Cosmic microwave background radiation
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{{Cosmology|cTopic=Early universe}}
In [[physical cosmology|cosmology]], the '''cosmic microwave background radiation''' (most often referred to by the acronym '''CMB''' but occasionally '''CMBR''', '''CBR''' or '''MBR''', also referred to as '''relic radiation''') is a form of [[electromagnetic radiation]] discovered in 1965 that fills the entire universe.<ref> {{cite journal |author=A.A. Penzias and R.W. Wilson |title=A Measurement of Excess Antenna Temperature at 4080 Mc/s |journal=Astrophysical Journal |volume=142 |pages=419–421 |year=1965 |doi=10.1086/148307}}</ref> It has a thermal [[black body]] spectrum at a temperature of 2.725 [[kelvin]]. Thus the spectrum peaks in the [[microwave]] range at a frequency of 160.2 [[hertz|GHz]], corresponding to a wavelength of 1.9 mm.
Measurements of cosmic background radiation are critical to cosmology, since any proposed model of the universe must explain this radiation as we observe it. Although the general feature of a black-body radiation spectrum could potentially be produced by many processes, the spectrum also contains small anisotropies, or irregularities, which vary with the size of the region examined. They have been measured in detail, and match to within experimental error that would be expected if small thermal fluctuations had expanded to the size of the universe we see today. As a result, most cosmologists consider this radiation to be the best evidence for the [[Big Bang]] model of the universe. See [[#Primary anisotropy|the plot of power spectrum of the cosmic microwave background radiation temperature anisotropy in terms of the angular scale]] below for details.
==Features==
[[Image:Firas spectrum.jpg|thumb|left|300px|The cosmic microwave background spectrum measured by the FIRAS instrument on the [[COBE| COBE satellite]] is the most precisely measured [[black body]] spectrum in nature. The [[data point]]s and [[Standard error of estimation|error bar]]s on this graph are obscured by the theoretical curve.]]
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The cosmic microwave background is [[isotropic]] to roughly one part in 100,000: the [[root mean square]] variations are only 18 µK.<ref>This ignores the [[dipole]] anisotropy, which is due to the [[Doppler shift]] of the microwave background radiation due to our [[peculiar velocity]] relative to the [[comoving coordinates|comoving]] cosmic rest frame. This feature is consistent with the Earth moving at some 380 km/s towards the constellation [[Virgo (constellation)|Virgo]].</ref> ''The Far-Infrared Absolute [[Spectrophotometer]]'' (''FIRAS'') instrument on the [[NASA]] [[COBE|Cosmic Background Explorer]] (COBE) satellite has carefully measured the spectrum of the cosmic microwave background. FIRAS compared the CMB with a reference [[black body]] and no difference could be seen in their spectra. Any deviations from the black body form that might still remain undetected in the CMB spectrum over the wavelength range from 0.5 to 5 mm must have a weighted [[Root mean square|rms]] value of at most 50 parts per million (0.005%) of the CMB peak brightness.<ref>{{cite journal |author=D. J. Fixsen ''et al.'' |title=The Cosmic Microwave Background Spectrum from the full COBE FIRAS data set |journal=Astrophysical Journal |volume=473 |pages=576–587 |year=1996 |doi=10.1086/178173}}</ref> This made the CMB spectrum the most precisely measured black body spectrum in nature.
The cosmic microwave background, and its level of [[isotropy]], are both predictions of [[Big Bang]] theory. In the theory, the early universe was made up of a hot [[plasma (physics)|plasma]] of [[photon]]s, [[electrons]] and [[baryon]]s. The photons were constantly interacting with the plasma through [[Thomson scattering]]. As the universe [[metric expansion of space|expanded]], adiabatic cooling caused the plasma to cool until it became favourable for [[electrons]] to combine with [[protons]] and form [[hydrogen]] atoms. This happened at around 3,000 K or when the universe was approximately 379,000<ref>{{cite web
| last=Abbott | first=Brian | date=[[May 30]], [[2007]]
| url=http://www.haydenplanetarium.org/universe/duguide/exgg_wmap.php
| title=Microwave (WMAP) All-Sky Survey
| publisher=Hayden Planetarium | accessdate=2008-01-13
}}</ref> years old (z=1088). At this point, the photons scattered off the now neutral atoms and began to travel freely through space. This process is called [[Timeline of the Big Bang#Recombination: 240,000-310,000 years|recombination]] or [[decoupling]] (referring to electrons combining with nuclei and to the decoupling of matter and radiation respectively).
The photons have continued cooling ever since; they have now reached 2.725 K and their temperature will continue to drop as long as the universe continues expanding. Accordingly, the radiation from the sky we measure today comes from a spherical surface, called the '''surface of last scattering'''. This represents the collection of points in space (currently around 46 billion light-years from the Earth—see [[Observable universe#Size|observable universe]]) at which the decoupling event happened long enough ago (less than 400,000 years after the Big Bang, 13.7 billion years ago) that the light from that part of space is just reaching observers.
