</a> regions) are <a href="/facts/Low-ionization_nuclear_emission-line_region/8dSxC8Qw">low-ionization nuclear emission-line regions</a> (LINERs). The emission from LINER-type galaxies is dominated by weakly <a href="/facts/Ion/3bePpDna">ionized</a> elements. The excitation sources for the weakly ionized lines include post-<a href="/facts/Asymptotic_giant_branch/R90sd1Hl">AGB</a> stars, AGN, and shocks.<a class="footnote-ref" id="fnref:146" href="#fn:146">146</a> Approximately one-third of nearby galaxies are classified as containing LINER nuclei.<a class="footnote-ref" id="fnref:147" href="#fn:147">147</a><a class="footnote-ref" id="fnref:148" href="#fn:148">148</a><a class="footnote-ref" id="fnref:149" href="#fn:149">149</a>

<h3>Luminous infrared galaxy</h3>
Main article: <a href="/facts/Luminous_infrared_galaxy/GP6F086N">Luminous infrared galaxy</a>
Luminous infrared galaxies (LIRGs) are galaxies with luminosities—the measurement of electromagnetic power output—above 1011 L☉ (solar luminosities). In most cases, most of their energy comes from large numbers of young stars which heat surrounding dust, which reradiates the energy in the infrared. Luminosity high enough to be a LIRG requires a star formation rate of at least 18 M☉ yr−1. Ultra-luminous infrared galaxies (ULIRGs) are at least ten times more luminous still and form stars at rates >180 M☉ yr−1. Many LIRGs also emit radiation from an AGN.<a class="footnote-ref" id="fnref:150" href="#fn:150">150</a><a class="footnote-ref" id="fnref:151" href="#fn:151">151</a> Infrared galaxies emit more energy in the infrared than all other wavelengths combined, with peak emission typically at wavelengths of 60 to 100 microns. LIRGs are believed to be created from the strong interaction and merger of spiral galaxies.<a class="footnote-ref" id="fnref:152" href="#fn:152">152</a> While uncommon in the local universe, LIRGs and ULIRGS were more prevalent when the universe was younger.<a class="footnote-ref" id="fnref:153" href="#fn:153">153</a>

<h2 id="physical-diameters">Physical diameters</h2>
Galaxies do not have a definite boundary by their nature, and are characterized by a gradually decreasing stellar density as a function of increasing distance from their center, making measurements of their true extents difficult. Nevertheless, astronomers over the past few decades have made several criteria in defining the sizes of galaxies.

<h3>Angular diameter</h3>
As early as the time of <a href="/facts/Edwin_Hubble/fpX3JlbJ">Edwin Hubble</a> in 1936, there have been attempts to characterize the diameters of galaxies. The earliest efforts were based on the observed angle subtended by the galaxy and its estimated distance, leading to an angular diameter (also called "metric diameter").<a class="footnote-ref" id="fnref:154" href="#fn:154">154</a>

<h3>Isophotal diameter</h3>
The isophotal diameter is introduced as a conventional way of measuring a galaxy's size based on its apparent surface brightness.<a class="footnote-ref" id="fnref:155" href="#fn:155">155</a> <a href="/facts/Isophote/WXKCjA8x">Isophotes</a> are curves in a diagram - such as a picture of a galaxy - that adjoins points of equal brightnesses, and are useful in defining the extent of the galaxy. The apparent brightness flux of a galaxy is measured in units of <a href="/facts/Magnitude_(astronomy)/f4FbscJu">magnitudes</a> per square <a href="/facts/Minute_and_second_of_arc/tybs6YGC">arcsecond</a> (mag/arcsec2; sometimes expressed as mag arcsec−2), which defines the brightness depth of the isophote. To illustrate how this unit works, a typical galaxy has a brightness flux of 18 mag/arcsec2 at its central region. This brightness is equivalent to the light of an 18th magnitude hypothetical point object (like a star) being spread out evenly in a one square arcsecond area of the sky.<a class="footnote-ref" id="fnref:156" href="#fn:156">156</a> The isophotal diameter is typically defined as the region enclosing all the light down to 25 mag/arcsec2 in the blue <a href="/facts/Jhk/7tUmLBGR">B-band</a>,<a class="footnote-ref" id="fnref:157" href="#fn:157">157</a> which is then referred to as the D25 standard.<a class="footnote-ref" id="fnref:158" href="#fn:158">158</a>

Examples of isophotal diameters (25.0 B-mag/arcsec2 isophote)<table><tbody><tr><th>galaxy</th><th>diameter</th><th>reference</th></tr><tr><td><a href="/facts/Large_Magellanic_Cloud/7VYAehNa">Large Magellanic Cloud</a></td><td>9.96 <a href="/facts/Parsec/SwSsk57J">kiloparsecs</a> (32,500 <a href="/facts/Light-year/IGc5NdQb">light-years</a>)</td><td><a class="footnote-ref" id="fnref:159" href="#fn:159">159</a></td></tr><tr><td><a href="/facts/Milky_Way/ulF6lccN">Milky Way</a></td><td>26.8 <a href="/facts/Parsec/SwSsk57J">kiloparsecs</a> (87,400 <a href="/facts/Light-year/IGc5NdQb">light-years</a>)</td><td><a class="footnote-ref" id="fnref:160" href="#fn:160">160</a></td></tr><tr><td><a href="/facts/Messier_87/x8Q1M5p4">Messier 87</a></td><td>40.55 <a href="/facts/Parsec/SwSsk57J">kiloparsecs</a> (132,000 <a href="/facts/Light-year/IGc5NdQb">light-years</a>)</td><td><a class="footnote-ref" id="fnref:161" href="#fn:161">161</a></td></tr><tr><td><a href="/facts/Andromeda_Galaxy/MjmSLV6m">Andromeda Galaxy</a></td><td>46.58 <a href="/facts/Parsec/SwSsk57J">kiloparsecs</a> (152,000 <a href="/facts/Light-year/IGc5NdQb">light-years</a>)</td><td><a class="footnote-ref" id="fnref:162" href="#fn:162">162</a></td></tr></tbody></table>
<h3>Effective radius (half-light) and its variations</h3>
The <a href="/facts/Half-light_radius/KngX0Vnm">half-light radius</a> (also known as effective radius; Re) is a measure that is based on the galaxy's overall brightness flux. This is the radius upon which half, or 50%, of the total brightness flux of the galaxy was emitted. This was first proposed by <a href="/facts/G%C3%A9rard_de_Vaucouleurs/4kTxWxAl">Gérard de Vaucouleurs</a> in 1948.<a class="footnote-ref" id="fnref:163" href="#fn:163">163</a> The choice of using 50% was arbitrary, but proved to be useful in further works by R. A. Fish in 1963,<a class="footnote-ref" id="fnref:164" href="#fn:164">164</a> where he established a luminosity concentration law that relates the brightnesses of elliptical galaxies and their respective Re, and by <a href="/facts/Jos%C3%A9_Luis_S%C3%A9rsic/hEF5wQR4">José Luis Sérsic</a> in 1968<a class="footnote-ref" id="fnref:165" href="#fn:165">165</a> that defined a mass-radius relation in galaxies.<a class="footnote-ref" id="fnref:166" href="#fn:166">166</a>
In defining Re, it is necessary that the overall brightness flux galaxy should be captured, with a method employed by Bershady in 2000 suggesting to measure twice the size where the brightness flux of an arbitrarily chosen radius, defined as the local flux, divided by the overall average flux equals to 0.2.<a class="footnote-ref" id="fnref:167" href="#fn:167">167</a> Using half-light radius allows a rough estimate of a galaxy's size, but is not particularly helpful in determining its morphology.<a class="footnote-ref" id="fnref:168" href="#fn:168">168</a>
Variations of this method exist. In particular, in the ESO-Uppsala Catalogue of Galaxies values of 50%, 70%, and 90% of the total blue light (the light detected through a B-band specific filter) had been used to calculate a galaxy's diameter.<a class="footnote-ref" id="fnref:169" href="#fn:169">169</a>

