WMAP

(Wilkinson Microwave Anisotropy Probe)

Other Web pages: Spires


References

  1 - Reviews

  2 - Articles

  3 - Detector

  4 - Conference Proceedings

The references in each group are listed in approximate inverted chronological order.
Click on the reference label to search it in inSPIRE.


1 - Reviews

[1-1]
The Wilkinson Microwave Anisotropy Probe, Lyman Page, arXiv:astro-ph/0306381, 2003. Carnegie Observatories Astrophysics Series, Vol. 2: Measuring and Modeling the Universe.


2 - Articles

[2-1]
Seven-Year Wilkinson Microwave Anisotropy Probe (WMAP) Observations: Are There Cosmic Microwave Background Anomalies?, C. L. Bennett et al., Astrophys. J. Suppl. 192 (2011) 17, arXiv:1001.4758.
[2-2]
Seven-Year Wilkinson Microwave Anisotropy Probe (WMAP) Observations: Sky Maps, Systematic Errors, and Basic Results, N. Jarosik et al., Astrophys. J. Suppl. 192 (2011) 14, arXiv:1001.4744.
[2-3]
Seven-Year Wilkinson Microwave Anisotropy Probe (WMAP) Observations: Planets and Celestial Calibration Sources, J. L. Weiland et al., Astrophys. J. Suppl. 192 (2011) 19, arXiv:1001.4731.
[2-4]
Seven-Year Wilkinson Microwave Anisotropy Probe (WMAP) Observations: Power Spectra and WMAP-Derived Parameters, D. Larson et al., Astrophys. J. Suppl. 192 (2011) 16, arXiv:1001.4635.
[2-5]
Seven-Year Wilkinson Microwave Anisotropy Probe (WMAP) Observations: Galactic Foreground Emission, B. Gold et al., Astrophys. J. Suppl. 192 (2011) 15, arXiv:1001.4555.
[2-6]
Seven-Year Wilkinson Microwave Anisotropy Probe (WMAP) Observations: Cosmological Interpretation, E. Komatsu et al. (WMAP), Astrophys. J. Suppl. 192 (2011) 18, arXiv:1001.4538.
From the abstract: Notable examples of improved parameters are the total mass of neutrinos, \sum m_\nu
< 0.58
<b>eV</b>
\text{(95% CL)}, and the effective number of neutrino species, N_{<b>eff</b>} = 4.34^{+ 0.86}_{- 0.88} \text{(68%~CL)}, which benefit from better determinations of the third peak and H_0.
[2-7]
Five-Year Wilkinson Microwave Anisotropy Probe (WMAP) Observations: Data Processing, Sky Maps, and Basic Results, G. Hinshaw et al. (WMAP), Astrophys. J. Suppl. 180 (2009) 225-245, arXiv:0803.0732.
[2-8]
Five-Year Wilkinson Microwave Anisotropy Probe (WMAP) Observations: Galactic Foreground Emission, B. Gold et al. (WMAP), Astrophys. J. Suppl. 180 (2009) 265-282, arXiv:0803.0715.
[2-9]
Five-Year Wilkinson Microwave Anisotropy Probe (WMAP) Observations: Angular Power Spectra, M. R. Nolta et al. (WMAP), Astrophys. J. Suppl. 180 (2009) 296-305, arXiv:0803.0593.
[2-10]
Five-Year Wilkinson Microwave Anisotropy Probe (WMAP) Observations: Likelihoods and Parameters from the WMAP data, J. Dunkley et al. (WMAP), Astrophys. J. Suppl. 180 (2009) 306-329, arXiv:0803.0586.
[2-11]
Five-Year Wilkinson Microwave Anisotropy Probe (WMAP)Observations: Beam Maps and Window Functions, R. S. Hill et al. (WMAP), Astrophys. J. Suppl. 180 (2009) 246-264, arXiv:0803.0570.
[2-12]
Five-Year Wilkinson Microwave Anisotropy Probe (WMAP) Observations: Cosmological Interpretation, E. Komatsu et al. (WMAP), Astrophys. J. Suppl. 180 (2009) 330-376, arXiv:0803.0547.
From the abstract: The WMAP 5-year data provide stringent limits on deviations from the minimal, 6-parameter \Lambda<b>CDM</b> model.... We detect no convincing deviations from the minimal model....
\Omega_\Lambda = 0.721 +- 0.015,..., H_0 = 70.1 +- 1.3 \text{km}
<b>s</b>^{-1} \text{Mpc}^{-1}, \Omega_b = 0.0462 +- 0.0015, \Omega_c = 0.233 +- 0.013,...
We obtain tight, simultaneous limits on the (constant) equation of state of dark energy and the spatial curvature of the universe: -0.11<1+w<0.14
<b>(95% CL)</b> and -0.0175<\Omega_k<0.0085 \text{(95% CL)}....
We find the limit on the total mass of massive neutrinos of \sum m_\nu
< 0.61
<b>eV</b>
\text{(95% CL)}, which is free from the uncertainty in the normalization of the large-scale structure data. The number of relativistic degrees of freedom, expressed in units of the effective number of neutrino species, is constrained as N_{\rm eff} = 4.4 +- 1.5 (68%), consistent with the standard value of 3.04.
[2-13]
Three-Year Wilkinson Microwave Anisotropy Probe (WMAP) Observations: Beam Profiles, Data Processing, Radiometer Characterization and Systematic Error Limits, N. Jarosik et al. (WMAP), Astrophys. J. Suppl. 170 (2007) 263, arXiv:astro-ph/0603452. http://lambda.gsfc.nasa.gov/product/map/dr2/pub_papers/threeyear/syserr/wmap_3yr_syserr.pdf.
[2-14]
Three-Year Wilkinson Microwave Anisotropy Probe (WMAP) Observations: Temperature Results, G. Hinshaw et al. (WMAP), Astrophys. J. Suppl. 170 (2007) 288, arXiv:astro-ph/0603451. http://lambda.gsfc.nasa.gov/product/map/dr2/pub_papers/threeyear/temperature/wmap_3yr_temp.pdf.
[2-15]
Three-Year Wilkinson Microwave Anisotropy Probe (WMAP) Observations: Polarization Analysis, L. Page et al. (WMAP), Astrophys. J. Suppl. 170 (2007) 335, arXiv:astro-ph/0603450. http://lambda.gsfc.nasa.gov/product/map/dr2/pub_papers/threeyear/polarization/wmap_3yr_pol.pdf.
[2-16]