The big bang theory suggests that the cosmic microwave background fills all of observable space, and that most of the radiation energy in the universe is in the cosmic microwave background, which makes up a fraction of roughly 5×10<sup>-5</sup> of the total density of the universe.<ref>The [[Planck's law of black body radiation|energy density of a black-body spectrum]] is <math>\pi^{2} k_{B}^{4}T^{4}/15(\hbar c)^{3}</math>, where ''T'' is the temperature, <math>k_B</math> is the Boltzmann constant, <math>\hbar</math> is the Planck constant and ''c'' is the speed of light. This can be related to the critical density of the universe using the parameters of the [[Lambda-CDM model]].</ref>
Two of the greatest successes of the big bang theory are its prediction of its almost perfect [[black body]] spectrum and its detailed prediction of the anisotropies in the cosmic microwave background. The recent [[Wilkinson Microwave Anisotropy Probe]] has precisely measured these anisotropies over the whole sky down to angular scales of 0.2 degrees.<ref>''Astrophysical Journal Supplement'', '''148''' (2003). In particular, {{cite journal |author=G. Hinshaw ''et al.'' |title=First-year Wilkinson Microwave Anisotropy Probe (WMAP) observations: the angular power spectrum |volume=148 |pages=135–159 |year=2003}}</ref> These can be used to estimate the parameters of the standard [[Lambda-CDM model]] of the big bang. Some information, such as the [[shape of the Universe]], can be obtained straightforwardly from the cosmic microwave background, while others, such as the [[Hubble constant]], are not constrained and must be inferred from other measurements.<ref>{{cite journal |author=D. N. Spergel ''et al.'' |title=First-year Wilkinson Microwave Anisotropy Probe (WMAP) observations: determination of cosmological parameters |journal=Astrophysical Journal Supplement |volume=148 |pages=175–194 |year=2003 |doi=10.1086/377226}} [http://arxiv.org/abs/astro-ph/0302209 arXiv preprint].</ref>
==History==
<!-- BEGIN TIMELINE -->
{| align="right" width="45%" style="border:1px solid #ddd; margin:0 0 1em 1em; padding:0 0 1em 1em; vertical-align:right;"
!colspan="2" align="center"|<big>Timeline of the CMB</big>
|-
|colspan="2" align="center"|<small>Important people and dates
|-valign=top
|-valign=top
|align="right">|1941
| [[Andrew McKellar]] The observational detection of an average bolometric temperature of 2.3 K based on the study of interstellar absorption lines is reported from the [[Dominion Astrophysical Observatory]].<ref name=>McKellar A (1941) Dominion Astrophysics Observatory Journal, Victoria, British Columbia, Vol VII, No 15, 251. McKellar was attempting to measure the average temperature of the intestellar medium. It is unlikely that he had any idea of the cosmological implications of his measurement, but it was a remarkable and sophisticated achievement.</ref><ref name=>Weinberg, Steven. Gravitation and Cosmology: Principles and applications of the general theory of relativity. John Wiley & sons Inc., 1972. p. 514</ref>
|-valign=top
|align="right">|1946
| [[Robert Dicke]] predicts ".. radiation from cosmic matter" at <20 K, but did not refer to background radiation<ref name=Kragh>Helge Kragh, Cosmology and Controversy: [http://books.google.com/books?id=f6p0AFgzeMsC&vid=ISBN069100546X&pg=PA135&lpg=PA135&sig=h6snxSfYc8zr3aoxiu-WbOJgpvk&q=cosmic+microwave The Historical Development of Two Theories of the Universe] (1999) ISBN 0-691-00546-X. "In 1946, Robert Dicke and coworkers at MIT tested equipment that could test a cosmic microwave background of intensity corresponding to about 20K in the microwave region. However, they did not refer to such a background, but only to 'radiation from cosmic matter'. Also, this work was unrelated to cosmology and is only mentioned because it suggests that by 1950, detection of the background radiation might have been technically possible, and also because of Dicke's later role in the discovery". See also Robert H. Dicke, Robert Beringer, Robert L. Kyhl, and A. B. Vane, "[http://prola.aps.org/abstract/PR/v70/i5-6/p340_1 Atmospheric Absorption Measurements with a Microwave Radiometer]" (1946) ''Phys. Rev''. 70, 340–348</ref>
|-valign=top
|align="right">|1948
|[[George Gamow]] calculates a temperature of 50 K (assuming a 3-billion year old Universe),<ref>George Gamow, ''[http://books.google.com/books?id=5awirwgmvAoC&pg=PA40&lpg=PA40&vq=50&dq=%22creation+of+the+universe%22+gamow&sig=cnNpSmeBqcMg7dnA4ImfKjiLNE0 The Creation Of The Universe]'' p.40 (Dover reprint of revised 1961 edition) ISBN 0-486-43868-6</ref> commenting it ".. is in reasonable agreement with the actual temperature of interstellar space", but does not mention background radiation.
