Wilkinson Microwave Anisotropy Probe

NASA satellite of the Explorer program

Wilkinson Microwave Anisotropy Probe
Wilkinson Microwave Anisotropy Probe (WMAP) satellite
NamesExplorer 80
MAP
Microwave Anisotropy Probe
MIDEX-2
WMAP
Mission typeCosmic microwave background Astronomy
OperatorNASA
COSPAR ID2001-027A Edit this at Wikidata
SATCAT no.26859
Websitehttp://map.gsfc.nasa.gov/
Mission duration27 months (planned)
9 years (achieved)[1]
Spacecraft properties
SpacecraftExplorer LXXX
Spacecraft typeWilkinson Microwave Anisotropy Probe
BusWMAP
ManufacturerNRAO
Launch mass840 kg (1,850 lb)[2]
Dry mass763 kg (1,682 lb)
Dimensions3.6 × 5.1 m (12 × 17 ft)
Power419 watts
Start of mission
Launch date30 June 2001, 19:46:46 UTC[3]
RocketDelta II 7425-10 (Delta 246)
Launch siteCape Canaveral, SLC-17B
ContractorBoeing Launch Services
Entered service1 October 2001
End of mission
DisposalGraveyard orbit
Deactivated20 October 2010[4]
Last contact19 August 2010
Orbital parameters
Reference system Sun-Earth L2 orbit
RegimeLissajous orbit
Main telescope
TypeGregorian
Diameter1.4 × 1.6 m (4 ft 7 in × 5 ft 3 in)
Wavelengths23 GHz to 94 GHz
Instruments
Pseudo-Correlation Radiometer

Wilkinson Microwave Anisotropy Probe mission patch
Explorer program
← HETE-2 (Explorer 79)
RHESSI (Explorer 81) →
 

The Wilkinson Microwave Anisotropy Probe (WMAP), originally known as the Microwave Anisotropy Probe (MAP and Explorer 80), was a NASA spacecraft operating from 2001 to 2010 which measured temperature differences across the sky in the cosmic microwave background (CMB) – the radiant heat remaining from the Big Bang.[5][6] Headed by Professor Charles L. Bennett of Johns Hopkins University, the mission was developed in a joint partnership between the NASA Goddard Space Flight Center and Princeton University.[7] The WMAP spacecraft was launched on 30 June 2001 from Florida. The WMAP mission succeeded the COBE space mission and was the second medium-class (MIDEX) spacecraft in the NASA Explorer program. In 2003, MAP was renamed WMAP in honor of cosmologist David Todd Wilkinson (1935–2002),[7] who had been a member of the mission's science team. After nine years of operations, WMAP was switched off in 2010, following the launch of the more advanced Planck spacecraft by European Space Agency (ESA) in 2009.

WMAP's measurements played a key role in establishing the current Standard Model of Cosmology: the Lambda-CDM model. The WMAP data are very well fit by a universe that is dominated by dark energy in the form of a cosmological constant. Other cosmological data are also consistent, and together tightly constrain the Model. In the Lambda-CDM model of the universe, the age of the universe is 13.772±0.059 billion years. The WMAP mission's determination of the age of the universe is to better than 1% precision.[8] The current expansion rate of the universe is (see Hubble constant) 69.32±0.80 km·s−1·Mpc−1. The content of the universe currently consists of 4.628%±0.093% ordinary baryonic matter; 24.02%+0.88%
−0.87%
cold dark matter (CDM) that neither emits nor absorbs light; and 71.35%+0.95%
−0.96%
of dark energy in the form of a cosmological constant that accelerates the expansion of the universe.[9] Less than 1% of the current content of the universe is in neutrinos, but WMAP's measurements have found, for the first time in 2008, that the data prefer the existence of a cosmic neutrino background[10] with an effective number of neutrino species of 3.26±0.35. The contents point to a Euclidean flat geometry, with curvature ( Ω k {\displaystyle \Omega _{k}} ) of −0.0027+0.0039
−0.0038
. The WMAP measurements also support the cosmic inflation paradigm in several ways, including the flatness measurement.

The mission has won various awards: according to Science magazine, the WMAP was the Breakthrough of the Year for 2003.[11] This mission's results papers were first and second in the "Super Hot Papers in Science Since 2003" list.[12] Of the all-time most referenced papers in physics and astronomy in the INSPIRE-HEP database, only three have been published since 2000, and all three are WMAP publications. Bennett, Lyman A. Page Jr., and David N. Spergel, the latter both of Princeton University, shared the 2010 Shaw Prize in astronomy for their work on WMAP.[13] Bennett and the WMAP science team were awarded the 2012 Gruber Prize in cosmology. The 2018 Breakthrough Prize in Fundamental Physics was awarded to Bennett, Gary Hinshaw, Norman Jarosik, Page, Spergel, and the WMAP science team.

