Hide metadata

dc.date.accessioned2023-09-15T16:38:21Z
dc.date.available2023-09-15T16:38:21Z
dc.date.created2023-09-01T11:08:38Z
dc.date.issued2023
dc.identifier.citationWatts, Duncan Galloway, Mathew Ihle, Håvard Tveit Andersen, Kristian Joten Aurvik, Ragnhild Banerji, Ranajoy Basyrov, Artem Bersanelli, M. Bertocco, S. Brilenkov, Maksym Carbone, M. Colombo, L.P.L. Eriksen, Hans Kristian Kamfjord Eskilt, Johannes Røsok Foss, Marie Kristine Franceschet, C. Fuskeland, Unni Galeotta, S. Gerakakis, S. Gjerløw, Eirik Hensley, B. Herman, Daniel Christopher Iacobellis, M. Ieronymaki, M. Jewell, J.B. Karakci, Ata Keihänen, Elina Keskitalo, R. Lunde, Jonas Gahr Sturtzel Maggio, G. Maino, D. Maris, M. Paradiso, S. Partridge, B. Reinecke, M. San, Metin Stutzer, Nils-Ole Suur-Uski, A.-S. Svalheim, Trygve Leithe Tavagnacco, D. Thommesen, Harald Wehus, Ingunn Kathrine Zacchei, A. . From BeyondPlanck to Cosmoglobe: Preliminary WMAP Q-band analysis. Astronomy and Astrophysics (A & A). 2023, 675
dc.identifier.urihttp://hdl.handle.net/10852/105053
dc.description.abstractWe present the first application of the C OSMOGLOBE analysis framework by analyzing nine-year WMAP time-ordered observations that uses similar machinery to that of B EYOND P LANCK for the Planck Low Frequency Instrument (LFI). We analyzed only the Q -band (41 GHz) data and report on the low-level analysis process based on uncalibrated time-ordered data to calibrated maps. Most of the existing B EYOND P LANCK pipeline may be reused for WMAP analysis with minimal changes to the existing codebase. The main modification is the implementation of the same preconditioned biconjugate gradient mapmaker used by the WMAP team. Producing a single WMAP Q 1-band sample requires 22 CPU-hrs, which is slightly more than the cost of a Planck 44 GHz sample of 17 CPU-hrs; this demonstrates that a full end-to-end Bayesian processing of the WMAP data is computationally feasible. In general, our recovered maps are very similar to the maps released by the WMAP team, although with two notable differences. In terms of temperature, we find a ∼2 μK quadrupole difference that most likely is caused by different gain modeling, while in polarization we find a distinct 2.5 μK signal that has been previously referred to as poorly measured modes by the WMAP team. In the C OSMOGLOBE processing, this pattern arises from temperature-to-polarization leakage from the coupling between the CMB Solar dipole, transmission imbalance, and sidelobes. No traces of this pattern are found in either the frequency map or TOD residual map, suggesting that the current processing has succeeded in modeling these poorly measured modes within the assumed parametric model by using Planck information to break the sky-synchronous degeneracies inherent in the WMAP scanning strategy.
dc.languageEN
dc.rightsAttribution 4.0 International
dc.rights.urihttps://creativecommons.org/licenses/by/4.0/
dc.titleFrom BeyondPlanck to Cosmoglobe: Preliminary WMAP Q-band analysis
dc.title.alternativeENEngelskEnglishFrom BeyondPlanck to Cosmoglobe: Preliminary WMAP Q-band analysis
dc.typeJournal article
dc.creator.authorWatts, Duncan
dc.creator.authorGalloway, Mathew
dc.creator.authorIhle, Håvard Tveit
dc.creator.authorAndersen, Kristian Joten
dc.creator.authorAurvik, Ragnhild
dc.creator.authorBanerji, Ranajoy
dc.creator.authorBasyrov, Artem
dc.creator.authorBersanelli, M.
dc.creator.authorBertocco, S.
dc.creator.authorBrilenkov, Maksym
dc.creator.authorCarbone, M.
dc.creator.authorColombo, L.P.L.
dc.creator.authorEriksen, Hans Kristian Kamfjord
dc.creator.authorEskilt, Johannes Røsok
dc.creator.authorFoss, Marie Kristine
dc.creator.authorFranceschet, C.
dc.creator.authorFuskeland, Unni
dc.creator.authorGaleotta, S.
dc.creator.authorGerakakis, S.
dc.creator.authorGjerløw, Eirik
dc.creator.authorHensley, B.
dc.creator.authorHerman, Daniel Christopher
dc.creator.authorIacobellis, M.
dc.creator.authorIeronymaki, M.
dc.creator.authorJewell, J.B.
dc.creator.authorKarakci, Ata
dc.creator.authorKeihänen, Elina
dc.creator.authorKeskitalo, R.
dc.creator.authorLunde, Jonas Gahr Sturtzel
dc.creator.authorMaggio, G.
dc.creator.authorMaino, D.
dc.creator.authorMaris, M.
dc.creator.authorParadiso, S.
dc.creator.authorPartridge, B.
dc.creator.authorReinecke, M.
dc.creator.authorSan, Metin
dc.creator.authorStutzer, Nils-Ole
dc.creator.authorSuur-Uski, A.-S.
dc.creator.authorSvalheim, Trygve Leithe
dc.creator.authorTavagnacco, D.
dc.creator.authorThommesen, Harald
dc.creator.authorWehus, Ingunn Kathrine
dc.creator.authorZacchei, A.
cristin.unitcode185,15,3,0
cristin.unitnameInstitutt for teoretisk astrofysikk
cristin.ispublishedtrue
cristin.fulltextoriginal
cristin.qualitycode2
dc.identifier.cristin2171595
dc.identifier.bibliographiccitationinfo:ofi/fmt:kev:mtx:ctx&ctx_ver=Z39.88-2004&rft_val_fmt=info:ofi/fmt:kev:mtx:journal&rft.jtitle=Astronomy and Astrophysics (A & A)&rft.volume=675&rft.spage=&rft.date=2023
dc.identifier.jtitleAstronomy and Astrophysics (A & A)
dc.identifier.volume675
dc.identifier.pagecount15
dc.identifier.doihttps://doi.org/10.1051/0004-6361/202243410
dc.subject.nviVDP::Astrofysikk, astronomi: 438
dc.type.documentTidsskriftartikkel
dc.type.peerreviewedPeer reviewed
dc.source.issn0004-6361
dc.type.versionPublishedVersion
cristin.articleidA16


Files in this item

Appears in the following Collection

Hide metadata

Attribution 4.0 International
This item's license is: Attribution 4.0 International