|-valign=top
|align="right">|1948
|[[Ralph Alpher]] and [[Robert Herman]] estimate "the temperature in the Universe" at 5 K. Although they do not specifically mention microwave background radiation, it may be inferred.<ref>Helge Kragh, Cosmology and Controversy: [http://books.google.com/books?vid=ISBN069100546X&id=f6p0AFgzeMsC&pg=PA132&lpg=PA132&vq=cosmic+microwave&sig=YvmlZ13jwKPS0ucC5ogFsPqwfnY The Historical Development of Two Theories of the Universe] (1999) ISBN 0-691-00546-X. "Alpher and Herman first calculated the present temperature of the decoupled primordial radiation in 1948, when they reported a value of 5 K. Although it was not mentioned either then or in later publications that the radiation is in the microwave region, this follows immediately from the temperature... Alpher and Herman made it clear that what they had called "the temperature in the universe" the previous year referred to a blackbody distributed background radiation quite different from sunliight".</ref>
|-valign=top
|align="right">|1950
|Ralph Alpher and Robert Herman re-re-estimate the temperature at 28 K.
|-valign=top
|align="right">|1953
|[[George Gamow]] estimates 7 K.<ref name=Kragh />
|-valign=top
|align="right">|1956
|[[George Gamow]] estimates 6 K.<ref name=Kragh />
|-valign=top
|align="right">|1957
|Tigran Shmaonov reports that "the absolute effective temperature of the radioemission background ... is 4+/- 3K".<ref>Tigran Shmaonov, ''Pribory i Teknika Eksperienta'' (1957)</ref> It is noted that the "measurements showed that radiation intensity was independent of either time or direction of observation... it is now clear that Shmaonov did observe the cosmic microwave background at a wavelength of 3.2cm"<ref>Dmitri I. Novikov, The Physics of the Cosmic Microwave Background, 2006, Cambridge University Press, 272 pages, ISBN 0521855500. ([http://books.google.com/books?hl=en&lr=&id=J2KCisZsWZ0C&oi=fnd&pg=RA1-PA1&dq=Shmaonov+cmb&ots=JBjbEu7tNl&sig=JgZNDEsD8ULPUv4WI8my3IZED1U#PRA1-PA5,M1 page 5])</ref>
|-valign=top
|align="right">|1960s
|Robert Dicke re-estimates a MBR (microwave background radiation) temperature of 40 K<ref name=Kragh />
|-valign=top
|align="right">|1964
| [[A. G. Doroshkevich]] and [[Igor Dmitriyevich Novikov|Igor Novikov]] publish a brief paper, where they name the CMB radiation phenomenon as detectable.<ref>A. G. Doroshkevich and I. D. Novikov, "[http://adsabs.harvard.edu/abs/1964SPhD....9..111D Mean Density of Radiation in the Metagalaxy and Certain Problems in Relativistic Cosmology]" ''Sov. Phys. Doklady'' 9, 111 (1964).</ref>
|-valign=top
|align="right">|1964-65
| [[Arno Penzias]] and [[Robert Woodrow Wilson]] measure the temperature to be approximately 3 K. Robert Dicke, [[P. J. E. Peebles]], P. G. Roll and [[David Todd Wilkinson|D. T. Wilkinson]] interpret this radiation as a signature of the big bang.
|-valign=top
|align="right">|1983
| [[RELIKT-1]] Soviet CMB anisotropy experiment was launched.
|-valign=top
|align="right">|1990
| FIRAS measures the black body form of the CMB spectrum with exquisite precision.
|-valign=top
|align="right">|January 1992
| Scientists who analysed data from [[RELIKT-1]] spacecraft report the discovery of anisotropy at the Moscow astrophysical seminar.<ref>''Nobel Prize In Physics: Russia's Missed Opportunities'', [[RIA Novosti]], November 21, 2006</ref>
|-valign=top
|align="right">|April, 1992
| Scientists who analysed data from [[COBE]] DMR announce the discovery of the primary temperature anisotropy.<ref>[http://www.berkeley.edu/news/media/releases/2006/10/03_nobelph.shtml 10.03.2006 - UC Berkeley & LBL scientist George Smoot awarded Nobel Prize in Physics<!-- Bot generated title -->]</ref>
|-valign=top
|align="right">|1999
| First measurements of acoustic oscillations in the CMB anisotropy angular power spectrum from the TOCO, BOOMERANG and Maxima Experiments.
