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==Cosmology== ===Large-scale dynamics=== Since the late 1980s it has been apparent that not only the [[Local Group]], but all matter out to a distance of at least 50 [[Parsec|Mpc]] is experiencing a bulk flow on the order of 600 km/s in the direction of the [[Norma Cluster| Norma Cluster (Abell 3627)]].<ref name="plionis91"> {{cite journal | author = Plionis, Manolis | author2 = Valdarnini, Riccardo | title = Evidence for large-scale structure on scales about 300/h MPC | journal = Monthly Notices of the Royal Astronomical Society | date = March 1991 | volume = 249 | pages = 46β61 | bibcode = 1991MNRAS.249...46P | doi =10.1093/mnras/249.1.46 | doi-access = free }}</ref> Lynden-Bell et al. (1988) dubbed the cause of this the "[[Great Attractor]]". The Great Attractor is now understood to be the center of mass of an even larger structure of galaxy clusters, dubbed "[[Laniakea Supercluster|Laniakea]]", which includes the Virgo Supercluster (including the Local Group) as well as the Hydra-Centaurus Supercluster, the Pavo-Indus Supercluster, and the Fornax Group. The Great Attractor, together with the entire supercluster, is found to be moving toward [[Shapley Supercluster]], with center of [[Shapley Attractor]].<ref>{{Cite web|url=http://www.universetoday.com/113150/what-is-the-great-attractor/|title = What is the Great Attractor?|date = 14 July 2014}}</ref> ===Dark matter=== The LS has a total mass ''M'' β 10<sup>15</sup> {{solar mass|link=yes}} and a total optical luminosity ''L'' β 3{{e|12}} {{solar luminosity|link=yes}}.<ref name="ein07" /> This yields a [[mass-to-light ratio]] of about 300 times that of the solar ratio ({{solar mass}}/{{solar luminosity}} = 1), a figure that is consistent with results obtained for other superclusters.<ref name="todd98"> {{cite journal | author = Small, Todd A. | display-authors = etal | title = The Norris Survey of the Corona Borealis Supercluster. III. Structure and Mass of the Supercluster | journal = Astrophysical Journal | date = Jan 1998 | volume = 492 | issue = 1| pages = 45β56 | bibcode = 1998ApJ...492...45S | doi = 10.1086/305037 | arxiv = astro-ph/9708153 | s2cid = 119451873 }}</ref><ref name="heymans08"> {{cite journal | author = Heymans, Catherine | display-authors = etal | title = The dark matter environment of the A901 abell A901/902 supercluster: a weak lensing analysis of the HST STAGES survey | journal = [[Monthly Notices of the Royal Astronomical Society]] | date = April 2008 | volume = 385 | issue = 3 | pages = 1431β1442 | bibcode = 2008MNRAS.385.1431H | doi = 10.1111/j.1365-2966.2008.12919.x | doi-access = free |arxiv = 0801.1156 | s2cid = 59057342 }}</ref> By comparison, the [[mass-to-light ratio]] for the [[Milky Way]] is 63.8 assuming a solar [[absolute magnitude]] of 4.83,<ref name=nssdc> {{cite web | last = Williams | first = D. R. | date = 2004 | title = Sun Fact Sheet | url = http://nssdc.gsfc.nasa.gov/planetary/factsheet/sunfact.html | publisher = [[NASA]] | access-date = 2012-03-17 }}</ref> a Milky Way absolute magnitude of β20.9,<ref>{{cite web | url = http://www.universetoday.com/guide-to-space/the-universe/absolute-magnitude/ | title = Absolute Magnitude | author = Jerry Coffey | access-date = 2010-04-09 }}</ref> and a Milky Way mass of {{Solar mass|1.25{{e|12}}}}.<ref name=McMillan2011>{{citation | last1 = McMillan | first1 = Paul J. | title = Mass models of the Milky Way | journal = Monthly Notices of the Royal Astronomical Society | volume = 414 | issue = 3 | pages = 2446β2457 |date=July 2011 | doi = 10.1111/j.1365-2966.2011.18564.x | doi-access = free | bibcode = 2011MNRAS.414.2446M |arxiv = 1102.4340 | s2cid = 119100616 }}</ref> These ratios are one of the main arguments in favor of the presence of large amounts of [[dark matter]] in the universe; if dark matter did not exist, much smaller mass-to-light ratios would be expected.
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