<h3>Petrosian magnitude</h3>
First described by Vahe Petrosian in 1976,<a class="footnote-ref" id="fnref:170" href="#fn:170">170</a> a modified version of this method has been used by the <a href="/facts/Sloan_Digital_Sky_Survey/MSHAk1RU">Sloan Digital Sky Survey</a> (SDSS). This method employs a mathematical model on a galaxy whose radius is determined by the azimuthally (horizontal) averaged profile of its brightness flux. In particular, the SDSS employed the Petrosian magnitude in the R-band (658 nm, in the red part of the visible spectrum) to ensure that the brightness flux of a galaxy would be captured as much as possible while counteracting the effects of background noise. For a galaxy whose brightness profile is exponential, it is expected to capture all of its brightness flux, and 80% for galaxies that follow a profile that follows <a href="/facts/De_Vaucouleurs%27s_law/V0CIxB0D">de Vaucouleurs's law</a>.<a class="footnote-ref" id="fnref:171" href="#fn:171">171</a>
Petrosian magnitudes have the advantage of being redshift and distance independent, allowing the measurement of the galaxy's apparent size since the Petrosian radius is defined in terms of the galaxy's overall luminous flux.<a class="footnote-ref" id="fnref:172" href="#fn:172">172</a>
A critique of an earlier version of this method has been issued by the <a href="/facts/Infrared_Processing_and_Analysis_Center/Vnx2JRt1">Infrared Processing and Analysis Center</a>,<a class="footnote-ref" id="fnref:173" href="#fn:173">173</a> with the method causing a magnitude of error (upwards to 10%) of the values than using isophotal diameter. The use of Petrosian magnitudes also have the disadvantage of missing most of the light outside the Petrosian aperture, which is defined relative to the galaxy's overall brightness profile, especially for elliptical galaxies, with higher signal-to-noise ratios on higher distances and redshifts.<a class="footnote-ref" id="fnref:174" href="#fn:174">174</a> A correction for this method has been issued by Graham et al. in 2005, based on the assumption that galaxies follow <a href="/facts/S%C3%A9rsic_profile/HhbcKxJQ">Sérsic's law</a>.<a class="footnote-ref" id="fnref:175" href="#fn:175">175</a>

<h3>Near-infrared method</h3>
This method has been used by <a href="/facts/2MASS/tKKkAJT0">2MASS</a> as an adaptation from the previously used methods of isophotal measurement. Since 2MASS operates in the near infrared, which has the advantage of being able to recognize dimmer, cooler, and older stars, it has a different form of approach compared to other methods that normally use B-filter. The detail of the method used by 2MASS has been described thoroughly in a document by Jarrett et al., with the survey measuring several parameters.<a class="footnote-ref" id="fnref:176" href="#fn:176">176</a>
The standard aperture ellipse (area of detection) is defined by the infrared isophote at the <a href="/facts/K_band_(infrared)/1MPj6hJ3">Ks band</a> (roughly 2.2 μm wavelength) of 20 mag/arcsec2. Gathering the overall luminous flux of the galaxy has been employed by at least four methods: the first being a circular aperture extending 7 arcseconds from the center, an isophote at 20 mag/arcsec2, a "total" aperture defined by the radial light distribution that covers the supposed extent of the galaxy, and the Kron aperture (defined as 2.5 times the first-moment radius, an integration of the flux of the "total" aperture).<a class="footnote-ref" id="fnref:177" href="#fn:177">177</a>

<h2 id="larger-scale-structures">Larger-scale structures</h2>
Main articles: <a href="/facts/Observable_universe/CdTGMdsp">Observable universe § Large-scale structure</a>, <a href="/facts/Galaxy_filament/MFPWn8pS">Galaxy filament</a>, and <a href="/facts/Galaxy_groups_and_clusters/saKzQDap">Galaxy groups and clusters</a>

Deep-sky surveys show that galaxies are often found in groups and <a href="/facts/Clusters_of_galaxies/CdTGMdsp">clusters</a>. Solitary galaxies that have not significantly interacted with other galaxies of comparable mass in the past few billion years are relatively scarce.<a class="footnote-ref" id="fnref:178" href="#fn:178">178</a> Only about 5% of the galaxies surveyed are isolated in this sense.<a class="footnote-ref" id="fnref:179" href="#fn:179">179</a><a class="footnote-ref" id="fnref:180" href="#fn:180">180</a> However, they may have interacted and even merged with other galaxies in the past,<a class="footnote-ref" id="fnref:181" href="#fn:181">181</a> and may still be orbited by smaller satellite galaxies.<a class="footnote-ref" id="fnref:182" href="#fn:182">182</a>
On the largest scale, the universe is continually expanding, resulting in an average increase in the separation between individual galaxies (see <a href="/facts/Hubble%27s_law/FJYfELCP">Hubble's law</a>). Associations of galaxies can overcome this expansion on a local scale through their mutual gravitational attraction. These associations formed early, as clumps of dark matter pulled their respective galaxies together. Nearby groups later merged to form larger-scale clusters. This ongoing merging process, as well as an influx of infalling gas, heats the intergalactic gas in a cluster to very high temperatures of 30–100 <a href="/facts/Megakelvin/ADXGAk8e">megakelvins</a>.<a class="footnote-ref" id="fnref:183" href="#fn:183">183</a> About 70–80% of a cluster's mass is in the form of dark matter, with 10–30% consisting of this heated gas and the remaining few percent in the form of galaxies.<a class="footnote-ref" id="fnref:184" href="#fn:184">184</a>
Most galaxies are gravitationally bound to a number of other galaxies. These form a <a href="/facts/Fractal/sXj38JeN">fractal</a>-like hierarchical distribution of clustered structures, with the smallest such associations being termed groups. A group of galaxies is the most common type of galactic cluster; these formations contain the majority of galaxies (as well as most of the <a href="/facts/Baryon/QFwAUWK2">baryonic</a> mass) in the universe.<a class="footnote-ref" id="fnref:185" href="#fn:185">185</a><a class="footnote-ref" id="fnref:186" href="#fn:186">186</a> To remain gravitationally bound to such a group, each member galaxy must have a sufficiently low velocity to prevent it from escaping (see <a href="/facts/Virial_theorem/w3qwDrkr">Virial theorem</a>). If there is insufficient <a href="/facts/Kinetic_energy/aJRxUd4p">kinetic energy</a>, however, the group may evolve into a smaller number of galaxies through mergers.<a class="footnote-ref" id="fnref:187" href="#fn:187">187</a>
Clusters of galaxies consist of hundreds to thousands of galaxies bound together by gravity.<a class="footnote-ref" id="fnref:188" href="#fn:188">188</a> Clusters of galaxies are often dominated by a single giant elliptical galaxy, known as the <a href="/facts/Brightest_cluster_galaxy/0n74Vo3W">brightest cluster galaxy</a>, which, over time, <a href="/facts/Tidal_force/GJgxo7gp">tidally</a> destroys its satellite galaxies and adds their mass to its own.<a class="footnote-ref" id="fnref:189" href="#fn:189">189</a>