Three-Year Wilkinson Microwave Anisotropy Probe (WMAP) Observations: Implications for Cosmology, D.N. Spergel et al. (WMAP), Astrophys. J. Suppl. 170 (2007) 377, arXiv:astro-ph/0603449. http://lambda.gsfc.nasa.gov/product/map/dr2/pub_papers/threeyear/parameters/wmap_3yr_param.pdf.
[2-17]
Three-Year Wilkinson Microwave Anisotropy Probe (WMAP) Observations: Three Year Explanatory Supplement, M. Limon et al. (WMAP), 2006. http://lambda.gsfc.nasa.gov/product/map/dr2/pub_papers/threeyear/supplement/wmap_3yr_supplement.pdf.
[2-18]
First Year Wilkinson Microwave Anisotropy Probe (WMAP) Observations: Implications for Inflation, Peiris, H. V. et al. (WMAP), Astrophys. J. Suppl. 148 (2003) 213, arXiv:astro-ph/0302225.
[2-19]
First Year Wilkinson Microwave Anisotropy Probe (WMAP) Observations: On-Orbit Radiometer Characterization, Jarosik, N. et al. (WMAP), Astrophys. J. Suppl. 148 (2003) 29, arXiv:astro-ph/0302224.
[2-20]
First Year Wilkinson Microwave Anisotropy Probe (WMAP) Observations: Tests of Gaussianity, Komatsu, E. et al. (WMAP), Astrophys. J. Suppl. 148 (2003) 119, arXiv:astro-ph/0302223.
[2-21]
First Year Wilkinson Microwave Anisotropy Probe (WMAP) Observations: Data Processing Methods and Systematic Errors Limits, Hinshaw, G. et al. (WMAP), Astrophys. J. Suppl. 148 (2003) 63, arXiv:astro-ph/0302222.
[2-22]
First Year Wilkinson Microwave Anisotropy Probe (WMAP) Observations: Interpretation of the TT and TE Angular Power Spectrum Peaks, Page, L. et al. (WMAP), Astrophys. J. Suppl. 148 (2003) 233, arXiv:astro-ph/0302220.
[2-23]
First Year Wilkinson Microwave Anisotropy Probe (WMAP) Observations: Parameter Estimation Methodology, Verde, L. et al. (WMAP), Astrophys. J. Suppl. 148 (2003) 195, arXiv:astro-ph/0302218.
[2-24]
First Year Wilkinson Microwave Anisotropy Probe (WMAP) Observations: Angular Power Spectrum, Hinshaw, G. et al. (WMAP), Astrophys. J. Suppl. 148 (2003) 135, arXiv:astro-ph/0302217.
[2-25]
First Year Wilkinson Microwave Anisotropy Probe (WMAP) Observations: Galactic Signal Contamination from Sidelobe Pickup, Barnes, C. et al. (WMAP), Astrophys. J. Suppl. 148 (2003) 51, arXiv:astro-ph/0302215.
[2-26]
First Year Wilkinson Microwave Anisotropy Probe (WMAP) Observations: Beam Profiles and Window Functions, Page, L. et al. (WMAP), Astrophys. J. Suppl. 148 (2003) 39, arXiv:astro-ph/0302214.
[2-27]
Wilkinson Microwave Anisotropy Probe (WMAP) First Year Observations: TE Polarization, Kogut, A. et al. (WMAP), Astrophys. J. Suppl. 148 (2003) 161, arXiv:astro-ph/0302213.
[2-28]
First Year Wilkinson Microwave Anisotropy Probe (WMAP) Observations: Determination of Cosmological Parameters, Spergel, D. N. et al. (WMAP), Astrophys. J. Supp. Ser. 148 (2003) 175-194, arXiv:astro-ph/0302209.
From the abstract: By combining WMAP data with other astronomical data sets, we constrain the geometry of the universe: \Omega_{tot} = 1.02 +- 0.02, the equation of state of the dark energy, w
< -0.78 (95% confidence limit), and the energy density in neutrinos, \Omega_\nu h^2
< 0.0076 (95% confidence limit). For 3 degenerate neutrino species, this limit implies that their mass is less than 0.23 eV (95% confidence limit). The WMAP detection of early reionization rules out warm dark matter.
[2-29]
First Year Wilkinson Microwave Anisotropy Probe (WMAP) Observations: Foreground Emission, Bennett, C. et al. (WMAP), Astrophys. J. Suppl. 148 (2003) 97, arXiv:astro-ph/0302208.
[2-30]
First Year Wilkinson Microwave Anisotropy Probe (WMAP) Observations: Preliminary Maps and Basic Results, Bennett, C. L. et al. (WMAP), Astrophys. J. Supp. Ser. 148 (2003) 1-27, arXiv:astro-ph/0302207.
From the abstract: A best-fit cosmological model to the CMB and other measures of large scale structure works remarkably well with only a few parameters. The age of the best-fit universe is t_0 = 13.7 +- 0.2
<b>
Gyr</b> old. Decoupling was t_{dec} = 379^{+ 8}_{- 7} \text{ kyr} after the Big Bang at a redshift of z_{dec} = 1089 +- 1. The thickness of the decoupling surface was \Delta z_{dec} = 195 +- 2. The matter density of the universe is \Omega_mh^2 = 0.135^{+ 0.008}_{- 0.009}, the baryon density is \Omega_bh^2 = 0.0224 +- 0.0009, and the total mass-energy of the universe is \Omega_{tot} = 1.02 +- 0.02.... This flat universe model is composed of 4.4% baryons, 22% dark matter and 73% dark energy.... Inflation theory is supported with n_s =~ 1, \Omega_{tot} =~ 1, Gaussian random phases of the CMB anisotropy, and superhorizon fluctuations implied by the TE anticorrelations at decoupling.
[2-31]
Design, Implementation and Testing of the MAP Radiometers, N. Jarosik et al., arXiv:astro-ph/0301164, 2003.
[2-32]
The Optical Design and Characterization of the Microwave Anisotropy Probe, L. Page et al., Astrophys. J. 585 (2003) 566, arXiv:astro-ph/0301160.
[2-33]
The MAP Satellite Feed Horns, C. Barnes et al., Astrophys. J. Supp. 143 (2002) 567, arXiv:astro-ph/0301159.
[2-34]
The Microwave Anisotropy Probe (MAP) Mission, C. L. Bennett et al. (WMAP), Astrophys. J. 583 (2003) 1, arXiv:astro-ph/0301158.
[2-35]
CMB Anisotropy Correlation Function and Topology from Simulated Maps for MAP, Park, Changbom et al., Astrophys. J. 506 (1998) 473-484, arXiv:astro-ph/9711057.


