Constraints on Cosmological Parameters from the 500 deg 2 SPTPOL Lensing Power Spectrum
We present cosmological constraints based on the cosmic microwave background (CMB) lensing potential power spectrum measurement from the recent 500 deg 2 SPTpol survey, the most precise CMB lensing measurement from the ground to date. We fit a flat ΛCDM model to the reconstructed lensing power spect...
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creator | Bianchini, F. Wu, W. L. K. Ade, P. A. R. Anderson, A. J. Austermann, J. E. Avva, J. S. Beall, J. A. Bender, A. N. Benson, B. A. Bleem, L. E. Carlstrom, J. E. Chang, C. L. Chaubal, P. Chiang, H. C. Citron, R. Moran, C. Corbett Crawford, T. M. Crites, A. T. de Haan, T. Dobbs, M. A. Everett, W. Gallicchio, J. George, E. M. Gilbert, A. Gupta, N. Halverson, N. W. Harrington, N. Henning, J. W. Hilton, G. C. Holder, G. P. Holzapfel, W. L. Hrubes, J. D. Huang, N. Hubmayr, J. Irwin, K. D. Knox, L. Lee, A. T. Li, D. Lowitz, A. Manzotti, A. McMahon, J. J. Meyer, S. S. Millea, M. Mocanu, L. M. Montgomery, J. Nadolski, A. Natoli, T. Nibarger, J. P. Noble, G. Novosad, V. Omori, Y. Padin, S. Patil, S. Pryke, C. Reichardt, C. L. Ruhl, J. E. Saliwanchik, B. R. Sayre, J. T. Schaffer, K. K. Sievers, C. Simard, G. Smecher, G. Stark, A. A. Story, K. T. Tucker, C. Vanderlinde, K. Veach, T. Vieira, J. D. Wang, G. Whitehorn, N. Yefremenko, V. |
description | We present cosmological constraints based on the cosmic microwave background (CMB) lensing potential power spectrum measurement from the recent 500 deg
2
SPTpol
survey, the most precise CMB lensing measurement from the ground to date. We fit a flat ΛCDM model to the reconstructed lensing power spectrum alone and in addition with other data sets: baryon acoustic oscillations (BAO), as well as primary CMB spectra from
Planck
and
SPTpol
. The cosmological constraints based on
SPTpol
and
Planck
lensing band powers are in good agreement when analyzed alone and in combination with
Planck
full-sky primary CMB data. With weak priors on the baryon density and other parameters, the
SPTpol
CMB lensing data alone provide a 4% constraint on
. Jointly fitting with BAO data, we find
,
, and
, up to
away from the central values preferred by
Planck
lensing + BAO. However, we recover good agreement between
SPTpol
and
Planck
when restricting the analysis to similar scales. We also consider single-parameter extensions to the flat ΛCDM model. The
SPTpol
lensing spectrum constrains the spatial curvature to be
and the sum of the neutrino masses to be
eV at 95% C.L. (with
Planck
primary CMB and BAO data), in good agreement with the
Planck
lensing results. With the differences in the signal-to-noise ratio of the lensing modes and the angular scales covered in the lensing spectra, this analysis represents an important independent check on the full-sky
Planck
lensing measurement. |
doi_str_mv | 10.3847/1538-4357/ab6082 |
format | Article |
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2
SPTpol
survey, the most precise CMB lensing measurement from the ground to date. We fit a flat ΛCDM model to the reconstructed lensing power spectrum alone and in addition with other data sets: baryon acoustic oscillations (BAO), as well as primary CMB spectra from
Planck
and
SPTpol
. The cosmological constraints based on
SPTpol
and
Planck
