Euclid preparation: I. The Euclid Wide Survey

preprint2021arXivOpen access
R. ScaramellaJ. AmiauxY. MellierC. BuriganaC. S. CarvalhoJ. -C. CuillandreA. Da SilvaA. DerosaJ. DinisE. MaioranoM. MarisI. TerenoR. LaureijsT. BoenkeG. BuenadichaX. DupacL. M. Gaspar VenancioP. Gómez-ÁlvarezJ. HoarJ. Lorenzo AlvarezG. D. RaccaG. Saavedra-CriadoJ. SchwartzR. VavrekM. SchirmerH. AusselR. AzzolliniV. F. CardoneM. CropperA. EaletB. GarilliW. GillardB. R. GranettL. GuzzoH. HoekstraK. JahnkeT. KitchingM. MeneghettiL. MillerR. NakajimaS. M. NiemiF. PasianW. J. PercivalM. SauvageM. ScodeggioS. WachterA. ZaccheiN. AghanimA. AmaraT. AuphanN. AuricchioS. AwanA. BalestraR. BenderC. BodendorfD. BoninoE. BranchiniS. Brau-NogueM. BresciaG. P. CandiniV. CapobiancoC. CarboneR. G. CarlbergJ. CarreteroR. CasasF. J. CastanderM. CastellanoS. CavuotiA. CimattiR. CledassouG. CongedoC. J. ConseliceL. ConversiY. CopinL. CorcioneA. CostilleF. CourbinH. DegaudenziM. DouspisF. DubathC. A. J. DuncanS. DusiniS. FarrensS. FerriolP. FosalbaN. FourmanoitM. FrailisE. FranceschiP. FranzettiM. FumanaB. GillisC. GiocoliA. GrazianF. GruppS. V. H. HauganW. HolmesF. HormuthP. HudelotS. KermicheA. KiesslingM. KilbingerR. KohleyB. KubikM. KümmelM. KunzH. Kurki-SuonioS. LigoriP. B. LiljeI. LloroO. MansuttiO. MarggrafK. MarkovicF. MarulliR. MasseyS. MaurogordatoM. MelchiorE. MerlinG. MeylanJ. J. MohrM. MorescoB. MorinL. MoscardiniE. MunariR. C. NicholC. PadillaS. PaltaniJ. PeacockK. PedersenV. PettorinoS. PiresM. PoncetL. PopaL. PozzettiF. RaisonR. ReboloJ. RhodesH. -W. RixM. RoncarelliE. RossettiR. SagliaP. SchneiderT. SchrabbackA. SecrounG. SeidelS. SerranoC. SirignanoG. SirriJ. SkottfeltL. StancoJ. L. StarckP. Tallada-CrespíD. TavagnaccoA. N. TaylorH. I. TeplitzR. Toledo-MoreoF. TorradeflotM. TrifoglioE. A. ValentijnL. ValenzianoG. A. Verdoes KleijnY. WangN. WelikalaJ. WellerM. WetzsteinG. ZamoraniJ. ZoubianS. AndreonM. BaldiS. BardelliA. BoucaudS. CameraG. FabbianR. FarinelliJ. Graciá-CarpioD. MainoE. MedinaceliS. MeiC. NeissnerG. PolentaA. RenziE. RomelliC. RossetF. SureauM. TentiT. VassalloE. ZuccaC. BaccigalupiA. Balaguera-AntolínezP. BattagliaA. BivianoS. BorganiE. BozzoR. CabanacA. CappiS. CasasG. CastignaniC. Colodro-CondeJ. CouponH. M. CourtoisJ. CubyS. de la TorreS. DesaiD. Di FerdinandoH. DoleM. FabriciusM. FarinaP. G. FerreiraF. FinelliP. Flose-ReimbergS. FotopoulouS. GaleottaK. GangaG. GozaliaslI. M. HookE. KeihanenC. C. KirkpatrickP. LiebingV. LindholmG. MainettiM. MartinelliN. MartinetM. MaturiH. J. McCrackenR. B. MetcalfG. MorganteJ. NightingaleA. NucitaL. PatriziiD. PotterG. RiccioA. G. SánchezD. SaponeJ. A. SchewtschenkoM. SchultheisV. ScottezR. TeyssierI. TutusausJ. ValiviitaM. VielW. VriendL. Whittaker

Abstract

Euclid is an ESA mission designed to constrain the properties of dark energy and gravity via weak gravitational lensing and galaxy clustering. It will carry out a wide area imaging and spectroscopy survey (EWS) in visible and near-infrared, covering roughly 15,000 square degrees of extragalactic sky on six years. The wide-field telescope and instruments are optimized for pristine PSF and reduced straylight, producing very crisp images. This paper presents the building of the Euclid reference survey: the sequence of pointings of EWS, Deep fields, Auxiliary fields for calibrations, and spacecraft movements followed by Euclid as it operates in a step-and-stare mode from its orbit around the Lagrange point L2. Each EWS pointing has four dithered frames; we simulate the dither pattern at pixel level to analyse the effective coverage. We use up-to-date models for the sky background to define the Euclid region-of-interest (RoI). The building of the reference survey is highly constrained from calibration cadences, spacecraft constraints and background levels; synergies with ground-based coverage are also considered. Via purposely-built software optimized to prioritize best sky areas, produce a compact coverage, and ensure thermal stability, we generate a schedule for the Auxiliary and Deep fields observations and schedule the RoI with EWS transit observations. The resulting reference survey RSD_2021A fulfills all constraints and is a good proxy for the final solution. Its wide survey covers 14,500 square degrees. The limiting AB magnitudes (5σ5σ point-like source) achieved in its footprint are estimated to be 26.2 (visible) and 24.5 (near-infrared); for spectroscopy, the Hα_α line flux limit is 2×10−162\times 10^{-16} erg cm−2^{-2} s−1^{-1} at 1600 nm; and for diffuse emission the surface brightness limits are 29.8 (visible) and 28.4 (near-infrared) mag arcsec−2^{-2}.

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