|-valign=top
|align="right">|2002
| Polarization discovered by DASI.<ref>J. Kovac ''et al.'', "Detection of polarization in the cosmic microwave background using DASI", ''Nature'' '''420''', 772-787 (2002).</ref>
|-valign=top
|align="right">|2004
| E-mode polarization spectrum obtained by the CBI.<ref>A. Readhead ''et al.'', "Polarization observations with the Cosmic Background Imager", ''Science'' '''306''', 836-844 (2004).</ref>
|}
<!-- END TIMELINE -->
{{see also|Discovery of cosmic microwave background radiation|Timeline of cosmic microwave background astronomy}}
The cosmic microwave background was predicted in 1948 by [[George Gamow]] and [[Ralph Alpher]], and by Alpher and [[Robert Herman]]. Moreover, Alpher and Herman were able to estimate the temperature of the cosmic microwave background to be 5 K, though two years later, they re-estimated it at 28 K.<ref>G. Gamow, "The Origin of Elements and the Separation of Galaxies," ''Physical Review'' '''74''' (1948), 505. G. Gamow, "The evolution of the universe", ''Nature'' '''162''' (1948), 680. R. A. Alpher and R. Herman, "On the Relative Abundance of the Elements," ''Physical Review'' '''74''' (1948), 1577.</ref> Although there were several
previous estimates of the temperature of space (see timeline), these suffered from two flaws. First, they were measurements of the ''effective'' temperature of space, and did not suggest that space was filled with a thermal [[Planck spectrum]]; second, they are dependent on our special place at the edge of the [[Milky Way galaxy]] and did not suggest the radiation is isotropic. Moreover, they would yield very different predictions if Earth happened to be located elsewhere in the universe.<ref>A. K. T. Assis, M. C. D. Neves, "History of the 2.7 K Temperature Prior to Penzias and Wilson," (1995, [http://redshift.vif.com/JournalFiles/Pre2001/V02NO3PDF/V02N3ASS.PDF PDF] | [http://www.dfi.uem.br/~macedane/history_of_2.7k.html HTML]) but see also N. Wright, "Eddington did not predict the CMB", [http://www.astro.ucla.edu/~wright/Eddington-T0.html].</ref>
The 1948 results of Gamow and Alpher were not widely discussed. However, they were rediscovered by [[Yakov Zel'dovich]] in the early 1960s, and independently predicted by [[Robert Dicke]] at the same time. The first published recognition of the CMB radiation as a detectable phenomenon appeared in a brief paper by [[Soviet Union|Soviet]] astrophysicists [[A. G. Doroshkevich]] and [[Igor Dmitriyevich Novikov|Igor Novikov]], in the spring of 1964.<ref>{{cite web|author=A. A. Penzias|title="The origin of elements."|work=[[Nobel Prize in Physics|Nobel lecture]]|url=http://nobelprize.org/nobel_prizes/physics/laureates/1978/penzias-lecture.pdf|accessmonthday=October 4 |accessyear=2006}}</ref> In 1964, [[David Todd Wilkinson]] and Peter Roll, Dicke's colleagues at [[Princeton University]], began constructing a Dicke radiometer to measure the cosmic microwave background.<ref>R. H. Dicke, "The measurement of thermal radiation at microwave frequencies", ''Rev. Sci. Instrum.'' '''17''', 268 (1946). This basic design for a radiometer has been used in most subsequent cosmic microwave background experiments.</ref> In 1965, [[Arno Penzias]] and [[Robert Woodrow Wilson]] at the [[Crawford Hill]] location of [[Bell Telephone Laboratories]] in nearby [[Holmdel Township, New Jersey]] had built a Dicke radiometer that they intended to use for radio astronomy and satellite communication experiments. Their instrument had an excess 3.5 K [[noise temperature|antenna temperature]] which they could not account for. After receiving a telephone call from Crawford Hill, Dicke famously quipped: "Boys, we've been scooped."<ref>A. A. Penzias and R. W. Wilson, "A Measurement of Excess Antenna Temperature at 4080 Mc/s," ''Astrophysical Journal'' '''142''' (1965), 419. R. H. Dicke, P. J. E. Peebles, P. G. Roll and D. T. Wilkinson, "Cosmic Black-Body Radiation," ''Astrophysical Journal'' '''142''' (1965), 414. The history is given in P. J. E. Peebles, ''Principles of physical cosmology'' (Princeton Univ. Pr., Princeton 1993).</ref> A meeting between the Princeton and Crawford Hill groups determined that the antenna temperature was indeed due to the microwave background. Penzias and Wilson received the 1978 [[Nobel Prize in Physics]] for their discovery.
The interpretation of the cosmic microwave background was a controversial issue in the 1960s with some proponents of the [[steady state theory]] arguing that the microwave background was the result of [[integrated starlight|scattered starlight]] from distant galaxies. Using this model, and based on the study of narrow absorption line features in the spectra of stars, the astronomer [[Andrew McKellar]] wrote in 1941: "It can be calculated that the '[[rotational temperature]]ˡ of interstellar space is 2 K."<ref>A. McKellar, ''Publ. Dominion Astrophys. Obs.'' '''7''', 251.</ref> However, during the 1970s the consensus was established that the cosmic microwave background is a remnant of the big bang. This was largely because new measurements at a range of frequencies showed that the spectrum was a thermal, [[black body]] spectrum, a result that the steady state model was unable to reproduce.