<a href="/facts/Supercluster/DIBrfG30">Superclusters</a> contain tens of thousands of galaxies, which are found in clusters, groups and sometimes individually. At the <a href="/facts/Large-scale_structure_of_the_Cosmos/CdTGMdsp">supercluster scale</a>, galaxies are arranged into sheets and filaments surrounding vast empty voids.<a class="footnote-ref" id="fnref:190" href="#fn:190">190</a> Above this scale, the universe appears to be the same in all directions (<a href="/facts/Isotropy/mc3QEY2x">isotropic</a> and homogeneous),<a class="footnote-ref" id="fnref:191" href="#fn:191">191</a> though this notion has been challenged in recent years by numerous findings of large-scale structures that appear to be exceeding this scale. The <a href="/facts/Hercules%E2%80%93Corona_Borealis_Great_Wall/kszfcMlc">Hercules–Corona Borealis Great Wall</a>, currently the <a href="/facts/List_of_largest_cosmic_structures/amD8w2ID">largest structure</a> in the universe found so far, is 10 billion <a href="/facts/Light-year/IGc5NdQb">light-years</a> (three gigaparsecs) in length.<a class="footnote-ref" id="fnref:192" href="#fn:192">192</a><a class="footnote-ref" id="fnref:193" href="#fn:193">193</a><a class="footnote-ref" id="fnref:194" href="#fn:194">194</a>
The Milky Way galaxy is a member of an association named the <a href="/facts/Local_Group/kjUefCLr">Local Group</a>, a relatively small group of galaxies that has a diameter of approximately one megaparsec. The Milky Way and the Andromeda Galaxy are the two brightest galaxies within the group; many of the other member galaxies are dwarf companions of these two.<a class="footnote-ref" id="fnref:195" href="#fn:195">195</a> The Local Group itself is a part of a cloud-like structure within the <a href="/facts/Virgo_Supercluster/kUNskKbo">Virgo Supercluster</a>, a large, extended structure of groups and clusters of galaxies centered on the <a href="/facts/Virgo_Cluster/dBsDKTzT">Virgo Cluster</a>.<a class="footnote-ref" id="fnref:196" href="#fn:196">196</a> In turn, the Virgo Supercluster is a portion of the <a href="/facts/Laniakea_Supercluster/pleQ3nUL">Laniakea Supercluster</a>.<a class="footnote-ref" id="fnref:197" href="#fn:197">197</a>

<h2 id="magnetic-fields">Magnetic fields</h2>
Galaxies have <a href="/facts/Magnetic_field/Ta8Ev588">magnetic fields</a> of their own. A galaxy's magnetic field influences its dynamics in multiple ways, including affecting the formation of spiral arms and transporting angular momentum in gas clouds. The latter effect is particularly important, as it is a necessary factor for the gravitational collapse of those clouds, and thus for star formation.<a class="footnote-ref" id="fnref:198" href="#fn:198">198</a>
The typical average <a href="/facts/Equipartition_theorem/EJfmTK6W">equipartition</a> strength for <a href="/facts/Spiral_galaxy/hRT2dtxJ">spiral galaxies</a> is about 10 μG (<a href="/facts/Gauss_(unit)/Nar24Pgc">microgauss</a>) or 1 nT (<a href="/facts/Tesla_(unit)/K6I5Stn9">nanotesla</a>). By comparison, the Earth's magnetic field has an average strength of about 0.3 G (Gauss) or 30 μT (<a href="/facts/Tesla_(unit)/K6I5Stn9">microtesla</a>). Radio-faint galaxies like <a href="/facts/Andromeda_Galaxy/MjmSLV6m">M 31</a> and <a href="/facts/Triangulum_Galaxy/etLCCGhP">M33</a>, the <a href="/facts/Milky_Way/ulF6lccN">Milky Way</a>'s neighbors, have weaker fields (about 5 μG), while gas-rich galaxies with high star-formation rates, like M 51, M 83 and NGC 6946, have 15 μG on average. In prominent spiral arms, the field strength can be up to 25 μG, in regions where cold gas and dust are also concentrated. The strongest total equipartition fields (50–100 μG) were found in <a href="/facts/Starburst_galaxy/EV0wM4Rs">starburst galaxies</a>—for example, in M 82 and the <a href="/facts/Antennae_Galaxies/GRKCY3bc">Antennae</a>; and in nuclear starburst regions, such as the centers of NGC 1097 and other <a href="/facts/Barred_spiral_galaxy/cntSCFX4">barred galaxies</a>.<a class="footnote-ref" id="fnref:199" href="#fn:199">199</a>

<h2 id="formation-and-evolution">Formation and evolution</h2>
Main article: <a href="/facts/Galaxy_formation_and_evolution/uAPtXxr4">Galaxy formation and evolution</a>
<h3>Formation</h3>

Current models of the formation of galaxies in the early universe are based on the <a href="/facts/Lambda-CDM_model/DmlhJHQU">ΛCDM</a> model. About 300,000 years after the <a href="/facts/Big_Bang/I5T1vTnv">Big Bang</a>, atoms of <a href="/facts/Hydrogen/BoYHjl0J">hydrogen</a> and <a href="/facts/Helium/yRul93TG">helium</a> began to form, in an event called <a href="/facts/Recombination_(cosmology)/cUGysC0q">recombination</a>. Nearly all the hydrogen was neutral (non-ionized) and readily absorbed light, and no stars had yet formed. As a result, this period has been called the "<a href="/facts/Timeline_of_the_Big_Bang/ezBKAdjy">dark ages</a>". It was from density fluctuations (or <a href="/facts/Anisotropy/YMqTQWVB">anisotropic</a> irregularities) in this primordial matter that <a href="/facts/Structure_formation/1wnrpsKz">larger structures</a> began to appear. As a result, masses of <a href="/facts/Baryon/QFwAUWK2">baryonic</a> matter started to condense within <a href="/facts/Cold_dark_matter/vL4134Kd">cold dark matter</a> halos.<a class="footnote-ref" id="fnref:200" href="#fn:200">200</a><a class="footnote-ref" id="fnref:201" href="#fn:201">201</a> These primordial structures allowed gasses to condense in to <a href="/facts/Protogalaxies/QvUW6nrC">protogalaxies</a>, large scale gas clouds that were precursors to the first galaxies.<a class="footnote-ref" id="fnref:202" href="#fn:202">202</a>: 6 
As gas falls in to the gravity of the dark matter halos, its pressure and temperature rise. To condense further, the gas must radiate energy. This process was slow in the early universe dominated by hydrogen atoms and molecules which are inefficient radiators compared to heavier elements. As clumps of gas aggregate forming rotating disks, temperatures and pressures continue to increase. Some places within the disk reach high enough density to form stars.