lensing band powers are in good agreement when analyzed alone and in combination with
Planck
full-sky primary CMB data. With weak priors on the baryon density and other parameters, the
SPTpol
CMB lensing data alone provide a 4% constraint on
. Jointly fitting with BAO data, we find
,
, and
, up to
away from the central values preferred by
Planck
lensing + BAO. However, we recover good agreement between
SPTpol
and
Planck
when restricting the analysis to similar scales. We also consider single-parameter extensions to the flat ΛCDM model. The
SPTpol
lensing spectrum constrains the spatial curvature to be
and the sum of the neutrino masses to be
eV at 95% C.L. (with
Planck
primary CMB and BAO data), in good agreement with the
Planck
lensing results. With the differences in the signal-to-noise ratio of the lensing modes and the angular scales covered in the lensing spectra, this analysis represents an important independent check on the full-sky
Planck
lensing measurement.</description><identifier>ISSN: 0004-637X</identifier><identifier>EISSN: 1538-4357</identifier><identifier>DOI: 10.3847/1538-4357/ab6082</identifier><language>eng</language><publisher>American Astronomical Society</publisher><subject>Astrophysics ; Physics</subject><ispartof>The Astrophysical journal, 2020-01, Vol.888 (2), p.119</ispartof><rights>Distributed under a Creative Commons Attribution 4.0 International License</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c1221-6cc92fd64e59aaff02739b13688e90f5551281f88f3e6e18f2399b58c2948173</citedby><cites>FETCH-LOGICAL-c1221-6cc92fd64e59aaff02739b13688e90f5551281f88f3e6e18f2399b58c2948173</cites><orcidid>0000-0003-4847-3483 ; 0000-0001-5871-7520 ; 0000-0002-2718-9996 ; 0000-0003-2226-9169 ; 0000-0001-7665-5079 ; 0000-0001-5105-9473 ; 0000-0002-5108-6823 ; 0000-0001-5411-6920 ; 0000-0001-9000-5013 ; 0000-0001-5800-3990 ; 0000-0002-0463-6394 ; 0000-0002-3157-0407 ; 0000-0003-0057-877X ; 0000-0002-5127-0401 ; 0000-0001-8599-7249 ; 0000-0001-7547-4241</orcidid></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>230,314,776,780,881,27901,27902</link.rule.ids><backlink>$$Uhttps://hal.science/hal-02350168$$DView record in HAL$$Hfree_for_read</backlink></links><search><creatorcontrib>Bianchini, F.</creatorcontrib><creatorcontrib>Wu, W. L. K.</creatorcontrib><creatorcontrib>Ade, P. A. R.</creatorcontrib><creatorcontrib>Anderson, A. J.</creatorcontrib><creatorcontrib>Austermann, J. E.</creatorcontrib><creatorcontrib>Avva, J. S.</creatorcontrib><creatorcontrib>Beall, J. A.</creatorcontrib><creatorcontrib>Bender, A. N.</creatorcontrib><creatorcontrib>Benson, B. A.</creatorcontrib><creatorcontrib>Bleem, L. E.</creatorcontrib><creatorcontrib>Carlstrom, J. E.</creatorcontrib><creatorcontrib>Chang, C. L.</creatorcontrib><creatorcontrib>Chaubal, P.</creatorcontrib><creatorcontrib>Chiang, H. C.</creatorcontrib><creatorcontrib>Citron, R.</creatorcontrib><creatorcontrib>Moran, C. Corbett</creatorcontrib><creatorcontrib>Crawford, T. M.</creatorcontrib><creatorcontrib>Crites, A. T.</creatorcontrib><creatorcontrib>de Haan, T.</creatorcontrib><creatorcontrib>Dobbs, M. A.</creatorcontrib><creatorcontrib>Everett, W.</creatorcontrib><creatorcontrib>Gallicchio, J.</creatorcontrib><creatorcontrib>George, E. M.</creatorcontrib><creatorcontrib>Gilbert, A.</creatorcontrib><creatorcontrib>Gupta, N.