[[Image:Horn Antenna-in Holmdel, New Jersey.jpeg|thumb|200px|left|The [[Horn Antenna]] on which Penzias and Wilson discovered the cosmic microwave background.]]
Harrison, Peebles and Yu, and Zel'dovich realized that the early universe would have to have inhomogeneities at the level of 10<sup>-4</sup> or 10<sup>−5</sup>.<ref>E. R. Harrison, "Fluctuations at the threshold of classical cosmology," ''Phys. Rev.'' '''D1''' (1970), 2726. P. J. E. Peebles and J. T. Yu, "Primeval adiabatic perturbation in an expanding universe," ''Astrophysical Journal'' '''162''' (1970), 815. Ya. B. Zel'dovich, "A hypothesis, unifying the structure and entropy of the universe," ''Monthly Notices of the Royal Astronomical Society'' '''160''' (1972).</ref> [[Rashid Sunyaev]] later calculated the observable imprint that these inhomogeneities would have on the cosmic microwave background.<ref>R. A. Sunyaev, "Fluctuations of the microwave background radiation," in ''Large Scale Structure of the Universe'' ed. M. S. Longair and J. Einasto, 393. Dordrecht: Reidel 1978. While this is the first paper to discuss the detailed observational imprint of density inhomogeneities as anisotropies in the cosmic microwave background, some of the groundwork was laid in Peebles and Yu, above.</ref> Increasingly stringent limits on the anisotropy of the cosmic microwave background were set by ground based experiments, but the anisotropy was first detected by the Differential Microwave Radiometer instrument on the [[COBE]] satellite.<ref>[[George Smoot|G. F. Smoot]] ''et al.'' "Structure in the COBE DMR first year maps", ''Astrophysical Journal'' '''396''' L1–L5 (1992). C. L. Bennett ''et al.'' "Four year COBE DMR cosmic microwave background observations: maps and basic results.", ''Astrophysical Journal'' '''464''' L1–L4 (1996).</ref>
Inspired by the COBE results, a series of ground and balloon-based experiments measured cosmic microwave background anisotropies on smaller angular scales over the next decade. The primary goal of these experiments was to measure the scale of the first acoustic peak, which COBE did not have sufficient resolution to resolve. The first peak in the anisotropy was tentatively detected by the [[Toco experiment]] and the result was confirmed by the [[BOOMERanG experiment|BOOMERanG]] and [[Millimeter Anisotropy eXperiment IMaging Array|MAXIMA]] experiments.<ref>A. D. Miller ''et al.'', "A measurement of the angular power spectrum of the cosmic microwave background from ''l'' = 100 to 400", ''Astrophysical Journal'' '''524''', L1–L4 (1999). A. Melchiorri ''et al.'', "A measurement of Omega from the North American test flight of BOOMERANG" (1999). A. E. Lange ''et al.'', "Cosmological parameters from the first results of Boomerang". P. de Bernardis ''et al.'', "A flat universe from high-resolution maps of the cosmic microwave background", ''Nature'' '''404''', 955 (2000). S. Hanany ''et al.'' "MAXIMA-1: A measurement of the cosmic microwave background anisotropy on angular scales of 10'-5°", ''Astrophysical Journal'' '''545''' L5–L9 (2000).</ref> These measurements demonstrated that the [[Shape of the Universe|Universe is approximately flat]] and were able to rule out [[cosmic strings]] as a major component of cosmic structure formation, and suggested [[cosmic inflation]] was the right theory of structure formation.
The second peak was tentatively detected by several experiments before being definitively detected by [[WMAP]], which has also tentatively detected the third peak. Several experiments to improve measurements of the polarization and the microwave background on small angular scales are ongoing. These include DASI, WMAP, BOOMERanG and the [[Cosmic Background Imager]]. Forthcoming experiments include the [[Planck (satellite)|Planck satellite]], [[Atacama Cosmology Telescope]], [[QUIET telescope]] and the [[South Pole Telescope]].
[[Image:WMAP 2008.png|thumb|right|300px|[[WMAP]] image of the CMB temperature anisotropy.]]
==Relationship to the Big Bang==
Measurements of the CMB have made the inflationary Big Bang theory the standard model of the earliest eras of the universe. The standard hot big bang model of the universe requires that the initial conditions for the universe are a [[Gaussian random field]] with a nearly [[scale invariant]] or Harrison-Zel'dovich spectrum. This is, for example, a prediction of the [[cosmic inflation]] model. This means that the initial state of the universe is random, but in a clearly specified way in which the amplitude of the primeval inhomogeneities is 10<sup>-5</sup>. Therefore, meaningful statements about the inhomogeneities in the universe need to be [[statistics|statistical]] in nature. This leads to [[cosmic variance]] in which the uncertainties in the variance of the largest scale fluctuations observed in the universe are difficult to accurately compare to theory.
