Asosiy kontentga oʻtish
Preprint

Euclid preparation XLVI. The Near-IR Background Dipole Experiment with Euclid

Euclid CollaborationA. KashlinskyDepartment of Astronomy, University of Maryland, College Park, MD, USARichard G. ArendtCenter for Space Sciences and Technology, University of Maryland, Baltimore County, Baltimore, MD, USAM. L. N. AshbyCenter for Astrophysics | Harvard \& Smithsonian, Cambridge, MA, USAF. Atrio‐BarandelaDepartamento de Física Fundamental. Universidad de Salamanca, Salamanca, SpainR. ScaramellaINFN-Sezione di Roma - c/o Dipartimento di Fisica, Roma, ItalyMichael A. StraussDepartment of Astrophysical Sciences, Princeton University, Princeton, NJ, USAB. AltieriESAC/ESA, Villanueva de la Cañada, Madrid, SpainA. AmaraSchool of Mathematics and Physics, University of Surrey, Guildford, Surrey, UKS. AndreonINAF-Osservatorio Astronomico di Brera, Milano, ItalyN. AuricchioOsservatorio di Astrofisica e Scienza dello SpazioMarco BaldiOsservatorio di Astrofisica e Scienza dello SpazioS. BardelliOsservatorio di Astrofisica e Scienza dello SpazioR. BenderUniversitäts-Sternwarte München, Fakultät für Physik, Ludwig-Maximilians-Universität München, München, GermanyC. BodendorfMax Planck Institute for Extraterrestrial Physics, Garching, GermanyE. BranchiniDipartimento di Fisica, Università di Genova, Genova, ItalyM. BresciaDepartment of Physics "E. Pancini", University Federico II, Napoli, ItalyJ. BrinchmannInstitute of Astrophysics and Space SciencesS. CameraINFN-Sezione di Torino, Torino, ItalyV. CapobiancoINAF-Osservatorio Astrofisico di Torino, Pino TorineseC. CarboneINAF-IASF Milano, Milano, ItalyJ. CarreteroInstitut de Física d'Altes EnergiesSantiago CasasM. CastellanoINAF-Osservatorio Astronomico di Roma, Monteporzio Catone, ItalyS. CavuotiINFN section of Naples, Napoli, ItalyA. CimattiDipartimento di Fisica e Astronomia "Augusto Righi" - Alma Mater Studiorum Università di Bologna, Bologna, ItalyG. CongedoInstitute for Astronomy, University of Edinburgh, Royal Observatory, Edinburgh, UKChristopher J. ConseliceJodrell Bank Centre for Astrophysics, Department of Physics and Astronomy, University of Manchester, Manchester, UKL. ConversiEuropean Space Agency/ESRIN, Frascati, Roma, ItalyY. CopinCentre National de la Recherche ScientifiqueL. CorcioneINAF-Osservatorio Astrofisico di Torino, Pino TorineseF. CourbinInstitute of Physics, Laboratory of Astrophysics, Ecole Polytechnique Fédérale de LausanneH. M. CourtoisInstitute of Nuclear Physics of LyonA. Da SilvaDepartamento de Física, Faculdade de Ciências, Universidade de Lisboa, Lisboa, PortugalH. DegaudenziDepartment of Astronomy, University of Geneva, Versoix, SwitzerlandA. M. Di GiorgioINAF-Istituto di Astrofisica e Planetologia Spaziali, Roma, ItalyJ. DinisDepartamento de Física, Faculdade de Ciências, Universidade de Lisboa, Lisboa, PortugalF. DubathDepartment of Astronomy, University of Geneva, Versoix, SwitzerlandX. DupacESAC/ESA, Villanueva de la Cañada, Madrid, SpainS. DusiniINFN-Padova, Padova, ItalyA. EaletUniv Claude Bernard Lyon 1, CNRS, IP2I Lyon, Villeurbanne, FranceM. FarinaINAF-Istituto di Astrofisica e Planetologia Spaziali, Roma, ItalyS. FarrensUniversité Paris-SaclayS. FerriolUniversity of Lyon, Univ Claude Bernard Lyon 1, CNRS/IN2P3, IP2I Lyon, Villeurbanne, FranceM. FrailisINAF-Osservatorio Astronomico di Trieste, Trieste, ItalyE. FranceschiINAF-Osservatorio di Astrofisica e Scienza dello Spazio di Bologna, Bologna, ItalyS. GaleottaINAF-Osservatorio Astronomico di Trieste, Trieste, ItalyB. GillisInstitute for Astronomy, University of Edinburgh, Royal Observatory, Edinburgh, UKC. GiocoliOsservatorio di Astrofisica e Scienza dello SpazioA. GrazianINAF-Osservatorio Astronomico di Padova, Padova, ItalyF. GruppUniversity Observatory, Faculty of Physics, Ludwig-Maximilians-Universität, Munich, GermanyS. V. H. HauganInstitute of Theoretical Astrophysics, University of Oslo, Blindern, Oslo, NorwayI. HookDepartment of Physics, Lancaster University, Lancaster, UKF. Hormuthvon Hoerner \& Sulger GmbH, Schwetzingen, GermanyA. HornstrupCosmic Dawn CenterK. JahnkęMax-Planck-Institut für Astronomie, Heidelberg, GermanyE. KeihänenHelsinki Institute of PhysicsS. KermicheAix-Marseille UniversitéA. KiesslingJet Propulsion Laboratory, California Institute of Technology, Pasadena, CA, USAM. KilbingerAstrophysique, Instrumentation et ModélisationB. KubikUniversity of Lyon, Univ Claude Bernard Lyon 1, CNRS/IN2P3, IP2I Lyon, Villeurbanne, FranceM. KunzUniversité de Genève, Département de Physique Théorique and Centre for Astroparticle Physics, Genève 4, SwitzerlandH. Kurki‐SuonioHelsinki Institute of Physics, University of Helsinki, Helsinki, FinlandS. LigoriINAF-Osservatorio Astrofisico di Torino, Pino TorineseP. B. LiljeInstitute of Theoretical Astrophysics, University of Oslo, Blindern, Oslo, NorwayV. LindholmDepartment of Physics, University of Helsinki, FinlandI. LloroNOVA optical infrared instrumentation group at ASTRON, Dwingeloo, The NetherlandsD. MainoINFN-Sezione di Milano, Milano, ItalyE. MaioranoINAF-Osservatorio di Astrofisica e Scienza dello Spazio di Bologna, Bologna, ItalyO. MansuttiINAF-Osservatorio Astronomico di Trieste, Trieste, ItalyO. MarggrafUniversität Bonn, Argelander-Institut für Astronomie, Bonn, GermanyK. MarkovičJet Propulsion Laboratory, California Institute of Technology, Pasadena, CA, USAN. MartinetAix-Marseille UniversitéF. MarulliUniversity of BolognaR. MasseyDepartment of Physics, Institute for Computational Cosmology, Durham University, South Road, UKS. MaurogordatoObservatoire de la Côte d’AzurH. J. McCrackenSorbonne UniversitéE. MedinaceliOsservatorio di Astrofisica e Scienza dello SpazioS. MeiUniversité Paris CitéY. MellierInstitut d'Astrophysique de Paris, Paris, FranceM. MeneghettiOsservatorio di Astrofisica e Scienza dello SpazioG. MeylanInstitute of Physics, Laboratory of Astrophysics, Ecole Polytechnique Fédérale de LausanneM. MorescoINAF-Osservatorio di Astrofisica e Scienza dello Spazio di Bologna, Bologna, ItalyL. MoscardiniUniversity of BolognaE. MunariINAF-Osservatorio Astronomico di Trieste, Trieste, ItalyS. -M. NiemiEuropean Space Agency/ESTEC, Noordwijk, The NetherlandsPadilla, C.Institut de Física d'Altes EnergiesS. PaltaniDepartment of Astronomy, University of Geneva, Versoix, SwitzerlandF. PasianINAF-Osservatorio Astronomico di Trieste, Trieste, ItalyK. PedersenDepartment of Physics and Astronomy, University of Aarhus, Aarhus C, DenmarkWill J. PercivalDepartment of Physics and Astronomy, University of Waterloo, Waterloo, Ontario, CanadaS. PiresAstrophysique, Instrumentation et ModélisationG. PolentaSpace Science Data Center, Italian Space Agency, Roma, ItalyM. PoncetCentre National d'Etudes Spatiales -- Centre spatial de Toulouse, Toulouse Cedex 9, FranceL. A. PopaInstitute of Space Science, Ilfov, RomaniaF. RaisonMax Planck Institute for Extraterrestrial Physics, Garching, GermanyA. RenziDipartimento di Fisica e Astronomia "G. Galilei", Università di Padova, Padova, ItalyJ. RhodesJet Propulsion Laboratory, California Institute of Technology, Pasadena, CA, USAG. RiccioINAF-Osservatorio Astronomico di Capodimonte, Napoli, ItalyE. RomelliINAF-Osservatorio Astronomico di Trieste, Trieste, Italy
arXiv (Cornell University)repository2024en
ABI