Once protogalaxies began to form and contract, the first <a href="/facts/Halo_star/hRT2dtxJ">halo stars</a>, called <a href="/facts/Population_3_stars/8ur1qDRK">Population III stars</a>, appeared within them.<a class="footnote-ref" id="fnref:203" href="#fn:203">203</a> These were composed of primordial gas, almost entirely of hydrogen and helium.
Emission from the first stars heats the remaining gas helping to trigger additional star formation; the ultraviolet light emission from the first generation of stars re-ionized the surrounding neutral hydrogen in expanding spheres eventually reaching the entire universe, an event called <a href="/facts/Reionization/tfqf1Ny9">reionization</a>.<a class="footnote-ref" id="fnref:204" href="#fn:204">204</a> The most massive stars collapse in violent <a href="/facts/Supernova/Pfo2J23l">supernova</a> explosions releasing heavy elements ("metals") into the <a href="/facts/Interstellar_medium/mokU0WEz">interstellar medium</a>.<a class="footnote-ref" id="fnref:205" href="#fn:205">205</a><a class="footnote-ref" id="fnref:206" href="#fn:206">206</a>: 14  This metal content is incorporated into <a href="/facts/Population_II_stars/8ur1qDRK">population II stars</a>.
Theoretical models for early galaxy formation have been verified and informed by a large number and variety of sophisticated astronomical observations.<a class="footnote-ref" id="fnref:207" href="#fn:207">207</a>: 43  The photometric observations generally need spectroscopic confirmation due the large number mechanisms that can introduce systematic errors. For example, a high redshift (z ~ 16) photometric observation by <a href="/facts/James_Webb_Space_Telescope/w4GAWnWX">James Webb Space Telescope</a> (JWST) was later corrected to be closer to z ~ 5.<a class="footnote-ref" id="fnref:208" href="#fn:208">208</a>
Nevertheless, confirmed observations from the JWST and other observatories are accumulating, allowing systematic comparison of early galaxies to predictions of theory.<a class="footnote-ref" id="fnref:209" href="#fn:209">209</a>
Evidence for individual Population III stars in early galaxies is even more challenging. Even seemingly confirmed spectroscopic evidence may turn out to have other origins. For example, astronomers reported HeII emission evidence for <a href="/facts/Population_3_stars/8ur1qDRK">Population III stars</a> in the <a href="/facts/Cosmos_Redshift_7/pXnbhuuG">Cosmos Redshift 7</a> galaxy, with a redshift value of 6.60.<a class="footnote-ref" id="fnref:210" href="#fn:210">210</a> Subsequent observations<a class="footnote-ref" id="fnref:211" href="#fn:211">211</a> found metallic emission lines, OIII, inconsistent with an early-galaxy star.<a class="footnote-ref" id="fnref:212" href="#fn:212">212</a>: 108

<h3>Evolution</h3>
Once stars begin to form, emit radiation, and in some cases explode, the process of galaxy formation becomes very complex, involving interactions between the forces of gravity, radiation, and thermal energy. Many details are still poorly understood.<a class="footnote-ref" id="fnref:213" href="#fn:213">213</a>
Within a billion years of a galaxy's formation, key structures begin to appear.<a class="footnote-ref" id="fnref:214" href="#fn:214">214</a> <a href="/facts/Globular_cluster/FL0EERJU">Globular clusters</a>, the central <a href="/facts/Supermassive_black_hole/BcuTx8Q5">supermassive black hole</a>, and a <a href="/facts/Bulge_(astronomy)/cjJ0LFan">galactic bulge</a> of metal-poor <a href="/facts/Metallicity/nhhPqbYF">Population II stars</a> form. The creation of a supermassive black hole appears to play a key role in actively regulating the growth of galaxies by limiting the total amount of additional matter added.<a class="footnote-ref" id="fnref:215" href="#fn:215">215</a> During this early epoch, galaxies undergo a major burst of star formation.<a class="footnote-ref" id="fnref:216" href="#fn:216">216</a>
During the following two billion years, the accumulated matter settles into a <a href="/facts/Disc_(galaxy)/D7GeqnFf">galactic disc</a>.<a class="footnote-ref" id="fnref:217" href="#fn:217">217</a> A galaxy will continue to absorb infalling material from <a href="/facts/High-velocity_cloud/jgaJ2kwd">high-velocity clouds</a> and <a href="/facts/Dwarf_galaxy/TKS7W9tA">dwarf galaxies</a> throughout its life.<a class="footnote-ref" id="fnref:218" href="#fn:218">218</a> This matter is mostly hydrogen and helium. The cycle of stellar birth and death slowly increases the abundance of heavy elements, eventually allowing the <a href="/facts/Planetary_formation/IT3D6MpE">formation</a> of <a href="/facts/Planet/rbPjE6Bx">planets</a>.<a class="footnote-ref" id="fnref:219" href="#fn:219">219</a>

Star formation rates in galaxies depend upon their local environment. Isolated 'void' galaxies have highest rate per stellar mass, with 'field' galaxies associated with spiral galaxies having lower rates and galaxies in dense cluster having the lowest rates.<a class="footnote-ref" id="fnref:220" href="#fn:220">220</a>
The evolution of galaxies can be significantly affected by interactions and collisions. Mergers of galaxies were common during the early epoch, and the majority of galaxies were peculiar in morphology.<a class="footnote-ref" id="fnref:221" href="#fn:221">221</a> Given the distances between the stars, the great majority of stellar systems in colliding galaxies will be unaffected. However, gravitational stripping of the interstellar gas and dust that makes up the spiral arms produces a long train of stars known as tidal tails. Examples of these formations can be seen in <a href="/facts/NGC_4676/Dnngcdks">NGC 4676</a><a class="footnote-ref" id="fnref:222" href="#fn:222">222</a> or the <a href="/facts/Antennae_Galaxies/GRKCY3bc">Antennae Galaxies</a>.<a class="footnote-ref" id="fnref:223" href="#fn:223">223</a>
The Milky Way galaxy and the nearby Andromeda Galaxy are moving toward each other at about 130 <a href="/facts/Metre_per_second/hSEkho3J">km/s</a>, and—depending upon the lateral movements—the two might collide in about five to six billion years. Although the Milky Way has never collided with a galaxy as large as Andromeda before, it has collided and merged with other galaxies in the past.<a class="footnote-ref" id="fnref:224" href="#fn:224">224</a> Cosmological simulations indicate that, 11 billion years ago, it merged with a particularly large galaxy that has been labeled the <a href="/facts/Kraken_galaxy/qBRh99kB">Kraken</a>.<a class="footnote-ref" id="fnref:225" href="#fn:225">225</a><a class="footnote-ref" id="fnref:226" href="#fn:226">226</a>
Such large-scale interactions are rare. As time passes, mergers of two systems of equal size become less common. Most bright galaxies have remained fundamentally unchanged for the last few billion years, and the net rate of star formation probably also peaked about ten billion years ago.<a class="footnote-ref" id="fnref:227" href="#fn:227">227</a>

