Euclidpreparation

Astronomy & Astrophysics EDP Sciences 657 (2021) A90-A90

Authors:

H Bretonnière, M Huertas-Company, A Boucaud, F Lanusse, E Jullo, E Merlin, D Tuccillo, M Castellano, J Brinchmann, CJ Conselice, H Dole, R Cabanac, HM Courtois, FJ Castander, PA Duc, P Fosalba, D Guinet, S Kruk, U Kuchner, S Serrano, E Soubrie, A Tramacere, L Wang, A Amara, N Auricchio, CAJ Duncan

Abstract:

We present a machine learning framework to simulate realistic galaxies for the Euclid Survey, producing more complex and realistic galaxies than the analytical simulations currently used in Euclid . The proposed method combines a control on galaxy shape parameters offered by analytic models with realistic surface brightness distributions learned from real Hubble Space Telescope observations by deep generative models. We simulate a galaxy field of 0.4 deg 2 as it will be seen by the Euclid visible imager VIS, and we show that galaxy structural parameters are recovered to an accuracy similar to that for pure analytic Sérsic profiles. Based on these simulations, we estimate that the Euclid Wide Survey (EWS) will be able to resolve the internal morphological structure of galaxies down to a surface brightness of 22.5 mag arcsec −2 , and the Euclid Deep Survey (EDS) down to 24.9 mag arcsec −2 . This corresponds to approximately 250 million galaxies at the end of the mission and a 50% complete sample for stellar masses above 10 10.6 M ⊙ (resp. 10 9.6 M ⊙ ) at a redshift z ∼ 0.5 for the EWS (resp. EDS). The approach presented in this work can contribute to improving the preparation of future high-precision cosmological imaging surveys by allowing simulations to incorporate more realistic galaxies.

On cosmological bias due to the magnification of shear and position samples in modern weak lensing analyses

ArXiv 2111.09867 (2021)

Authors:

Christopher AJ Duncan, Joachim Harnois-Déraps, Lance Miller

Euclid: Forecasts from redshift-space distortions and the Alcock–Paczynski test with cosmic voids

Astronomy & Astrophysics EDP Sciences 658 (2021) A20-A20

Authors:

N Hamaus, M Aubert, A Pisani, S Contarini, G Verza, M-C Cousinou, S Escoffier, A Hawken, G Lavaux, G Pollina, BD Wandelt, J Weller, M Bonici, C Carbone, L Guzzo, A Kovacs, F Marulli, E Massara, L Moscardini, P Ntelis, WJ Percival, S Radinović, M Sahlén, Z Sakr, AG Sánchez

Abstract:

Euclid is poised to survey galaxies across a cosmological volume of unprecedented size, providing observations of more than a billion objects distributed over a third of the full sky. Approximately 20 million of these galaxies will have their spectroscopy available, allowing us to map the three-dimensional large-scale structure of the Universe in great detail. This paper investigates prospects for the detection of cosmic voids therein and the unique benefit they provide for cosmological studies. In particular, we study the imprints of dynamic (redshift-space) and geometric (Alcock-Paczynski) distortions of average void shapes and their constraining power on the growth of structure and cosmological distance ratios. To this end, we made use of the Flagship mock catalog, a state-of-the-art simulation of the data expected to be observed with Euclid. We arranged the data into four adjacent redshift bins, each of which contains about 11000 voids and we estimated the stacked void-galaxy cross-correlation function in every bin. Fitting a linear-theory model to the data, we obtained constraints on f/b and DMH, where f is the linear growth rate of density fluctuations, b the galaxy bias, D-M the comoving angular diameter distance, and H the Hubble rate. In addition, we marginalized over two nuisance parameters included in our model to account for unknown systematic effects in the analysis. With this approach, Euclid will be able to reach a relative precision of about 4% on measurements of f/b and 0.5% on DMH in each redshift bin. Better modeling or calibration of the nuisance parameters may further increase this precision to 1% and 0.4%, respectively. Our results show that the exploitation of cosmic voids in Euclid will provide competitive constraints on cosmology even as a stand-alone probe. For example, the equation-of-state parameter, w, for dark energy will be measured with a precision of about 10%, consistent with previous more approximate forecasts.Peer reviewe

Euclid preparation

Astronomy & Astrophysics EDP Sciences 655 (2021) a44

Authors:

A Pocino, I Tutusaus, FJ Castander, P Fosalba, M Crocce, A Porredon, S Camera, V Cardone, S Casas, T Kitching, F Lacasa, M Martinelli, A Pourtsidou, Z Sakr, S Andreon, N Auricchio, C Baccigalupi, A Balaguera-Antolínez, M Baldi, A Balestra, S Bardelli, R Bender, A Biviano, C Bodendorf, D Bonino, A Boucaud, E Bozzo, E Branchini, M Brescia, J Brinchmann, C Burigana, R Cabanac, V Capobianco, A Cappi, CS Carvalho, M Castellano, G Castignani, S Cavuoti, A Cimatti, R Cledassou, C Colodro-Conde, G Congedo, CJ Conselice, L Conversi, Y Copin, L Corcione, A Costille, J Coupon, HM Courtois, M Cropper, J-G Cuby, A Da Silva, S de la Torre, D Di Ferdinando, F Dubath, C Duncan, X Dupac, S Dusini, S Farrens, PG Ferreira, I Ferrero, F Finelli, S Fotopoulou, M Frailis, E Franceschi, S Galeotta, B Garilli, W Gillard, B Gillis, C Giocoli, G Gozaliasl, J Graciá-Carpio, F Grupp, L Guzzo, W Holmes, F Hormuth, K Jahnke, E Keihanen, S Kermiche, A Kiessling, CC Kirkpatrick, M Kunz, H Kurki-Suonio, S Ligori, PB Lilje, I Lloro, D Maino, E Maiorano, O Mansutti, O Marggraf, N Martinet, F Marulli, R Massey, S Maurogordato, E Medinaceli, S Mei, M Meneghetti, R Benton Metcalf, G Meylan, M Moresco, B Morin, L Moscardini, E Munari, R Nakajima, C Neissner, RC Nichol, S Niemi, J Nightingale, C Padilla, S Paltani, F Pasian, L Patrizii, K Pedersen, WJ Percival, V Pettorino, S Pires, G Polenta, M Poncet, L Popa, D Potter, L Pozzetti, F Raison, A Renzi, J Rhodes, G Riccio, E Romelli, M Roncarelli, E Rossetti, R Saglia, AG Sánchez, D Sapone, R Scaramella, P Schneider, V Scottez, A Secroun, G Seidel, S Serrano, C Sirignano, G Sirri, L Stanco, F Sureau, AN Taylor, M Tenti, I Tereno, R Teyssier, R Toledo-Moreo, A Tramacere, EA Valentijn, L Valenziano, J Valiviita, T Vassallo, M Viel, Y Wang, N Welikala, L Whittaker, A Zacchei, G Zamorani, J Zoubian, E Zucca

MIGHTEE: total intensity radio continuum imaging and the COSMOS/XMM-LSS Early Science fields

Monthly Notices of the Royal Astronomical Society Oxford University Press 509:2 (2021) 2150-2168

Authors:

I Heywood, Mj Jarvis, Cl Hale, Ih Whittam, Hl Bester, B Hugo, Js Kenyon, M Prescott, Om Smirnov, C Tasse, Jm Afonso, Pn Best, Jd Collier, Rp Deane, Bs Frank, Mj Hardcastle, K Knowles, N Maddox, Ej Murphy, I Prandoni, Sm Randriamampandry, Mg Santos, S Sekhar, F Tabatabaei, Ar Taylor, K Thorat

Abstract:

MIGHTEE is a galaxy evolution survey using siltaneous radio continuum, spectropolarimetry, and spectral line observations from the South African MeerKAT telescope. When complete, the survey will image 20 deg2 over the COSMOS, E-CDFS, ELAIS-S1, and XMM-Newton Large Scale Structure field (XMM-LSS) extragalactic deep fields with a central frequency of 1284 MHz. These were selected based on the extensive ltiwavelength data sets from numerous existing and forthcoming observational campaigns. Here, we describe and validate the data processing strategy for the total intensity continuum aspect of MIGHTEE, using a single deep pointing in COSMOS (1.6 deg2) and a three-pointing mosaic in XMM-LSS (3.5 deg2). The processing includes the correction of direction-dependent effects, and results in theal noise levels below 2 ${}$Jy beam-1 in both fields, limited in the central regions by classical confusion at 8 arcsec angular resolution, and meeting the survey specifications. We also produce images at 5 arcsec resolution that are 3 times shallower. The resulting image products fo the basis of the Early Science continuum data release for MIGHTEE. From these images we extract catalogues containing 9896 and 20 274 radio components in COSMOS and XMM-LSS, respectively. We also process a close-packed mosaic of 14 additional pointings in COSMOS and use these in conjunction with the Early Science pointing to investigate methods for primary beam correction of broad-band radio images, an analysis that is of relevance to all full-band MeerKAT continuum observations, and wide-field interferometric imaging in general. A public release of the MIGHTEE Early Science continuum data products accompanies this article.