In October 2010, the WMAP spacecraft was derelict in a heliocentric graveyard orbit after completing nine years of operations.[14] All WMAP data are released to the public and have been subject to careful scrutiny. The final official data release was the nine-year release in 2012.[15][16]

Some aspects of the data are statistically unusual for the Standard Model of Cosmology. For example, the largest angular-scale measurement, the quadrupole moment, is somewhat smaller than the Model would predict, but this discrepancy is not highly significant.[17] A large cold spot and other features of the data are more statistically significant, and research continues into these.

Objectives

The universe's timeline, from the Big Bang to the WMAP
A comparison of the sensitivity of WMAP with COBE and Penzias and Wilson's telescope (simulated data)

The WMAP objective was to measure the temperature differences in the Cosmic Microwave Background (CMB) radiation. The anisotropies then were used to measure the universe's geometry, content, and evolution; and to test the Big Bang model, and the cosmic inflation theory.[18] For that, the mission created a full-sky map of the CMB, with a 13 arcminutes resolution via multi-frequency observation. The map required the fewest systematic errors, no correlated pixel noise, and accurate calibration, to ensure angular-scale accuracy greater than its resolution.[18] The map contains 3,145,728 pixels, and uses the HEALPix scheme to pixelize the sphere.[19] The telescope also measured the CMB's E-mode polarization,[18] and foreground polarization.[10] Its service life was 27 months; 3 to reach the L2 position, and 2 years of observation.[18]

Development

The MAP mission was proposed to NASA in 1995, selected for definition study in 1996, and approved for development in 1997.[20][21]

The WMAP was preceded by two missions to observe the CMB; (i) the Soviet RELIKT-1 that reported the upper-limit measurements of CMB anisotropies, and (ii) the U.S. COBE satellite that first reported large-scale CMB fluctuations. The WMAP was 45 times more sensitive, with 33 times the angular resolution of its COBE satellite predecessor.[22] The successor European Planck mission (operational 2009–2013) had a higher resolution and higher sensitivity than WMAP and observed in 9 frequency bands rather than WMAP's 5, allowing improved astrophysical foreground models.

Spacecraft

WMAP spacecraft diagram
Illustration of WMAP's receivers

The telescope's primary reflecting mirrors are a pair of Gregorian 1.4 × 1.6 m (4 ft 7 in × 5 ft 3 in) dishes (facing opposite directions), that focus the signal onto a pair of 0.9 × 1.0 m (2 ft 11 in × 3 ft 3 in) secondary reflecting mirrors. They are shaped for optimal performance: a carbon fibre shell upon a Korex core, thinly-coated with aluminium and silicon oxide. The secondary reflectors transmit the signals to the corrugated feedhorns that sit on a focal plane array box beneath the primary reflectors.[18]

The receivers are polarization-sensitive differential radiometers measuring the difference between two telescope beams. The signal is amplified with High-electron-mobility transistor (HEMT) low-noise amplifiers, built by the National Radio Astronomy Observatory (NRAO). There are 20 feeds, 10 in each direction, from which a radiometer collects a signal; the measure is the difference in the sky signal from opposite directions. The directional separation azimuth is 180°; the total angle is 141°. To improve subtraction of foreground signals from our Milky Way galaxy, the WMAP used five discrete radio frequency bands, from 23 GHz to 94 GHz.[18]

Properties of WMAP at different frequencies[18]
Property K-band Ka-band Q-band V-band W-band
Central wavelength (mm) 13 9.1 7.3 4.9 3.2
Central frequency (GHz) 23 33 41 61 94
Bandwidth (GHz) 5.5 7.0 8.3 14.0 20.5
Beam size (arcminutes) 52.8 39.6 30.6 21 13.2
Number of radiometers 2 2 4 4 8
System temperature (K) 29 39 59 92 145
Sensitivity (mK s 1 / 2 {\displaystyle ^{1/2}} ) 0.8 0.8 1.0 1.2 1.6

The WMAP's base is a 5.0 m (16.4 ft)-diameter solar panel array that keeps the instruments in shadow during CMB observations, (by keeping the craft constantly angled at 22°, relative to the Sun). Upon the array sit a bottom deck (supporting the warm components) and a top deck. The telescope's cold components: the focal-plane array and the mirrors, are separated from the warm components with a cylindrical, 33 cm (13 in)-long thermal isolation shell atop the deck.[18]

Passive thermal radiators cool the WMAP to approximately 90 K (−183.2 °C; −297.7 °F); they are connected to the low-noise amplifiers. The telescope consumes 419 W of power. The available telescope heaters are emergency-survival heaters, and there is a transmitter heater, used to warm them when off. The WMAP spacecraft's temperature is monitored with platinum resistance thermometers.[18]

The WMAP's calibration is effected with the CMB dipole and measurements of Jupiter; the beam patterns are measured against Jupiter. The telescope's data are relayed daily via a 2-GHz transponder providing a 667 kbit/s downlink to a 70 m (230 ft) Deep Space Network station. The spacecraft has two transponders, one a redundant backup; they are minimally active – about 40 minutes daily – to minimize radio frequency interference. The telescope's position is maintained, in its three axes, with three reaction wheels, gyroscopes, two star trackers and Sun sensors, and is steered with eight hydrazine thrusters.[18]

Launch, trajectory, and orbit

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