Annotatsiya

Verifying the fully kinematic nature of the cosmic microwave background (CMB) dipole is of fundamental importance in cosmology. In the standard cosmological model with the Friedman-Lemaitre-Robertson-Walker (FLRW) metric from the inflationary expansion the CMB dipole should be entirely kinematic. Any non-kinematic CMB dipole component would thus reflect the preinflationary structure of spacetime probing the extent of the FLRW applicability. Cosmic backgrounds from galaxies after the matter-radiation decoupling, should have kinematic dipole component identical in velocity with the CMB kinematic dipole. Comparing the two can lead to isolating the CMB non-kinematic dipole. It was recently proposed that such measurement can be done using the near-IR cosmic infrared background (CIB) measured with the currently operating Euclid telescope, and later with Roman. The proposed method reconstructs the resolved CIB, the Integrated Galaxy Light (IGL), from Euclid's Wide Survey and probes its dipole, with a kinematic component amplified over that of the CMB by the Compton-Getting effect. The amplification coupled with the extensive galaxy samples forming the IGL would determine the CIB dipole with an overwhelming signal/noise, isolating its direction to sub-degree accuracy. We develop details of the method for Euclid's Wide Survey in 4 bands spanning 0.6 to 2 mic. We isolate the systematic and other uncertainties and present methodologies to minimize them, after confining the sample to the magnitude range with negligible IGL/CIB dipole from galaxy clustering. These include the required star-galaxy separation, accounting for the extinction correction dipole using the method newly developed here achieving total separation, accounting for the Earth's orbital motion and other systematic effects. (Abridged)

Hali tarjima qilinmagan

Mavzular

Identifikatorlar

Iqtiboslar va manbalar

0 ta iqtibos0 ta foydalanilgan manba