</creatorcontrib><creatorcontrib>Halverson, N. W.</creatorcontrib><creatorcontrib>Harrington, N.</creatorcontrib><creatorcontrib>Henning, J. W.</creatorcontrib><creatorcontrib>Hilton, G. C.</creatorcontrib><creatorcontrib>Holder, G. P.</creatorcontrib><creatorcontrib>Holzapfel, W. L.</creatorcontrib><creatorcontrib>Hrubes, J. D.</creatorcontrib><creatorcontrib>Huang, N.</creatorcontrib><creatorcontrib>Hubmayr, J.</creatorcontrib><creatorcontrib>Irwin, K. D.</creatorcontrib><creatorcontrib>Knox, L.</creatorcontrib><creatorcontrib>Lee, A. T.</creatorcontrib><creatorcontrib>Li, D.</creatorcontrib><creatorcontrib>Lowitz, A.</creatorcontrib><creatorcontrib>Manzotti, A.</creatorcontrib><creatorcontrib>McMahon, J. J.</creatorcontrib><creatorcontrib>Meyer, S. S.</creatorcontrib><creatorcontrib>Millea, M.</creatorcontrib><creatorcontrib>Mocanu, L. M.</creatorcontrib><creatorcontrib>Montgomery, J.</creatorcontrib><creatorcontrib>Nadolski, A.</creatorcontrib><creatorcontrib>Natoli, T.</creatorcontrib><creatorcontrib>Nibarger, J. P.</creatorcontrib><creatorcontrib>Noble, G.</creatorcontrib><creatorcontrib>Novosad, V.</creatorcontrib><creatorcontrib>Omori, Y.</creatorcontrib><creatorcontrib>Padin, S.</creatorcontrib><creatorcontrib>Patil, S.</creatorcontrib><creatorcontrib>Pryke, C.</creatorcontrib><creatorcontrib>Reichardt, C. L.</creatorcontrib><creatorcontrib>Ruhl, J. E.</creatorcontrib><creatorcontrib>Saliwanchik, B. R.</creatorcontrib><creatorcontrib>Sayre, J. T.</creatorcontrib><creatorcontrib>Schaffer, K. K.</creatorcontrib><creatorcontrib>Sievers, C.</creatorcontrib><creatorcontrib>Simard, G.</creatorcontrib><creatorcontrib>Smecher, G.</creatorcontrib><creatorcontrib>Stark, A. A.</creatorcontrib><creatorcontrib>Story, K. T.</creatorcontrib><creatorcontrib>Tucker, C.</creatorcontrib><creatorcontrib>Vanderlinde, K.</creatorcontrib><creatorcontrib>Veach, T.</creatorcontrib><creatorcontrib>Vieira, J. D.</creatorcontrib><creatorcontrib>Wang, G.</creatorcontrib><creatorcontrib>Whitehorn, N.</creatorcontrib><creatorcontrib>Yefremenko, V.</creatorcontrib><title>Constraints on Cosmological Parameters from the 500 deg 2 SPTPOL Lensing Power Spectrum</title><title>The Astrophysical journal</title><description>We present cosmological constraints based on the cosmic microwave background (CMB) lensing potential power spectrum measurement from the recent 500 deg
2
SPTpol
survey, the most precise CMB lensing measurement from the ground to date. We fit a flat ΛCDM model to the reconstructed lensing power spectrum alone and in addition with other data sets: baryon acoustic oscillations (BAO), as well as primary CMB spectra from
Planck
and
SPTpol
. The cosmological constraints based on
SPTpol
and
Planck
lensing band powers are in good agreement when analyzed alone and in combination with
Planck
full-sky primary CMB data. With weak priors on the baryon density and other parameters, the
SPTpol
CMB lensing data alone provide a 4% constraint on
. Jointly fitting with BAO data, we find
,
, and
, up to
away from the central values preferred by
Planck
lensing + BAO. However, we recover good agreement between
SPTpol
and
Planck
when restricting the analysis to similar scales. We also consider single-parameter extensions to the flat ΛCDM model. The
SPTpol
lensing spectrum constrains the spatial curvature to be
