Euclid preparation

Astronomy & Astrophysics EDP Sciences 684 (2024) a138

Authors:

AC Deshpande, T Kitching, A Hall, ML Brown, N Aghanim, L Amendola, S Andreon, N Auricchio, M Baldi, S Bardelli, R Bender, D Bonino, E Branchini, M Brescia, J Brinchmann, S Camera, GP Candini, V Capobianco, C Carbone, VF Cardone, J Carretero, S Casas, FJ Castander, M Castellano, S Cavuoti, A Cimatti, R Cledassou, G Congedo, CJ Conselice, L Conversi, L Corcione, F Courbin, HM Courtois, M Cropper, A Da Silva, H Degaudenzi, M Douspis, F Dubath, CAJ Duncan, X Dupac, M Farina, S Farrens, S Ferriol, P Fosalba, M Frailis, E Franceschi, M Fumana, S Galeotta, B Garilli, B Gillis, C Giocoli, A Grazian, F Grupp, SVH Haugan, H Hoekstra, W Holmes, A Hornstrup, P Hudelot, K Jahnke, E Keihänen, S Kermiche, M Kilbinger, M Kunz, H Kurki-Suonio, S Ligori, PB Lilje, V Lindholm, I Lloro, E Maiorano, O Mansutti, O Marggraf, K Markovic, N Martinet, F Marulli, R Massey, S Mei, Y Mellier, M Meneghetti, G Meylan, L Moscardini, S-M Niemi, JW Nightingale, T Nutma, C Padilla, S Paltani, F Pasian, K Pedersen, V Pettorino, S Pires, G Polenta, J Pollack, M Poncet, LA Popa, F Raison, A Renzi, J Rhodes, G Riccio, E Romelli, M Roncarelli, E Rossetti, R Saglia, D Sapone, B Sartoris, P Schneider, T Schrabback, A Secroun, G Seidel, S Serrano, C Sirignano, G Sirri, L Stanco, P Tallada-Crespí, AN Taylor, I Tereno, R Toledo-Moreo, F Torradeflot, I Tutusaus, EA Valentijn, L Valenziano, T Vassallo, Y Wang, J Weller, A Zacchei, G Zamorani, J Zoubian, E Zucca, A Boucaud, E Bozzo, C Colodro-Conde, D Di Ferdinando, G Fabbian, J Graciá-Carpio, N Mauri, V Scottez, M Tenti, Y Akrami, C Baccigalupi, A Balaguera-Antolínez, M Ballardini, F Bernardeau, A Biviano, A Blanchard, AS Borlaff, C Burigana, R Cabanac, A Cappi, CS Carvalho, G Castignani, T Castro, KC Chambers, AR Cooray, J Coupon, S Davini, S de la Torre, G De Lucia, G Desprez, H Dole, JA Escartin, S Escoffier, I Ferrero, F Finelli, J Garcia-Bellido, K George, F Giacomini, G Gozaliasl, H Hildebrandt, JJE Kajava, V Kansal, CC Kirkpatrick, L Legrand, A Loureiro, J Macias-Perez, M Magliocchetti, G Mainetti, R Maoli, M Martinelli, CJAP Martins, S Matthew, L Maurin, RB Metcalf, P Monaco, G Morgante, S Nadathur, AA Nucita, L Patrizii, A Peel, M Pöntinen, V Popa, C Porciani, D Potter, A Pourtsidou, P Reimberg, Z Sakr, AG Sánchez, A Schneider, E Sefusatti, M Sereno, A Shulevski, A Spurio Mancini, J Steinwagner, R Teyssier, M Viel, IA Zinchenko, P Fleury

A novel Bayesian approach for decomposing the radio emission of quasars: I. Modelling the radio excess in red quasars

Monthly Notices of the Royal Astronomical Society Oxford University Press (OUP) 529:4 (2024) 3939-3957

Authors:

B-H Yue, PN Best, KJ Duncan, G Calistro-Rivera, LK Morabito, JW Petley, I Prandoni, HJA Röttgering, DJB Smith

Abstract:

ABSTRACT Studies show that both radio jets from the active galactic nuclei (AGNs) and the star formation (SF) activity in quasar host galaxies contribute to the quasar radio emission; yet their relative contributions across the population remain unclear. Here, we present an improved parametric model that allows us to statistically separate the SF and AGN components in observed quasar radio flux density distributions, and investigate how their relative contributions evolve with AGN bolometric luminosity ($L_\mathrm{bol}$) and redshift (z) using a fully Bayesian method. Based on the newest data from LOw-Frequency ARray Two-metre Sky Survey data release 2, our model gives robust fitting results out to $z\sim 4$, showing a quasar host galaxy SF rate (SFR) evolution that increases with bolometric luminosity and with redshift out to $z\sim 4$. This differs from the global cosmic SFR density, perhaps due to the importance of galaxy mergers. The prevalence of radio AGN emissions increases with quasar luminosity, but has little dependence on redshift. Furthermore, our new methodology and large sample size allow us to subdivide our data set to investigate the role of other parameters. Specifically, in this paper, we explore quasar colour and demonstrate that the radio excess in red quasars is due to an enhancement in AGN-related emission, since the host galaxy SF contribution to the total radio emission is independent of quasar colour. We also find evidence that this radio enhancement occurs mostly in quasars with weak or intermediate radio power.

Euclid: Improving the efficiency of weak lensing shear bias calibration

Astronomy & Astrophysics EDP Sciences 683 (2024) a240

Authors:

H Jansen, M Tewes, T Schrabback, N Aghanim, A Amara, S Andreon, N Auricchio, M Baldi, E Branchini, M Brescia, J Brinchmann, S Camera, V Capobianco, C Carbone, VF Cardone, J Carretero, S Casas, M Castellano, S Cavuoti, A Cimatti, G Congedo, L Conversi, Y Copin, L Corcione, F Courbin, HM Courtois, A Da Silva, H Degaudenzi, J Dinis, F Dubath, X Dupac, M Farina, S Farrens, S Ferriol, M Frailis, E Franceschi, M Fumana, S Galeotta, B Gillis, C Giocoli, A Grazian, F Grupp, SVH Haugan, H Hoekstra, W Holmes, F Hormuth, A Hornstrup, P Hudelot, K Jahnke, B Joachimi, S Kermiche, A Kiessling, M Kilbinger, T Kitching, B Kubik, H Kurki-Suonio, S Ligori, PB Lilje, V Lindholm, I Lloro, E Maiorano, O Mansutti, O Marggraf, K Markovic, N Martinet, F Marulli, R Massey, E Medinaceli, S Mei, M Melchior, Y Mellier, M Meneghetti, E Merlin, G Meylan, L Miller, M Moresco, L Moscardini, E Munari, R Nakajima, S-M Niemi, C Padilla, S Paltani, F Pasian, K Pedersen, V Pettorino, S Pires, G Polenta, M Poncet, F Raison, A Renzi, J Rhodes, G Riccio, E Romelli, M Roncarelli, E Rossetti, R Saglia, D Sapone, B Sartoris, P Schneider, A Secroun, G Seidel, S Serrano, C Sirignano, G Sirri, J Skottfelt, L Stanco, P Tallada-Crespí, I Tereno, R Toledo-Moreo, F Torradeflot, I Tutusaus, EA Valentijn, L Valenziano, T Vassallo, A Veropalumbo, Y Wang, J Weller, G Zamorani, J Zoubian, C Colodro-Conde, V Scottez

Euclid preparation: XXXIV. The effect of linear redshift-space distortions in photometric galaxy clustering and its cross-correlation with cosmic shear

Astronomy & Astrophysics EDP Sciences 683 (2024) A17

Authors:

Konstantinos Tanidis, Vf Cardone, M Martinelli, I Tutusaus, S Camera, N Aghanim, A Amara, S Andreon, N Auricchio, M Baldi, S Bardelli, E Branchini, M Brescia, J Brinchmann, V Capobianco, C Carbone, J Carretero, S Casas, M Castellano, S Cavuoti, A Cimatti, R Cledassou, G Congedo, L Conversi, Y Copin, L Corcione, F Courbin, Hm Courtois, A Da Silvay, H Degaudenzi, J Dinis, F Dubath, X Dupac, S Dusini, M Farina, S Farrens, S Ferriol, P Fosalba, M Frailis, E Franceschi, M Fumana, S Galeotta, B Garilli, W Gillard, B Gillis, C Giocoli, A Grazian, F Grupp, L Guzzo, Svh Haugan

