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Black Hole

Lensing of space time around a black hole. At Oxford we study black holes observationally and theoretically on all size and time scales - it is some of our core work.

Credit: ALAIN RIAZUELO, IAP/UPMC/CNRS. CLICK HERE TO VIEW MORE IMAGES.

Christopher Duncan

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Sub department

  • Astrophysics

Research groups

  • Beecroft Institute for Particle Astrophysics and Cosmology
  • Euclid
christopher.duncan@physics.ox.ac.uk
Telephone: 01865(2)83016
Denys Wilkinson Building, room 555A
  • About
  • Publications

Euclid

Astronomy & Astrophysics EDP Sciences 697 (2025) ARTN A5

Authors:

Fj Castander, P Fosalba, J Stadel, D Potter, J Carretero, P Tallada-Crespí, L Pozzetti, M Bolzonella, Ga Mamon, L Blot, K Hoffmann, M Huertas-Company, P Monaco, Ej Gonzalez, G De Lucia, C Scarlata, M-A Breton, L Linke, C Viglione, S-S Li, Z Zhai, Z Baghkhani, K Pardede, C Neissner, R Teyssier, M Crocce, I Tutusaus, L Miller, G Congedo, A Biviano, M Hirschmann, A Pezzotta, H Aussel, H Hoekstra, T Kitching, Wj Percival, L Guzzo, Y Mellier, Pa Oesch, Raa Bowler, S Bruton, V Allevato, V Gonzalez-Perez, M Manera, S Avila, A Kovács, N Aghanim, B Altieri, A Amara, L Amendola

Abstract:

We present the Flagship galaxy mock, a simulated catalogue of billions of galaxies designed to support the scientific exploitation of the Euclid mission. Euclid is a medium-class mission of the European Space Agency optimised to determine the properties of dark matter and dark energy on the largest scales of the Universe. It probes structure formation over more than 10 billion years primarily from the combination of weak gravitational lensing and galaxy clustering data. The breadth of Euclid’s data will also foster a wide variety of scientific analyses. The Flagship simulation was developed to provide a realistic approximation to the galaxies that will be observed by Euclid and used in its scientific exploitation. We ran a state-of-the-art N-body simulation with four trillion particles, producing a lightcone on the fly. From the dark matter particles, we produced a catalogue of 16 billion haloes in one octant of the sky in the lightcone up to redshift z = 3. We then populated these haloes with mock galaxies using a halo occupation distribution and abundance-matching approach, calibrating the free parameters of the galaxy mock against observed correlations and other basic galaxy properties. Modelled galaxy properties include luminosity and flux in several bands, redshifts, positions and velocities, spectral energy distributions, shapes and sizes, stellar masses, star formation rates, metallicities, emission line fluxes, and lensing properties. We selected a final sample of 3.4 billion galaxies with a magnitude cut of HE < 26, where we are complete. We have performed a comprehensive set of validation tests to check the similarity to observational data and theoretical models. In particular, our catalogue is able to closely reproduce the main characteristics of the weak lensing and galaxy clustering samples to be used in the mission main cosmological analysis. Moreover, given its depth and completeness, this new galaxy mock also provides the community with a powerful tool for developing a wide range of scientific analyses beyond the Euclid mission.

Euclid preparation

Astronomy & Astrophysics EDP Sciences 695 (2025) ARTN A280

Authors:

L Ingoglia, M Sereno, S Farrens, C Giocoli, L Baumont, Gf Lesci, L Moscardini, C Murray, M Vannier, A Biviano, C Carbone, G Covone, G Despali, M Maturi, S Maurogordato, M Meneghetti, M Radovich, B Altieri, A Amara, S Andreon, N Auricchio, C Baccigalupi, M Baldi, S Bardelli, F Bellagamba, R Bender, F Bernardeau, D Bonino, E Branchini, M Brescia, J Brinchmann, S Camera, V Capobianco, J Carretero, S Casas, M Castellano, G Castignani, S Cavuoti, A Cimatti, C Colodro-Conde, G Congedo, Cj Conselice, L Conversi, Y Copin, F Courbin, Hm Courtois, M Cropper, A Da Silva, H Degaudenzi, G De Lucia

Abstract:

The ability to measure unbiased weak-lensing (WL) masses is a key ingredient to exploit galaxy clusters as a competitive cosmological probe with the ESA Euclid survey or future missions. We investigate the level of accuracy and precision of cluster masses measured with the Euclid data processing pipeline. We use the DEMNUni-Cov N-body simulations to assess how well the WL mass probes the true halo mass, and, then, how well WL masses can be recovered in the presence of measurement uncertainties. We consider different halo mass density models, priors, and mass point estimates, that is the biweight, mean, and median of the marginalised posterior distribution and the maximum likelihood parameter. WL mass differs from true mass due to, for example, the intrinsic ellipticity of sources, correlated or uncorrelated matter and large-scale structure, halo triaxiality and orientation, and merging or irregular morphology. In an ideal scenario without observational or measurement errors, the maximum likelihood estimator is the most accurate, with WL masses biased low by {bM} =a-14.6-±-1.7% on average over the full range M200c > 5×1013 M⊙ and z < 1. Due to the stabilising effect of the prior, the biweight, mean, and median estimates are more precise, that is with smaller intrinsic scatter. The scatter decreases with increasing mass and informative priors can significantly reduce the scatter. Halo mass density profiles with a truncation provide better fits to the lensing signal, while the accuracy and precision are not significantly affected. We further investigate the impact of various additional sources of systematic uncertainty on the WL mass estimates, namely the impact of photometric redshift uncertainties and source selection, the expected performance of Euclid cluster detection algorithms, and the presence of masks. Taken in isolation, we find that the largest effect is induced by non-conservative source selection with {bM} =a-33.4-±-1.6%. This effect can be mostly removed with a robust selection. As a final Euclid-like test, we combine systematic effects in a realistic observational setting and find {bM} =a-15.5-±-2.4% under a robust selection. This is very similar to the ideal case, though with a slightly larger scatter mostly due to cluster redshift uncertainty and miscentering.

Euclid preparation

Astronomy & Astrophysics EDP Sciences 695 (2025) ARTN A232

Authors:

G Rácz, M-A Breton, B Fiorini, Amc Le Brun, H-A Winther, Z Sakr, L Pizzuti, A Ragagnin, T Gayoux, E Altamura, E Carella, K Pardede, G Verza, K Koyama, M Baldi, A Pourtsidou, F Vernizzi, Ag Adame, J Adamek, S Avila, C Carbone, G Despali, C Giocoli, C Hernández-Aguayo, F Hassani, M Kunz, B Li, Y Rasera, G Yepes, V Gonzalez-Perez, P-S Corasaniti, J García-Bellido, N Hamaus, A Kiessling, M Marinucci, C Moretti, Df Mota, L Piga, A Pisani, I Szapudi, P Tallada-Crespí, N Aghanim, S Andreon, C Baccigalupi, S Bardelli, D Bonino, E Branchini, M Brescia, J Brinchmann, S Camera

Euclid preparation

Astronomy & Astrophysics EDP Sciences 697 (2025) ARTN A85

Authors:

My Elkhashab, D Bertacca, C Porciani, J Salvalaggio, N Aghanim, A Amara, S Andreon, N Auricchio, C Baccigalupi, M Baldi, S Bardelli, C Bodendorf, D Bonino, E Branchini, M Brescia, J Brinchmann, S Camera, V Capobianco, C Carbone, Vf Cardone, J Carretero, R Casas, S Casas, M Castellano, G Castignani, S Cavuoti, A Cimatti, C Colodro-Conde, G Congedo, Cj Conselice, L Conversi, Y Copin, F Courbin, Hm Courtois, A Da Silva, H Degaudenzi, Am Di Giorgio, J Dinis, M Douspis, F Dubath, Caj Duncan, X Dupac, S Dusini, M Farina, S Farrens, S Ferriol, P Fosalba, M Frailis, E Franceschi, S Galeotta

Abstract:

Measurements of galaxy clustering are affected by redshift-space distortions (RSDs). Peculiar velocities, gravitational lensing, and other light-cone projection effects modify the observed redshifts, fluxes, and sky positions of distant light sources. We determined which of these effects leave a detectable imprint on several two-point clustering statistics to be extracted from the Euclid wide spectroscopic survey (EWSS) on large scales. We generated 140 mock galaxy catalogues with the survey geometry and selection function of the EWSS and made use of the LIGER (LIght cones with GEneral Relativity) method to account for a variable number of relativistic RSDs to linear order in the cosmological perturbations. We estimated different two-point clustering statistics from the mocks and used the likelihood-ratio test to calculate the statistical significance with which the EWSS could reject the null hypothesis that certain relativistic projection effects can be neglected in the theoretical models. We find that the combined effects of lensing magnification and convergence imprint characteristic signatures on several clustering observables. Their signal-to-noise ratio (S/N) ranges between 2.5 and 6 (depending on the adopted summary statistic) for the highest-redshift galaxies in the EWSS. The corresponding feature due to the peculiar velocity of the Sun is measured with a S/N of order one or two. The multipoles of the power spectrum from the catalogues that include all relativistic effects reject the null hypothesis that RSDs are only generated by the variation in the peculiar velocity along the line of sight with a significance of 2.9 standard deviations. As a by-product of our study, we demonstrate that the mixing-matrix formalism to model finite-volume effects in the multipole moments of the power spectrum can be robustly applied to surveys made of several disconnected patches. Our results indicate that relativistic RSDs, in particular the contribution from weak gravitational lensing, cannot be disregarded when modelling two-point clustering statistics extracted from the EWSS.