===Temperature===
The cosmic microwave background radiation and the cosmological [[red shift]] are together regarded as the best available evidence for the [[Big Bang]] (BB) theory. The discovery of the CMB in the mid-1960s curtailed interest in [[non-standard cosmology|alternatives]] such as the [[steady state theory]]. The CMB gives a snapshot of the [[Universe]] when, according to standard cosmology, the temperature dropped enough to allow [[electron]]s and [[proton]]s to form [[hydrogen]] atoms, thus making the universe transparent to radiation. When it originated some [[1 E13 s|400,000 years]] after the Big Bang — this time period is generally known as the "time of last scattering" or the period of [[recombination]] or [[decoupling]] — the temperature of the Universe was about [[1 E3 K|3,000 K]]. This corresponds to an energy of about 0.25 [[electronvolt|eV]], which is much less than the 13.6 eV ionization energy of hydrogen. Since then, the temperature of the radiation has dropped by a factor of roughly 1100 due to the expansion of the Universe. As the universe expands, the CMB photons are [[redshift]]ed, making the radiation's temperature [[inversely proportional]] to the Universe's [[Scale factor (Universe)|scale length]]. For details about the reasoning that the radiation is evidence for the Big Bang, see [[Big Bang#Cosmic microwave background radiation|Cosmic background radiation of the Big Bang]].
[[Image:WMAP TT power spectrum.png|thumb|right|300px|The power spectrum of the cosmic microwave background radiation temperature anisotropy in terms of the angular scale (or [[multipole moment]]). The data shown come from the [[WMAP]] (2006), [[Arcminute Cosmology Bolometer Array Receiver|Acbar]] (2004) [[BOOMERanG experiment|Boomerang]] (2005), [[Cosmic Background Imager|CBI]] (2004) and [[Very Small Array|VSA]] (2004) instruments.]]
===Primary anisotropy===
The [[anisotropy]] of the cosmic microwave background is divided into two sorts: primary anisotropy – which is due to effects which occur at the last scattering surface and before – and secondary anisotropy – which is due to effects, such as interactions with hot gas or gravitational potentials, between the last scattering surface and the observer.
The structure of the cosmic microwave background anisotropies is principally determined by two effects: acoustic oscillations and diffusion damping (also called collisionless damping or [[Joseph Silk| Silk damping]]). The acoustic oscillations arise because of a competition in the [[photon]]-[[baryon]] plasma in the early universe. The pressure of the photons tends to erase anisotropies, whereas the gravitational attraction of the baryons – which are moving at speeds much less than the speed of light – makes them tend to collapse to form dense haloes. These two effects compete to create acoustic oscillations which give the microwave background its characteristic peak structure. The peaks correspond, roughly, to resonances in which the photons decouple when a particular mode is at its peak amplitude.
The peaks contain interesting physical signatures. The angular scale of the first peak determines the [[shape of the Universe|curvature of the Universe]] (but not the [[topology]] of the Universe). The second peak – truly the ratio of the odd peaks to the even peaks – determines the reduced baryon density. The third peak can be used to extract information about the dark matter density.
The locations of the peaks also give important information about the nature of the primordial density perturbations. There are two fundamental types of density perturbations -- called "adiabatic" and "isocurvature."
A general density perturbation is a mixture of these two types, and different theories that purport to explain the primordial density perturbation spectrum predict different mixtures.
*adiabatic density perturbations
:the fractional overdensity in each matter component ([[baryon]]s, [[photon]]s ...) is the same. That is, if there is 1% more energy in baryons than average in one spot, then with a pure adiabatic density perturbations there is also 1% more energy in photons, and 1% more energy in neutrinos, than average. [[Cosmic inflation]] predicts that the primordial perturbations are adiabatic.
*isocurvature density perturbations
:the sum of the fractional overdensities is zero. That is, a perturbation where at some spot there is 1% more energy in baryons than average, 1% more energy in photons than average, and 2% ''lower'' energy in neutrinos than average, would be a pure isocurvature perturbation. [[Cosmic string]]s would produce mostly isocurvature primordial perturbations.
The CMB spectrum is able to distinguish these two because these two types of perturbations produce different peak locations. Isocurvature density perturbations produce a series of peaks whose angular scales (''l''-values of the peaks) are roughly in the ratio 1 : 3 : 5 ..., while adiabatic density perturbations produce peaks whose locations are in the ratio 1 : 2 : 3 ...<ref name="hu_white_1996">Wayne Hu and Martin White, "Acoustic Signatures in the Cosmic Microwave Background." Astrophysical Journal, ''471'', 30.</ref> Observations are consistent with the primordial density perturbations being entirely adiabatic, providing key support for inflation, and ruling out many models of structure formation involving, for example, cosmic strings.
Collisionless damping is caused by two effects, when the treatment of the primordial plasma as a [[fluid]] begins to break down:
* the increasing [[mean free path]] of the photons as the primordial plasma becomes increasingly rarefied in an expanding universe
* the finite thickness of the last scattering surface (LSS), which causes the mean free path to increase rapidly during decoupling, even while some Compton scattering is still occurring.