<h3>Future trends</h3>
Main article: <a href="/facts/Future_of_an_expanding_universe/ySer1Ltq">Future of an expanding universe</a>
Spiral galaxies, like the <a href="/facts/Milky_Way/ulF6lccN">Milky Way</a>, produce new generations of stars as long as they have dense <a href="/facts/Molecular_cloud/5jEwCJxs">molecular clouds</a> of interstellar hydrogen in their spiral arms.<a class="footnote-ref" id="fnref:228" href="#fn:228">228</a> Elliptical galaxies are largely devoid of this gas, and so form few new stars.<a class="footnote-ref" id="fnref:229" href="#fn:229">229</a> The supply of star-forming material is finite; once stars have converted the available supply of hydrogen into heavier elements, new star formation will come to an end.<a class="footnote-ref" id="fnref:230" href="#fn:230">230</a><a class="footnote-ref" id="fnref:231" href="#fn:231">231</a>
The current era of star formation is expected to continue for up to one hundred billion years, and then the "stellar age" will wind down after about ten trillion to one hundred trillion years (1013–1014 years), as the smallest, longest-lived stars in the visible universe, tiny <a href="/facts/Red_dwarf/56CMQcF0">red dwarfs</a>, begin to fade. At the end of the stellar age, galaxies will be composed of <a href="/facts/Compact_star/AVByG6nR">compact objects</a>: <a href="/facts/Brown_dwarf/fa7kr9lH">brown dwarfs</a>, <a href="/facts/White_dwarf/gIYlTtrC">white dwarfs</a> that are cooling or cold ("<a href="/facts/Black_dwarf/oaMHrFSb">black dwarfs</a>"), <a href="/facts/Neutron_star/4enfoxBA">neutron stars</a>, and <a href="/facts/Black_hole/1r2lmkcF">black holes</a>. Eventually, as a result of <a href="/facts/Relaxation_(physics)/IhdVkDQ4">gravitational relaxation</a>, all stars will either fall into central supermassive black holes or be flung into intergalactic space as a result of collisions.<a class="footnote-ref" id="fnref:232" href="#fn:232">232</a><a class="footnote-ref" id="fnref:233" href="#fn:233">233</a>

<h2 id="gallery">Gallery</h2>

<h2 id="see-also">See also</h2>
<ul>
<li>solar system portal</li><li>outer space portal</li><li>astronomy portal</li><li>stars portal</li></ul>

<ul><li><a href="/facts/Bright_early_galaxies/w4GAWnWX">Bright early galaxies</a></li>
<li><a href="/facts/Dark_galaxy/Ja0gWgLT">Dark galaxy</a></li>
<li><a href="/facts/Galactic_orientation/WPDTAuHw">Galactic orientation</a></li>
<li><a href="/facts/Galaxy_formation_and_evolution/uAPtXxr4">Galaxy formation and evolution</a></li>
<li><a href="/facts/Illustris_project/6QbkyNgt">Illustris project</a></li>
<li><a href="/facts/List_of_galaxies/9PJtf6ld">List of galaxies</a></li>
<li><a href="/facts/List_of_the_most_distant_astronomical_objects/xutYjJn3">List of the most distant astronomical objects</a></li>
<li><a href="/facts/List_of_nearest_galaxies/Egc6SFls">List of nearest galaxies</a></li>
<li><a href="/facts/List_of_largest_galaxies/9PJtf6ld">List of largest galaxies</a></li>
<li><a href="/facts/Low_surface_brightness_galaxy/6bE09r46">Low surface brightness galaxy</a></li>
<li><a href="/facts/Outline_of_galaxies/FbRgtF2E">Outline of galaxies</a></li>
<li><a href="/facts/Timeline_of_knowledge_about_galaxies,_clusters_of_galaxies,_and_large-scale_structure/2Qq2TTed">Timeline of knowledge about galaxies, clusters of galaxies, and large-scale structure</a></li></ul>