Euclid preparation

Astronomy & Astrophysics EDP Sciences 695 (2025) a229

Authors:

L Zalesky, CJR McPartland, JR Weaver, S Toft, DB Sanders, B Mobasher, N Suzuki, I Szapudi, I Valdes, G Murphree, N Chartab, N Allen, S Taamoli, SWJ Barrow, O Chávez Ortiz, SL Finkelstein, S Gwyn, M Sawicki, HJ McCracken, D Stern, H Dannerbauer, B Altieri, S Andreon, N Auricchio, C Baccigalupi, M Baldi, S Bardelli, R Bender, C Bodendorf, D Bonino, E Branchini, M Brescia, J Brinchmann, S Camera, V Capobianco, C Carbone, J Carretero, S Casas, FJ Castander, M Castellano, G Castignani, S Cavuoti, A Cimatti, C Colodro-Conde, G Congedo, CJ Conselice, L Conversi, Y Copin, L Corcione, F Courbin, HM Courtois, A Da Silva, H Degaudenzi, G De Lucia, AM Di Giorgio, J Dinis, F Dubath, CAJ Duncan, X Dupac, S Dusini, M Farina, S Farrens, S Ferriol, S Fotopoulou, M Frailis, E Franceschi, S Galeotta, B Garilli, W Gillard, B Gillis, C Giocoli, P Gómez-Alvarez, A Grazian, F Grupp, SVH Haugan, H Hoekstra, W Holmes, I Hook, F Hormuth, A Hornstrup, P Hudelot, K Jahnke, B Joachimi, E Keihänen, S Kermiche, A Kiessling, M Kilbinger, B Kubik, K Kuijken, M Kümmel, M Kunz, H Kurki-Suonio, R Laureijs, S Ligori, PB Lilje, V Lindholm, I Lloro, G Mainetti, D Maino, E Maiorano, O Mansutti, O Marggraf, K Markovic, M Martinelli, N Martinet, F Marulli, R Massey, S Maurogordato, S Mei, Y Mellier, M Meneghetti, E Merlin, G Meylan, M Moresco, L Moscardini, E Munari, C Neissner, S-M Niemi, JW Nightingale, C Padilla, S Paltani, F Pasian, K Pedersen, WJ Percival, V Pettorino, S Pires, G Polenta, M Poncet, LA Popa, L Pozzetti, F Raison, R Rebolo, A Renzi, J Rhodes, G Riccio, E Romelli, M Roncarelli, E Rossetti, R Saglia, Z Sakr, D Sapone, R Scaramella, M Schirmer, P Schneider, T Schrabback, A Secroun, E Sefusatti, G Seidel, S Serrano, C Sirignano, G Sirri, L Stanco, J Steinwagner, P Tallada-Crespí, HI Teplitz, I Tereno, R Toledo-Moreo, F Torradeflot, I Tutusaus, EA Valentijn, L Valenziano, T Vassallo, G Verdoes Kleijn, A Veropalumbo, Y Wang, J Weller, G Zamorani, E Zucca, M Bolzonella, A Boucaud, E Bozzo, C Burigana, D Di Ferdinando, JA Escartin Vigo, R Farinelli, J Gracia-Carpio, N Mauri, AA Nucita, V Scottez, M Tenti, M Viel, M Wiesmann, Y Akrami, V Allevato, S Anselmi, M Ballardini, M Bethermin, A Blanchard, L Blot, S Borgani, S Bruton, R Cabanac, A Calabro, A Cappi, CS Carvalho, T Castro, KC Chambers, R Chary, S Contarini, T Contini, AR Cooray, B De, G Desprez, A Díaz-Sánchez, S Di Domizio, H Dole, S Escoffier, AG Ferrari, I Ferrero, F Finelli, F Fornari, L Gabarra, K Ganga, J García-Bellido, E Gaztanaga, F Giacomini, G Gozaliasl, A Hall, WG Hartley, H Hildebrandt, J Hjorth, M Huertas-Company, O Ilbert, A Jimenez Muñoz, JJE Kajava, V Kansal, D Karagiannis, CC Kirkpatrick, L Legrand, G Libet, A Loureiro, J Macias-Perez, G Maggio, M Magliocchetti, C Mancini, F Mannucci, R Maoli, CJAP Martins, S Matthew, L Maurin, RB Metcalf, P Monaco, C Moretti, G Morgante, Nicholas A Walton, J Odier, L Patrizii, A Pezzotta, M Pöntinen, V Popa, C Porciani, D Potter, P Reimberg, I Risso, P-F Rocci, M Sahlén, C Scarlata, A Schneider, M Sereno, A Silvestri, P Simon, A Spurio Mancini, SA Stanford, C Tao, G Testera, R Teyssier, S Tosi, A Troja, M Tucci, C Valieri, J Valiviita, D Vergani, G Verza, IA Zinchenko

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