These effects contribute about equally to the suppression of anisotropies on small scales, and give rise to the characteristic exponential damping tail seen in the very small angular scale anisotropies.
The thickness of the LSS refers to the fact that the decoupling of the photons and baryons does not happen instantaneously, but instead requires an appreciable fraction of the age of the Universe up to that era. One method to quantify exactly ''how'' long this process took uses the ''photon visibility function'' (PVF). This function is defined so that, denoting the PVF by P(t), the probability that a CMB photon last scattered between time t and t+dt is given by P(t)dt.
The maximum of the PVF (the time where it is most likely that a given CMB photon last scattered) is known quite precisely. The first-year WMAP results put the time at which P(t) is maximum as 372 +/- 14 kyr.<ref name="WMAP_1_cosmo_params">WMAP Collaboration, " First year Wilkinson Microwave Anisotropy Probe (WMAP) observations: Determination of cosmological parameters." Astrophys. J. Suppl. ''148'' 175 (2003). arXiv astro-ph/0302209</ref> This is often taken as the "time" at which the CMB formed. However, to figure out how ''long'' it took the photons and baryons to decouple, we need a measure of the width of the PVF. The WMAP team finds that the PVF is greater than half of its maximum value (the "full width at half maximum", or FWHM) over an interval of 115 +/- 5 kyr. By this measure, decoupling took place over roughly 115,000 years, and when it was complete, the universe was roughly 487,000 years old.
===Late time anisotropy===
After the creation of the CMB, it is modified by several physical processes collectively referred to as late-time anisotropy or secondary anisotropy. After the emission of the CMB, ordinary matter in the universe was mostly in the form of neutral hydrogen and helium atoms, but from observations of galaxies it seems that most of the volume of the [[intergalactic medium]] (IGM) today consists of ionized material (since there are few absorption lines due to hydrogen atoms). This implies a period of [[reionization]] in which the material of the universe breaks down into hydrogen ions.
The CMB photons scatter off free charges such as electrons that are not bound in atoms. In an ionized universe, such electrons have been liberated from neutral atoms by ionizing (ultraviolet) radiation. Today these free charges are at sufficiently low density in most of the volume of the Universe that they do not measurably affect the CMB. However, if the IGM was ionized at very early times when the universe was still denser, then there are two main effects on the CMB:
# Small scale anisotropies are erased (just as when looking at an object through fog, details of the object appear fuzzy).
# The physics of how photons scatter off free electrons ([[Thomson scattering]]) induces polarization anisotropies on large angular scales. This large angle polarization is correlated with the large angle temperature perturbation.
Both of these effects have been observed by the WMAP satellite, providing evidence that the universe was ionized at very early times, at a [[redshift]] larger than 17. The detailed provenance of this early ionizing radiation is still a matter of scientific debate. It may have included starlight from the very first population of stars ([[population III]] stars), supernovae when these first stars reached the end of their lives, or the ionizing radiation produced by the accretion disks of massive black holes.
The period after the emission of the cosmic microwave background and before the observation of the first stars is semi-humorously referred to by cosmologists as the [[Dark Ages (disambiguation)|dark age]], and is a period which is under intense study by astronomers (See [[21 centimeter radiation]]).
Other effects that occur between reionization and our observation of the cosmic microwave background which cause anisotropies include the [[Sunyaev-Zel'dovich effect]], in which a cloud of high energy electrons scatters the radiation, transferring some energy to the CMB photons, and the [[Sachs-Wolfe effect]], which causes [[photon]]s from the cosmic microwave background to be gravitationally redshifted or blue shifted due to changing gravitational fields.
[[Image:WMAP 3yr EE.png|thumb|right|300px|E polarization measurements as of March 2006 in terms of angular scale (or [[multipole moment]]). The polarization is much more poorly measured than the temperature anisotropy.]]
===Velocity relative to CMB anisotropy===
From the CMB data it is seen that our local group of galaxies (the galactic cluster that includes the Solar System's Milky Way Galaxy) appears to be moving at 627 ± 22 km/s relative to the reference frame of the CMB in the direction of galactic longitude ''l'' = 264.4<sup>o</sup>, ''b'' = 48.4<sup>o</sup>. <ref>[http://adsabs.harvard.edu/abs/1993ApJ...419....1K "Dipole Anisotropy in the COBE Differential Microwave Radiometers First-Year Sky Maps" Kogut, et al Astrophysical Journal, 1993]</ref> This motion results in an anisotropy of the data (CMB appearing slightly warmer in the direction of movement than in the opposite direction).
