Wilkinson Microwave Anisotropy Probe
NINE-YEAR PAPERS
NINE-YEAR DATA
COSMOLOGICAL PARAMETERS TABLE
SEVEN-YEAR DATA
FIVE-YEAR DATA
THREE-YEAR DATA
FIRST-YEAR DATA
WMAP MISSION SITE
The WMAP (Wilkinson Microwave Anisotropy Probe) mission is designed to determine
the geometry, content, and evolution of the universe via a 13 arcminute FWHM
resolution full sky map of the temperature anisotropy of the cosmic microwave
background radiation. The choice of orbit, sky-scanning strategy and
instrument/spacecraft design were driven by the goals of uncorrelated pixel noise,
minimal systematic errors, multifrequency observations, and accurate calibration.
The skymap data products derived from the WMAP observations have 45 times the
sensitivity and 33 times the angular resolution of the COBE DMR mission. The WMAP
mission characteristics are summarized in the table below.
In the first release of WMAP data (February 2003), only the temperature data and analyses from the
first year of operations at L2 were provided.
Much more information and data was provided in the second release (March 2006); the
differences between the two are characterized by:
- Data from the first three years of spacecraft operations at L2 are made available.
- Polarization analysis, maps, and time-ordered data are made available.
- The temperature analysis and maps are improved.
- The error analysis was improved.
- The map-making algorithm was changed.
The third data release took place in March 2008. It was characterized by:
- Data from the first five years of spacecraft operations at L2 are made available.
- The temperature and polarization analysis and maps are improved.
- The error analysis was improved.
- The calibration algorithm was improved.
- The beam maps were improved.
The fourth release of data took place in January 2010. It is characterized by:
- Data from the first seven years of spacecraft operations at L2 are made available.
- The temperature and polarization analysis and maps are improved.
- The error analysis was improved.
- The calibration algorithm was improved.
- The beam maps were improved.
The fifth and final release of data took place in June 2012. It is characterized by:
- Data from the full nine years of spacecraft operations at L2 are made available.
- The temperature and polarization analysis and maps are improved.
- The error analysis was improved.
- The calibration algorithm was improved.
- The beam maps were improved.
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K-Banda |
Ka-Banda |
Q-Banda |
V-Banda |
W-Banda |
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Wavelength
(mm)b |
13 |
9.1 |
7.3 |
4.9 |
3.2 |
Frequency (GHz)b |
23 |
33 |
41 |
61 |
94 |
Bandwidth
(GHz)b, c |
5.5 |
7.0 |
8.3 |
14.0 |
20.5 |
Number of Differencing
Assemblies |
1 |
1 |
2 |
2 |
4 |
Number
of Radiometers |
2 |
2 |
4 |
4 |
8 |
Number of Channels |
4 |
4 |
8 |
8 |
16 |
Beam
Size (deg)b, d |
0.88 |
0.66 |
0.51 |
0.35 |
0.22 |
System Temperature,
Tsys (K)b, e |
29 |
39 |
59 |
92 |
145 |
Sensitivity
(mK sec½ )b |
0.8 |
0.8 |
1.0 |
1.2 |
1.6 |
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Sky Coverage |
Full sky |
Optical System |
Back-to-Back Gregorian, 1.4 x 1.6 m primaries |
Radiometric System |
Differential
polarization sensitive receivers |
Detection |
HEMT amplifiers |
Radiometer Modulation |
2.5 kHz phase switch |
Spin Modulation |
0.464 rpm = ~ 7.57 mHz spacecraft spin |
Precession Modulation |
1 rev hr -1 = ~ 0.3 mHz spacecraft precession |
Calibration |
In-flight: amplitude from dipole modulation, beam from Jupiter |
Cooling System |
Passively cooled to ~ 90 K |
Attitude Control |
3-axis controlled, 3 wheels, gyros, star trackers, sun sensors |
Propulsion |
Blow-down hydrazine with 8 thrusters |
RF Communication |
2 GHz transponders, 667 kbps down-link to 70 m DSN |
Power |
419 Watts |
Mass |
840 kg |
Launch |
Delta II 7425-10 on June 30, 2001 at 3:46:46.183 EDT |
Orbit |
1° - 10° Lissajous orbit about second Lagrange point, L2 |
Trajectory |
3 Earth-Moon phasing loops, lunar gravity assist to L2 |
Design Lifetime |
27 months = 3 month trajectory + 2 yrs at L2 |
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a Commercial
waveguide band designations used for the five MAP
frequency bands |
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b Typical values for a radiometer
are given. |
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c Effective signal bandwidth. |
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d The beam patterns are not Gaussian, and
thus are not simply specified. The size given here is the square-
root of the beam solid angle. |
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e Effective system temperature of the entire
system. |
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