<h2 id="notes">Notes</h2>

<h2 id="bibliography">Bibliography</h2>

<ul><li>Belkora, Leila (2003). <a href="https://books.google.com/books?id=cTdsuAEACAAJ">Minding the Heavens: the Story of our Discovery of the Milky Way</a>. <a href="/facts/CRC_Press/duTuH4hz">CRC Press</a>. <a href="/facts/ISBN_(identifier)/15AdSPa9">ISBN</a> 978-0-7503-0730-7. <a href="https://web.archive.org/web/20210324072023/https://books.google.com/books?id=cTdsuAEACAAJ">Archived</a> from the original on March 24, 2021. Retrieved July 25, 2018.</li>
<li><a href="/facts/Giuseppe_Bertin/2NBvgRP5">Bertin, Giuseppe</a>; <a href="/facts/Chia-Chiao_Lin/JQQmHdXY">Lin, Chia-Chiao</a> (1996). <a href="https://books.google.com/books?id=06yfwrdpTk4C">Spiral Structure in Galaxies: a Density Wave Theory</a>. <a href="/facts/MIT_Press/eTerUM3c">MIT Press</a>. <a href="/facts/ISBN_(identifier)/15AdSPa9">ISBN</a> 978-0-262-02396-2. <a href="https://web.archive.org/web/20210324074538/https://books.google.com/books?id=06yfwrdpTk4C">Archived</a> from the original on March 24, 2021. Retrieved July 25, 2018.</li>
<li><a href="/facts/James_Binney/D0nodWhv">Binney, James</a>; Merrifield, Michael (1998). <a href="https://books.google.com/books?id=0CKLswEACAAJ">Galactic Astronomy</a>. Princeton University Press. <a href="/facts/ISBN_(identifier)/15AdSPa9">ISBN</a> 978-0-691-00402-0. <a href="/facts/OCLC_(identifier)/Yqad8waq">OCLC</a> <a href="https://search.worldcat.org/oclc/39108765">39108765</a>. <a href="https://web.archive.org/web/20210324072040/https://books.google.com/books?id=0CKLswEACAAJ">Archived</a> from the original on March 24, 2021. Retrieved July 25, 2018.</li>
<li>Dickinson, Terence (2004). The Universe and Beyond (4th ed.). Firefly Books. <a href="/facts/ISBN_(identifier)/15AdSPa9">ISBN</a> 978-1-55297-901-3. <a href="/facts/OCLC_(identifier)/Yqad8waq">OCLC</a> <a href="https://search.worldcat.org/oclc/55596414">55596414</a>.</li>
<li><a href="/facts/Andrew_Fraknoi/asPtklNX">Fraknoi, Andrew</a>; et al. (2023). <a href="https://openstax.org/details/books/astronomy-2e">Astronomy 2e</a>. <a href="/facts/OpenStax/WKeVahLR">OpenStax</a>. <a href="/facts/ISBN_(identifier)/15AdSPa9">ISBN</a> 978-1-951693-50-3.</li>
<li>Heidarzadeh, Tofigh (2008). <a href="https://books.google.com/books?id=acraAAAAMAAJ">A History of Physical Theories of Comets, from Aristotle to Whipple</a>. Springer. <a href="/facts/ISBN_(identifier)/15AdSPa9">ISBN</a> 978-1-4020-8322-8. <a href="https://web.archive.org/web/20210324072049/https://books.google.com/books?id=acraAAAAMAAJ">Archived</a> from the original on March 24, 2021. Retrieved July 25, 2018.</li>
<li>Mo, Houjun; van den Bosch, Frank; <a href="/facts/Simon_White/vs1GKLlI">White, Simon</a> (2010). <a href="https://books.google.com/books?id=Zj7fDU3Z4wsC">Galaxy Formation and Evolution</a>. <a href="/facts/Cambridge_University_Press/fgEBSSRq">Cambridge University Press</a>. <a href="/facts/ISBN_(identifier)/15AdSPa9">ISBN</a> 978-0-521-85793-2. <a href="https://web.archive.org/web/20210324072050/https://books.google.com/books?id=Zj7fDU3Z4wsC">Archived</a> from the original on March 24, 2021. Retrieved July 25, 2018.</li>
<li>Kepple, George R.; Sanner, Glen W. (1998). <a href="https://books.google.com/books?id=aCocRAAACAAJ">The Night Sky Observer's Guide, Volume 1</a>. Willmann-Bell. <a href="/facts/ISBN_(identifier)/15AdSPa9">ISBN</a> 978-0-943396-58-3. <a href="https://web.archive.org/web/20210324072055/https://books.google.com/books?id=aCocRAAACAAJ">Archived</a> from the original on March 24, 2021. Retrieved July 25, 2018.</li>
<li><a href="/facts/Malcolm_Longair/ybx6HuPj">Longair, Malcolm S.</a> (2008). <a href="https://link.springer.com/book/10.1007/978-3-540-73478-9">Galaxy Formation</a>. Astronomy and Astrophysics Library (2nd ed.). Berlin: <a href="/facts/Springer_Science%2BBusiness_Media/nAesf6nT">Springer</a>. <a href="/facts/Doi_(identifier)/muM9Etpq">doi</a>:<a href="https://doi.org/10.1007%2F978-3-540-73478-9">10.1007/978-3-540-73478-9</a>. <a href="/facts/ISBN_(identifier)/15AdSPa9">ISBN</a> 978-3-540-73477-2.</li>
<li><a href="/facts/David_Merritt/NdPIrkcc">Merritt, David R.</a> (2013). <a href="https://books.google.com/books?id=cOa1ku640zAC">Dynamics and Evolution of Galactic Nuclei</a>. <a href="/facts/Princeton_University_Press/kwvFlKEj">Princeton University Press</a>. <a href="/facts/ISBN_(identifier)/15AdSPa9">ISBN</a> 978-1-4008-4612-2. <a href="https://web.archive.org/web/20210324074542/https://books.google.com/books?id=cOa1ku640zAC">Archived</a> from the original on March 24, 2021. Retrieved July 25, 2018.</li>
<li>Mohamed, Mohaini (2000). <a href="https://books.google.com/books?id=8uEFaPCpAdgC">Great Muslim Mathematicians</a>. Penerbit UTM. <a href="/facts/ISBN_(identifier)/15AdSPa9">ISBN</a> 978-983-52-0157-8. <a href="/facts/OCLC_(identifier)/Yqad8waq">OCLC</a> <a href="https://search.worldcat.org/oclc/48759017">48759017</a>. <a href="https://web.archive.org/web/20210324072117/https://books.google.com/books?id=8uEFaPCpAdgC">Archived</a> from the original on March 24, 2021. Retrieved July 25, 2018.</li>
<li>Paul, Erich R. (1993). <a href="https://books.google.com/books?id=A7PA9EsFB84C">The Milky Way Galaxy and Statistical Cosmology, 1890–1924</a>. <a href="/facts/Cambridge_University_Press/fgEBSSRq">Cambridge University Press</a>. <a href="/facts/ISBN_(identifier)/15AdSPa9">ISBN</a> 978-0-521-35363-2. <a href="https://web.archive.org/web/20210324072121/https://books.google.com/books?id=A7PA9EsFB84C">Archived</a> from the original on March 24, 2021. Retrieved July 25, 2018.</li>
<li><a href="/facts/Allan_Sandage/Qk1kRoTm">Sandage, Allan R.</a>; Kron, Richard G.; <a href="/facts/Malcolm_Longair/ybx6HuPj">Longair, Malcolm S.</a> (1995). <a href="https://books.google.com/books?id=I8zkMgEACAAJ">The Deep Universe</a>. Saas-Fee Advanced Course, Swiss Society for Astrophysics and Astronomy. Vol. 23. <a href="/facts/Springer-Verlag/nAesf6nT">Springer-Verlag</a>. <a href="/facts/ISBN_(identifier)/15AdSPa9">ISBN</a> 978-3-54-058913-6.</li>
<li><a href="/facts/Linda_Sparke/wLhz4yYs">Sparke, Linda S.</a>; Gallagher, John S. (2000). <a href="https://books.google.com/books?id=tzNF79roUfoC">Galaxies in the Universe: An Introduction</a>. <a href="/facts/Cambridge_University_Press/fgEBSSRq">Cambridge University Press</a>. <a href="/facts/ISBN_(identifier)/15AdSPa9">ISBN</a> 978-0-521-59740-1. <a href="https://web.archive.org/web/20210324072126/https://books.google.com/books?id=tzNF79roUfoC">Archived</a> from the original on March 24, 2021. Retrieved July 25, 2018.</li>
<li><a href="/facts/Sidney_Van_den_Bergh/0CLKXmG9">Van den Bergh, Sidney</a> (1998). <a href="https://books.google.com/books?id=geEVkpueEPcC">Galaxy Morphology and Classification</a>. Cambridge University Press. <a href="/facts/ISBN_(identifier)/15AdSPa9">ISBN</a> 978-0-521-62335-3. <a href="https://web.archive.org/web/20210324072137/https://books.google.com/books?id=geEVkpueEPcC">Archived</a> from the original on March 24, 2021. Retrieved July 25, 2018.</li>
<li>Waller, William H.; <a href="/facts/Paul_W._Hodge/PlwP3xaz">Hodge, Paul W.</a> (2003). <a href="https://archive.org/details/galaxiescosmicfr0000wall">Galaxies and the Cosmic Frontier</a>. <a href="/facts/Harvard_University_Press/YluAnq74">Harvard University Press</a>. <a href="/facts/ISBN_(identifier)/15AdSPa9">ISBN</a> 978-0-674-01079-6.</li>
<li><a href="/facts/Thomas_Wright_(astronomer)/zlfrX17L">Wright, Thomas</a> (1750). <a href="https://web.archive.org/web/20210430062726/https://books.google.com/books?id=80VZAAAAcAAJ&source=gbs_navlinks_s">An Original Theory or New Hypothesis of the Universe</a>. London: Chapelle. Archived from <a href="https://books.google.com/books?id=80VZAAAAcAAJ">the original</a> on April 30, 2021. Retrieved April 21, 2024. ... the stars are not infinitely dispersed and distributed in a promiscuous manner throughout all the mundane space, without order or design, ... this phænomenon [is] no other than a certain effect arising from the observer's situation, ... To a spectator placed in an indefinite space, ... it [i.e., the Milky Way (Via Lactea)] [is] a vast ring of stars ...</li></ul>