The standard interpretation of this temperature variation is a simple velocity redshift and blueshift due to motion relative to the CMB, however alternative cosmological models can explain some fraction of the observed dipole temperature distribution in the CMB (see reference for one example). <ref>[http://adsabs.harvard.edu/abs/2007ApJ...664..650I "Local Voids as the Origin of Large-Angle Cosmic Microwave Background Anomalies: The Effect of a Cosmological Constant." Inoue and Silk Astrophysical Journal, 2007]</ref>
===Polarization===<!-- This section is linked from [[Cosmic inflation]] -->
The cosmic microwave background is [[polarization|polarized]] at the level of a few microkelvins. There are two types of polarization, called ''E''-modes and ''B''-modes. This is in analogy to [[electrostatics]], in which the electric field (''E''-field) has a vanishing [[Curl (mathematics)|curl]] and the magnetic field (''B''-field) has a vanishing [[divergence]]. The ''E''-modes arise naturally from [[Thomson scattering]] in an inhomogeneous plasma. The ''B''-modes, which have not been measured and are thought to have an amplitude of at most a 0.1 µK, are not produced from the plasma physics alone. They are a signal from [[cosmic inflation]] and are determined by the density of primordial [[gravitational wave]]s. Detecting the ''B''-modes will be extremely difficult, particularly given that the degree of foreground contamination is unknown, and the [[weak gravitational lensing]] signal mixes the relatively strong ''E''-mode signal with the ''B''-mode signal.<ref>{{cite journal | author = A. Lewis and A. Challinor | title = Weak gravitational lensing of the CMB | journal = Phys. Rep. | volume= 429|year=2006|pages=1–65 | doi = 10.1016/j.physrep.2006.03.002}}{{arxiv|archive=astro-ph|id=0601594}}</ref>
==Microwave background observations==
{{main|Cosmic microwave background experiments}}
Subsequent to the discovery of the CMB, hundreds of cosmic microwave background experiments have been conducted to measure and characterize the signatures of the radiation. The most famous experiment is probably the [[NASA]] Cosmic Background Explorer ([[COBE]]) satellite that orbited in 1989–1996 and which detected and quantified the large scale anisotropies at the limit of its detection capabilities. Inspired by the initial COBE results of an extremely isotropic and homogeneous background, a series of ground- and balloon-based experiments quantified CMB anisotropies on smaller angular scales over the next decade. The primary goal of these experiments was to measure the angular scale of the first acoustic peak, for which COBE did not have sufficient resolution. These measurements were able to rule out [[cosmic strings]] as the leading theory of cosmic structure formation, and suggested [[cosmic inflation]] was the right theory. During the 1990s, the first peak was measured with increasing sensitivity and by 2000 the [[BOOMERanG experiment]] reported that the highest power fluctuations occur at scales of approximately one degree. Together with other cosmological data, these results implied that the geometry of the Universe is [[flat space|flat]]. A number of ground-based [[interferometer]]s provided measurements of the fluctuations with higher accuracy over the next three years, including the [[Very Small Array]],
[[Degree Angular Scale Interferometer]] (DASI) and the [[Cosmic Background Imager]] (CBI). DASI made the first detection of the polarization of the CMB and the CBI provided the first E-mode polarization spectrum with compelling evidence that it is out of phase with the T-mode spectrum.
In June 2001, [[NASA]] launched a second CMB space mission, [[WMAP]], to make much more precise measurements of the large scale anisotropies over the full sky. The first results from this mission, disclosed in 2003, were detailed measurements of the angular power spectrum to below degree scales, tightly constraining various cosmological parameters. The results are broadly consistent with those expected from [[cosmic inflation]] as well as various other competing theories, and are available in detail at NASA's data center for Cosmic Microwave Background (CMB) (see links below). Although WMAP provided very accurate measurements of the large angular-scale fluctuations in the CMB (structures about as large in the sky as the moon), it did not have the angular resolution to measure the smaller scale fluctuations which had been observed using previous ground-based [[interferometer]]s.
A third space mission, the [[Planck Surveyor]], is to be launched in 2008. Planck employs both [[HEMT]] radiometers as well as [[bolometer]] technology and will measure the CMB on smaller scales than WMAP. Unlike the previous two space missions, Planck is a collaboration between NASA and [[European Space Agency|ESA]] (the European Space Agency). Its detectors got a trial run at the Antarctic [[Viper telescope]] as ACBAR ([[Arcminute Cosmology Bolometer Array Receiver]]) experiment – which has produced the most precise measurements at small angular scales to date – and at the [[Archeops]] balloon telescope.
Additional ground-based instruments such as the [[South Pole Telescope]] in Antarctica and the proposed [[Clover (telescope)|Clover]] Project, [[Atacama Cosmology Telescope]] and the [[QUIET telescope]] in Chile will provide additional data not available from satellite observations, possibly including the B-mode polarization.
==References==
{{commonscat}}
{{Reflist}}
== External links ==
* [http://www.astroscience-berlin.org/index.php/become Here you can "listen" to the echo of the Big Bang]
[[Category:Radio astronomy]]
[[Category:Physical cosmology]]
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