3 - Detector

[3-1]
First Year Wilkinson Microwave Anisotropy Probe (WMAP) Observations: Explanatory Supplement, M. Limon et al., 2003. http://lambda.gsfc.nasa.gov/product/map/pub_papers/firstyear/supplement/WMAP_supplement.pdf.


4 - Conference Proceedings

[4-1]
Comparing and combining Wilkinson Microwave Anisotropy (WMAP) probe results and Large Scale Structure, Licia verde, arXiv:astro-ph/0306272, 2003. Davis Inflation Meeting, 2003.
[4-2]
WMAP First Year Results, Wright, E. L., arXiv:astro-ph/0306132, 2003. The Cosmic Microwave Background and its Polarization, New Astronomy Reviews.
[4-3]
WMAP Polarization Results, A. Kogut, arXiv:astro-ph/0306048, 2003. "The Cosmic Microwave Background and its Polarization", New Astronomy Reviews.
[4-4]
Future Cosmic Microwave Background Experiments, Halpern, Mark, Scott, Douglas, arXiv:astro-ph/9904188, 1999. ASP, San Francisco, 1999.


Useful Links

LAMBDA, Legacy Archive for Microwave Background Data Analysis


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Authors:
Carlo Giunti / giunti@to.infn.it
Marco Laveder / marco.laveder@pd.infn.it
Last Update: Tue 15 May 2012, day 136 of the year 2012, 09:42:22 UTC