<h2 id="external-links">External links</h2>

<ul><li><a href="https://ned.ipac.caltech.edu">NASA/IPAC Extragalactic Database (NED)</a></li>
<li><a href="http://ned.ipac.caltech.edu/Library/Distances/">NED Redshift-Independent Distances</a></li>
<li><a href="https://www.bbc.co.uk/programmes/p003c1cn">Galaxies</a> on <a href="/facts/In_Our_Time_(radio_series)/UuCUdLfM">In Our Time</a> at the <a href="/facts/BBC/qFateIz8">BBC</a></li>
<li><a href="https://web.archive.org/web/20150718054637/http://www.atlasoftheuniverse.com/">An Atlas of The Universe</a></li>
<li><a href="https://web.archive.org/web/20150912191650/http://www.nightskyinfo.com/galaxies/">Galaxies – Information and amateur observations</a></li>
<li><a href="http://www.galaxyzoo.org/">Galaxy Zoo – citizen science galaxy classification project</a></li>
<li><a href="https://www.youtube.com/watch?v=08LBltePDZw">"A Flight Through the Universe, by the Sloan Digital Sky Survey" – animated video from Berkeley Lab</a></li></ul>

<h2 id="references">References</h2>

<ol>
<li id="fn:1">Sparke & Gallagher 2000, p. i - Sparke, Linda S.; Gallagher, John S. (2000). Galaxies in the Universe: An Introduction. Cambridge University Press. ISBN 978-0-521-59740-1. Archived from the original on March 24, 2021. Retrieved July 25, 2018. <a href="https://books.google.com/books?id=tzNF79roUfoC" target="_blank">https://books.google.com/books?id=tzNF79roUfoC</a> <a href="#fnref:1" class="footnote-back-ref">↩</a></li>
<li id="fn:2">Hupp, Erica; Roy, Steve; Watzke, Megan (August 12, 2006). "NASA Finds Direct Proof of Dark Matter". NASA. Archived from the original on March 28, 2020. Retrieved April 17, 2007. <a href="https://web.archive.org/web/20200328193824/https://www.nasa.gov/home/hqnews/2006/aug/HQ_06297_CHANDRA_Dark_Matter.html" target="_blank">https://web.archive.org/web/20200328193824/https://www.nasa.gov/home/hqnews/2006/aug/HQ_06297_CHANDRA_Dark_Matter.html</a> <a href="#fnref:2" class="footnote-back-ref">↩</a></li>
<li id="fn:3">Howell, Elizabeth; Harvey, Ailsa (February 11, 2022). "How many stars are in the universe? - Can we estimate the total number of stars?". Space.com. Retrieved July 16, 2022. <a href="https://www.space.com/26078-how-many-stars-are-there.html" target="_blank">https://www.space.com/26078-how-many-stars-are-there.html</a> <a href="#fnref:3" class="footnote-back-ref">↩</a></li>
<li id="fn:4">Strigari, Louis E.; Bullock, James S.; Kaplinghat, Manoj; Simon, Joshua D.; Geha, Marla; Willman, Beth; Walker, Matthew G. (2008). "A common mass scale for satellite galaxies of the Milky Way". Nature. 454 (7208): 1096–1097. arXiv:0808.3772. Bibcode:2008Natur.454.1096S. doi:10.1038/nature07222. ISSN 0028-0836. PMID 18756252. <a href="/wiki/Marla_Geha" target="_blank">/wiki/Marla_Geha</a> <a href="#fnref:4" class="footnote-back-ref">↩</a></li>
<li id="fn:5">Hoover, Aaron (June 16, 2003). "UF Astronomers: Universe Slightly Simpler Than Expected" (Press release). University of Florida. Archived from the original on July 20, 2011. Retrieved March 4, 2011.
Based on: Graham, Alister W.; Guzmán, Rafael (2003). "HST Photometry of Dwarf Elliptical Galaxies in Coma, and an Explanation for the Alleged Structural Dichotomy between Dwarf and Bright Elliptical Galaxies". The Astronomical Journal. 125 (6): 2936–2950. arXiv:astro-ph/0303391. Bibcode:2003AJ....125.2936G. doi:10.1086/374992. S2CID 13284968.
 <a href="https://web.archive.org/web/20110720083835/http://news.ufl.edu/2003/06/16/galaxies/" target="_blank">https://web.archive.org/web/20110720083835/http://news.ufl.edu/2003/06/16/galaxies/</a> <a href="#fnref:5" class="footnote-back-ref">↩</a></li>
<li id="fn:6">Jarrett, T. H. "Near-Infrared Galaxy Morphology Atlas". Infrared Processing and Analysis Center. California Institute of Technology. Archived from the original on November 20, 2023. Retrieved January 9, 2007. <a href="http://www.ipac.caltech.edu/2mass/gallery/galmorph/" target="_blank">http://www.ipac.caltech.edu/2mass/gallery/galmorph/</a> <a href="#fnref:6" class="footnote-back-ref">↩</a></li>
<li id="fn:7">Chemla, Sarah (January 14, 2021). "Astronomers were wrong about the number of galaxies in universe". The Jerusalem Post. Archived from the original on January 14, 2021. Retrieved January 14, 2021. <a href="https://www.jpost.com/health-science/astronomers-were-wrong-about-the-number-of-galaxies-in-universe-655425" target="_blank">https://www.jpost.com/health-science/astronomers-were-wrong-about-the-number-of-galaxies-in-universe-655425</a> <a href="#fnref:7" class="footnote-back-ref">↩</a></li>
<li id="fn:8">Saunders, Toby (July 25, 2023). "How many galaxies are in the Universe? A lot more than you'd think". BBC Science Focus. Retrieved January 9, 2024. <a href="https://www.sciencefocus.com/space/how-many-galaxies-are-in-the-universe" target="_blank">https://www.sciencefocus.com/space/how-many-galaxies-are-in-the-universe</a> <a href="#fnref:8" class="footnote-back-ref">↩</a></li>
<li id="fn:9">Goodwin, Simon P.; Gribbin, John; Hendry, Martin A. (1998). "The relative size of the Milky Way" (PDF). The Observatory. 118: 201–208. Bibcode:1998Obs...118..201G. <a href="/wiki/John_Gribbin" target="_blank">/wiki/John_Gribbin</a> <a href="#fnref:9" class="footnote-back-ref">↩</a></li>
<li id="fn:10">This is the diameter measured using the D25 standard. A 2018 study suggested that there is a presence of disk stars beyond this diameter, although it is not clear how much of this influences the surface brightness profile.[10][11] <a href="#fnref:10" class="footnote-back-ref">↩</a></li>
<li id="fn:11">Riess, Adam G.; Fliri, Jürgen; Valls-Gabaud, David (2012). "Cepheid Period-Luminosity Relations in the Near-Infrared and the Distance to M31 from the Hubble Space Telescope Wide Field Camera 3". The Astrophysical Journal. 745 (2): 156. arXiv:1110.3769. Bibcode:2012ApJ...745..156R. doi:10.1088/0004-637X/745/2/156. S2CID 119113794. <a href="/wiki/Adam_Riess" target="_blank">/wiki/Adam_Riess</a> <a href="#fnref:11" class="footnote-back-ref">↩</a></li>