and the sum of the neutrino masses to be
eV at 95% C.L. (with
Planck
primary CMB and BAO data), in good agreement with the
Planck
lensing results. With the differences in the signal-to-noise ratio of the lensing modes and the angular scales covered in the lensing spectra, this analysis represents an important independent check on the full-sky
Planck
lensing measurement.</description><subject>Astrophysics</subject><subject>Physics</subject><issn>0004-637X</issn><issn>1538-4357</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2020</creationdate><recordtype>article</recordtype><recordid>eNo9kMFLwzAYxYMoOKd3j7l6qPuSNGlyHEWdUFhhA72FLEu2StuMpCr-91oqOz3e4713-CF0T-CRybxYEM5kljNeLMxOgKQXaHaOLtEMAPJMsOL9Gt2k9DFaqtQMvZWhT0M0TT8kHHpchtSFNhwaa1pcm2g6N7iYsI-hw8PRYQ6A9-6AKd7U23pd4cr1qekPuA7fLuLNydkhfna36MqbNrm7f52j7fPTtlxl1frltVxWmSWUkkxYq6jfi9xxZYz3QAumdoQJKZ0CzzknVBIvpWdOOCI9ZUrtuLRU5ZIUbI4eptujafUpNp2JPzqYRq-WlR4zoIwDEfKL_HVh6toYUorOnwcE9MhQj8D0CExPDNkvNBhiPg</recordid><startdate>20200110</startdate><enddate>20200110</enddate><creator>Bianchini, F.</creator><creator>Wu, W. L. K.</creator><creator>Ade, P. A. R.</creator><creator>Anderson, A. J.</creator><creator>Austermann, J. E.</creator><creator>Avva, J. S.</creator><creator>Beall, J. A.</creator><creator>Bender, A. N.</creator><creator>Benson, B. 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L. K. ; Ade, P. A. R. ; Anderson, A. J. ; Austermann, J. E. ; Avva, J. S. ; Beall, J. A. ; Bender, A. N. ; Benson, B. A. ; Bleem, L. E. ; Carlstrom, J. E. ; Chang, C. L. ; Chaubal, P. ; Chiang, H. C. ; Citron, R. ; Moran, C. Corbett ; Crawford, T. M. ; Crites, A. T. ; de Haan, T. ; Dobbs, M. A. ; Everett, W. ; Gallicchio, J. ; George, E. M. ; Gilbert, A. ; Gupta, N. ; Halverson, N. W. ; Harrington, N. ; Henning, J. W. ; Hilton, G. C. ; Holder, G. P. ; Holzapfel, W. L. ; Hrubes, J. D. ; Huang, N. ; Hubmayr, J. ; Irwin, K. D. ; Knox, L. ; Lee, A. T. ; Li, D. ; Lowitz, A. ; Manzotti, A. ; McMahon, J. J. ; Meyer, S. S. ; Millea, M. ; Mocanu, L. M. ; Montgomery, J. ; Nadolski, A. ; Natoli, T. ; Nibarger, J. P. ; Noble, G. ; Novosad, V. ; Omori, Y. ; Padin, S. ; Patil, S. ; Pryke, C. ; Reichardt, C. L. ; Ruhl, J. E. ; Saliwanchik, B. R. ; Sayre, J. T. ; Schaffer, K. K. ; Sievers, C. ; Simard, G. ; Smecher, G. ; Stark, A. A. ; Story, K. T. ; Tucker, C. ; Vanderlinde, K. ; Veach, T. ; Vieira, J. D. ; Wang, G. ; Whitehorn, N. ; Yefremenko, V.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c1221-6cc92fd64e59aaff02739b13688e90f5551281f88f3e6e18f2399b58c2948173</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2020</creationdate><topic>Astrophysics</topic><topic>Physics</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Bianchini, F.</creatorcontrib><creatorcontrib>Wu, W. L. K.</creatorcontrib><creatorcontrib>Ade, P. A. R.</creatorcontrib><creatorcontrib>Anderson, A. J.</creatorcontrib><creatorcontrib>Austermann, J. E.</creatorcontrib><creatorcontrib>Avva, J. S.</creatorcontrib><creatorcontrib>Beall, J. A.</creatorcontrib><creatorcontrib>Bender, A. N.</creatorcontrib><creatorcontrib>Benson, B. A.</creatorcontrib><creatorcontrib>Bleem, L. E.</creatorcontrib><creatorcontrib>Carlstrom, J. 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D.</creatorcontrib><creatorcontrib>Huang, N.</creatorcontrib><creatorcontrib>Hubmayr, J.</creatorcontrib><creatorcontrib>Irwin, K. D.