Abstract:

Context. The cosmological surveys that are planned for the current decade will provide us with unparalleled observations of the distribution of galaxies on cosmic scales, by means of which we can probe the underlying large-scale structure (LSS) of the Universe. This will allow us to test the concordance cosmological model and its extensions. However, precision pushes us to high levels of accuracy in the theoretical modelling of the LSS observables, so that no biases are introduced into the estimation of the cosmological parameters. In particular, effects such as redshift-space distortions (RSD) can become relevant in the computation of harmonic-space power spectra even for the clustering of the photometrically selected galaxies, as has previously been shown in literature.

Aims. In this work, we investigate the contribution of linear RSD, as formulated in the Limber approximation by a previous work, in forecast cosmological analyses with the photometric galaxy sample of the Euclid survey. We aim to assess their impact and to quantify the bias on the measurement of cosmological parameters that would be caused if this effect were neglected.

Methods. We performed this task by producing mock power spectra for photometric galaxy clustering and weak lensing, as is expected to be obtained from the Euclid survey. We then used a Markov chain Monte Carlo approach to obtain the posterior distributions of cosmological parameters from these simulated observations.

Results. When the linear RSD is neglected, significant biases are caused when galaxy correlations are used alone and when they are combined with cosmic shear in the so-called 3 × 2 pt approach. These biases can be equivalent to as much as 5σ when an underlying ΛCDM cosmology is assumed. When the cosmological model is extended to include the equation-of-state parameters of dark energy, the extension parameters can be shifted by more than 1σ.

Euclidpreparation

Astronomy & Astrophysics EDP Sciences 685 (2024) A108-A108

Authors:

E Lusso, S Fotopoulou, M Selwood, V Allevato, G Calderone, C Mancini, M Mignoli, M Scodeggio, L Bisigello, A Feltre, F Ricci, F La Franca, D Vergani, L Gabarra, V Le Brun, E Maiorano, E Palazzi, M Moresco, G Zamorani, G Cresci, K Jahnke, A Humphrey, H Landt, F Mannucci, A Marconi

Abstract:

The statistical distribution and evolution of key properties of active galactic nuclei (AGN), such as their accretion rate, mass, and spin, remains a subject of open debate in astrophysics. The ESA Euclid space mission, launched on July 1 2023, promises a breakthrough in this field. We create detailed mock catalogues of AGN spectra from the rest-frame near-infrared down to the ultraviolet – including emission lines – to simulate what Euclid will observe for both obscured (type 2) and unobscured (type 1) AGN. We concentrate on the red grisms of the NISP instrument, which will be used for the wide-field survey, opening a new window for spectroscopic AGN studies in the near-infrared. We quantify the efficiency in the redshift determination as well as in retrieving the emission line flux of the Hα+[N II] complex, as Euclid is mainly focused on this emission line, given that it is expected to be the brightest one in the probed redshift range. Spectroscopic redshifts are measured for 83% of the simulated AGN in the interval where the Hα is visible (i.e. 0.89 <  z <  1.83 at a line flux of > 2 × 10−16 erg s−1 cm−2, encompassing the peak of AGN activity at z ≃ 1 − 1.5) within the spectral coverage of the red grism. Outside this redshift range, the measurement efficiency decreases significantly. Overall, a spectroscopic redshift iscorrectly determined for about 90% of type 2 AGN down to an emission line flux of roughly 3 × 10−16 erg s−1 cm−2, and for type 1 AGN down to 8.5 × 10−16 erg s−1 cm−2. Recovered values for black hole mass show a small offset with respect to the input values by about 10%, but the agreement is good overall. With such a high spectroscopic coverage at z <  2, we will be able to measure AGN demography, scaling relations, and clustering from the epoch of the peak of AGN activity down to the present-day Universe for hundreds of thousands of AGN with homogeneous spectroscopic information