<li id="fn:12">"Galaxy Clusters and Large-Scale Structure". University of Cambridge. Archived from the original on April 26, 2012. Retrieved January 15, 2007. <a href="https://web.archive.org/web/20120426215141/http://www.damtp.cam.ac.uk/research/gr/public/gal_lss.html" target="_blank">https://web.archive.org/web/20120426215141/http://www.damtp.cam.ac.uk/research/gr/public/gal_lss.html</a> <a href="#fnref:12" class="footnote-back-ref">↩</a></li>
<li id="fn:13">Gibney, Elizabeth (2014). "Earth's new address: 'Solar System, Milky Way, Laniakea'". Nature. doi:10.1038/nature.2014.15819. S2CID 124323774. <a href="/wiki/Elizabeth_Gibney" target="_blank">/wiki/Elizabeth_Gibney</a> <a href="#fnref:13" class="footnote-back-ref">↩</a></li>
<li id="fn:14">Onions, Charles T.; Friedrichsen, G.W.S.; Burchfield, Robert W., eds. (1966). The Oxford Dictionary of English Etymology. Oxford: Clarendon Press. p. 385. <a href="/wiki/Charles_Talbut_Onions" target="_blank">/wiki/Charles_Talbut_Onions</a> <a href="#fnref:14" class="footnote-back-ref">↩</a></li>
<li id="fn:15">Harper, Douglas. "galaxy". Online Etymology Dictionary. Archived from the original on November 17, 2011. Retrieved November 11, 2011. <a href="http://www.etymonline.com/index.php?term=galaxy" target="_blank">http://www.etymonline.com/index.php?term=galaxy</a> <a href="#fnref:15" class="footnote-back-ref">↩</a></li>
<li id="fn:16">Waller & Hodge 2003, p. 91 - Waller, William H.; Hodge, Paul W. (2003). Galaxies and the Cosmic Frontier. Harvard University Press. ISBN 978-0-674-01079-6. <a href="https://archive.org/details/galaxiescosmicfr0000wall" target="_blank">https://archive.org/details/galaxiescosmicfr0000wall</a> <a href="#fnref:16" class="footnote-back-ref">↩</a></li>
<li id="fn:17">Konečný, Lubomír. "Emblematics, Agriculture, and Mythography in The Origin of the Milky Way" (PDF). Academy of Sciences of the Czech Republic. Archived from the original (PDF) on July 20, 2006. Retrieved January 5, 2007. <a href="https://web.archive.org/web/20060720204104/http://www.udu.cas.cz/collegium/tintoretto.pdf" target="_blank">https://web.archive.org/web/20060720204104/http://www.udu.cas.cz/collegium/tintoretto.pdf</a> <a href="#fnref:17" class="footnote-back-ref">↩</a></li>
<li id="fn:18">Bartusiak, M. (2010). The Day We Found the Universe. United States: Knopf Doubleday Publishing Group. <a href="#fnref:18" class="footnote-back-ref">↩</a></li>
<li id="fn:19">"Results for object MESSIER 109 (M109)". NASA/IPAC Extragalactic Database. California Institute of Technology. Retrieved January 13, 2023. <a href="https://ned.ipac.caltech.edu/byname?objname=M109&hconst=67.8&omegam=0.308&omegav=0.692&wmap=4&corr_z=1" target="_blank">https://ned.ipac.caltech.edu/byname?objname=M109&hconst=67.8&omegam=0.308&omegav=0.692&wmap=4&corr_z=1</a> <a href="#fnref:19" class="footnote-back-ref">↩</a></li>
<li id="fn:20">"What is the Sloan Digital Sky Survey?". Sloan Digital Sky Survey. Archived from the original on January 12, 2024. Retrieved March 3, 2024. <a href="https://web.archive.org/web/20240112203017/https://skyserver.sdss.org/dr7/en/sdss/" target="_blank">https://web.archive.org/web/20240112203017/https://skyserver.sdss.org/dr7/en/sdss/</a> <a href="#fnref:20" class="footnote-back-ref">↩</a></li>
<li id="fn:21">Plutarch (2006). The Complete Works Volume 3: Essays and Miscellanies. Echo Library. p. 66. ISBN 978-1-4068-3224-2. Archived from the original on March 24, 2021. Retrieved July 25, 2018. <a href="978-1-4068-3224-2" target="_blank">978-1-4068-3224-2</a> <a href="#fnref:21" class="footnote-back-ref">↩</a></li>
<li id="fn:22">Montada, Josep Puig (September 28, 2007). "Ibn Bâjja". Stanford Encyclopedia of Philosophy. Archived from the original on March 16, 2020. Retrieved July 11, 2008. <a href="http://plato.stanford.edu/entries/ibn-bajja" target="_blank">http://plato.stanford.edu/entries/ibn-bajja</a> <a href="#fnref:22" class="footnote-back-ref">↩</a></li>
<li id="fn:23">Heidarzadeh 2008, pp. 23–25 - Heidarzadeh, Tofigh (2008). A History of Physical Theories of Comets, from Aristotle to Whipple. Springer. ISBN 978-1-4020-8322-8. Archived from the original on March 24, 2021. Retrieved July 25, 2018. <a href="https://books.google.com/books?id=acraAAAAMAAJ" target="_blank">https://books.google.com/books?id=acraAAAAMAAJ</a> <a href="#fnref:23" class="footnote-back-ref">↩</a></li>
<li id="fn:24">Mohamed 2000, pp. 49–50 - Mohamed, Mohaini (2000). Great Muslim Mathematicians. Penerbit UTM. ISBN 978-983-52-0157-8. OCLC 48759017. Archived from the original on March 24, 2021. Retrieved July 25, 2018. <a href="https://books.google.com/books?id=8uEFaPCpAdgC" target="_blank">https://books.google.com/books?id=8uEFaPCpAdgC</a> <a href="#fnref:24" class="footnote-back-ref">↩</a></li>
<li id="fn:25">Bouali, Hamid-Eddine; Zghal, Mourad; Lakhdar, Zohra B. (2005). "Popularisation of optical phenomena: Establishing the first Ibn Al-Haytham workshop on photography" (PDF). In Flory, François (ed.). Ninth International Topical Meeting on Education and Training in Optics and Photonics. Proceedings of SPIE. Vol. 9664, Ninth International Topical Meeting on Education and Training in Optics and Photonics. Bibcode:2005SPIE.9664E..22B. doi:10.1117/12.2207764. <a href="http://spie.org/etop/ETOP2005_080.pdf" target="_blank">http://spie.org/etop/ETOP2005_080.pdf</a> <a href="#fnref:25" class="footnote-back-ref">↩</a></li>
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<li id="fn:33">Wright called the Milky Way the Vortex Magnus (Great Whirlpool) and estimated its diameter to be 8.64×1012 miles (13.9×1012 km).[32] <a href="#fnref:33" class="footnote-back-ref">↩</a></li>
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</ol>

Galaxy open-in-new

Galaxy