</creatorcontrib><creatorcontrib>Knox, L.</creatorcontrib><creatorcontrib>Lee, A. T.</creatorcontrib><creatorcontrib>Li, D.</creatorcontrib><creatorcontrib>Lowitz, A.</creatorcontrib><creatorcontrib>Manzotti, A.</creatorcontrib><creatorcontrib>McMahon, J. J.</creatorcontrib><creatorcontrib>Meyer, S. S.</creatorcontrib><creatorcontrib>Millea, M.</creatorcontrib><creatorcontrib>Mocanu, L. M.</creatorcontrib><creatorcontrib>Montgomery, J.</creatorcontrib><creatorcontrib>Nadolski, A.</creatorcontrib><creatorcontrib>Natoli, T.</creatorcontrib><creatorcontrib>Nibarger, J. P.</creatorcontrib><creatorcontrib>Noble, G.</creatorcontrib><creatorcontrib>Novosad, V.</creatorcontrib><creatorcontrib>Omori, Y.</creatorcontrib><creatorcontrib>Padin, S.</creatorcontrib><creatorcontrib>Patil, S.</creatorcontrib><creatorcontrib>Pryke, C.</creatorcontrib><creatorcontrib>Reichardt, C. L.</creatorcontrib><creatorcontrib>Ruhl, J. E.</creatorcontrib><creatorcontrib>Saliwanchik, B. R.</creatorcontrib><creatorcontrib>Sayre, J. T.</creatorcontrib><creatorcontrib>Schaffer, K. K.</creatorcontrib><creatorcontrib>Sievers, C.</creatorcontrib><creatorcontrib>Simard, G.</creatorcontrib><creatorcontrib>Smecher, G.</creatorcontrib><creatorcontrib>Stark, A. A.</creatorcontrib><creatorcontrib>Story, K. T.</creatorcontrib><creatorcontrib>Tucker, C.</creatorcontrib><creatorcontrib>Vanderlinde, K.</creatorcontrib><creatorcontrib>Veach, T.</creatorcontrib><creatorcontrib>Vieira, J. D.</creatorcontrib><creatorcontrib>Wang, G.</creatorcontrib><creatorcontrib>Whitehorn, N.</creatorcontrib><creatorcontrib>Yefremenko, V.</creatorcontrib><collection>CrossRef</collection><collection>Hyper Article en Ligne (HAL)</collection><jtitle>The Astrophysical journal</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Bianchini, F.</au><au>Wu, W. L. K.</au><au>Ade, P. A. R.</au><au>Anderson, A. J.</au><au>Austermann, J. E.</au><au>Avva, J. S.</au><au>Beall, J. A.</au><au>Bender, A. N.</au><au>Benson, B. A.</au><au>Bleem, L. E.</au><au>Carlstrom, J. E.</au><au>Chang, C. L.</au><au>Chaubal, P.</au><au>Chiang, H. C.</au><au>Citron, R.</au><au>Moran, C. Corbett</au><au>Crawford, T. M.</au><au>Crites, A. T.</au><au>de Haan, T.</au><au>Dobbs, M. A.</au><au>Everett, W.</au><au>Gallicchio, J.</au><au>George, E. M.</au><au>Gilbert, A.</au><au>Gupta, N.</au><au>Halverson, N. W.</au><au>Harrington, N.</au><au>Henning, J. W.</au><au>Hilton, G. C.</au><au>Holder, G. P.</au><au>Holzapfel, W. L.</au><au>Hrubes, J. D.</au><au>Huang, N.</au><au>Hubmayr, J.</au><au>Irwin, K. D.</au><au>Knox, L.</au><au>Lee, A. T.</au><au>Li, D.</au><au>Lowitz, A.</au><au>Manzotti, A.</au><au>McMahon, J. J.</au><au>Meyer, S. S.</au><au>Millea, M.</au><au>Mocanu, L. M.</au><au>Montgomery, J.</au><au>Nadolski, A.</au><au>Natoli, T.</au><au>Nibarger, J. P.</au><au>Noble, G.</au><au>Novosad, V.</au><au>Omori, Y.</au><au>Padin, S.</au><au>Patil, S.</au><au>Pryke, C.</au><au>Reichardt, C. L.</au><au>Ruhl, J. E.</au><au>Saliwanchik, B. R.</au><au>Sayre, J. T.</au><au>Schaffer, K. K.</au><au>Sievers, C.</au><au>Simard, G.</au><au>Smecher, G.</au><au>Stark, A. A.</au><au>Story, K. T.</au><au>Tucker, C.</au><au>Vanderlinde, K.</au><au>Veach, T.</au><au>Vieira, J. D.</au><au>Wang, G.</au><au>Whitehorn, N.</au><au>Yefremenko, V.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Constraints on Cosmological Parameters from the 500 deg 2 SPTPOL Lensing Power Spectrum</atitle><jtitle>The Astrophysical journal</jtitle><date>2020-01-10</date><risdate>2020</risdate><volume>888</volume><issue>2</issue><spage>119</spage><pages>119-</pages><issn>0004-637X</issn><eissn>1538-4357</eissn><abstract>We present cosmological constraints based on the cosmic microwave background (CMB) lensing potential power spectrum measurement from the recent 500 deg
2
SPTpol
survey, the most precise CMB lensing measurement from the ground to date. We fit a flat ΛCDM model to the reconstructed lensing power spectrum alone and in addition with other data sets: baryon acoustic oscillations (BAO), as well as primary CMB spectra from
Planck
and
SPTpol
. The cosmological constraints based on
SPTpol
and
Planck
lensing band powers are in good agreement when analyzed alone and in combination with
Planck
full-sky primary CMB data. With weak priors on the baryon density and other parameters, the
SPTpol
CMB lensing data alone provide a 4% constraint on
. Jointly fitting with BAO data, we find
,
, and
, up to
away from the central values preferred by
Planck
lensing + BAO. However, we recover good agreement between
SPTpol
and
Planck
when restricting the analysis to similar scales. We also consider single-parameter extensions to the flat ΛCDM model. The
SPTpol
lensing spectrum constrains the spatial curvature to be
and the sum of the neutrino masses to be
eV at 95% C.L. (with
Planck
primary CMB and BAO data), in good agreement with the
Planck
lensing results. With the differences in the signal-to-noise ratio of the lensing modes and the angular scales covered in the lensing spectra, this analysis represents an important independent check on the full-sky
Planck
lensing measurement.</abstract><pub>American Astronomical Society</pub><doi>10.3847/1538-4357/ab6082</doi><orcidid>https://orcid.org/0000-0003-4847-3483</orcidid><orcidid>https://orcid.org/0000-0001-5871-7520</orcidid><orcidid>https://orcid.org/0000-0002-2718-9996</orcidid><orcidid>https://orcid.org/0000-0003-2226-9169</orcidid><orcidid>https://orcid.org/0000-0001-7665-5079</orcidid><orcidid>https://orcid.org/0000-0001-5105-9473</orcidid><orcidid>https://orcid.org/0000-0002-5108-6823</orcidid><orcidid>https://orcid.org/0000-0001-5411-6920</orcidid><orcidid>https://orcid.org/0000-0001-9000-5013</orcidid><orcidid>https://orcid.org/0000-0001-5800-3990</orcidid><orcidid>https://orcid.org/0000-0002-0463-6394</orcidid><orcidid>https://orcid.org/0000-0002-3157-0407</orcidid><orcidid>https://orcid.org/0000-0003-0057-877X</orcidid><orcidid>https://orcid.org/0000-0002-5127-0401</orcidid><orcidid>https://orcid.org/0000-0001-8599-7249</orcidid><orcidid>https://orcid.org/0000-0001-7547-4241</orcidid></addata></record> |
fulltext | fulltext |
identifier | ISSN: 0004-637X |
ispartof | The Astrophysical journal, 2020-01, Vol.888 (2), p.119 |
issn | 0004-637X 1538-4357 |
language | eng |
recordid | cdi_hal_primary_oai_HAL_hal_02350168v1 |
source | IOP Publishing Free Content; Elektronische Zeitschriftenbibliothek - Frei zugängliche E-Journals; Alma/SFX Local Collection |
subjects | Astrophysics Physics |
title | Constraints on Cosmological Parameters from the 500 deg 2 SPTPOL Lensing Power Spectrum |
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