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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

Visitor

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 preparation

Astronomy & Astrophysics EDP Sciences 694 (2025) ARTN A141

Authors:

N Tessore, B Joachimi, A Loureiro, A Hall, G Cañas-Herrera, I Tutusaus, N Jeffrey, K Naidoo, Jd McEwen, A Amara, S Andreon, N Auricchio, C Baccigalupi, M Baldi, S Bardelli, F Bernardeau, D Bonino, E Branchini, M Brescia, J Brinchmann, A Caillat, S Camera, V Capobianco, C Carbone, Vf Cardone, 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, J Dinis, F Dubath, Caj Duncan, X Dupac, S Dusini, M Farina, S Farrens, F Faustini

Abstract:

In this paper we present the framework for measuring angular power spectra in the Euclid mission. The observables in galaxy surveys, such as galaxy clustering and cosmic shear, are not continuous fields, but discrete sets of data, obtained only at the positions of galaxies. We show how to compute the angular power spectra of such discrete data sets, without treating observations as maps of an underlying continuous field that is overlaid with a noise component. This formalism allows us to compute the exact theoretical expectations for our measured spectra, under a number of assumptions that we track explicitly. In particular, we obtain exact expressions for the additive biases ('shot noise') in angular galaxy clustering and cosmic shear. For efficient practical computations, we introduce a spin-weighted spherical convolution with a well-defined convolution theorem, which allows us to apply exact theoretical predictions to finite-resolution maps, including HEALPix. When validating our methodology, we find that our measurements are biased by less than 1% of their statistical uncertainty in simulations of Euclid's first data release.

Euclid preparation

Astronomy & Astrophysics EDP Sciences 694 (2025) a262

Authors:

D Scognamiglio, T Schrabback, M Tewes, B Gillis, H Hoekstra, EM Huff, O Marggraf, T Kitching, R Massey, I Tereno, CS Carvalho, A Robertson, G Congedo, N Aghanim, B Altieri, A Amara, S Andreon, N Auricchio, C Baccigalupi, M Baldi, S Bardelli, P Battaglia, C Bodendorf, D Bonino, E Branchini, M Brescia, J Brinchmann, S Camera, V Capobianco, C Carbone, VF Cardone, J Carretero, S Casas, FJ Castander, M Castellano, G Castignani, S Cavuoti, A Cimatti, C Colodro-Conde, CJ Conselice, L Conversi, Y Copin, F Courbin, HM Courtois, M Cropper, 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, P Fosalba, M Frailis, E Franceschi, S Galeotta, C Giocoli, P Gómez-Alvarez, A Grazian, F Grupp, L Guzzo, SVH Haugan, W Holmes, F Hormuth, A Hornstrup, P Hudelot, K Jahnke, B Joachimi, E Keihänen, S Kermiche, A Kiessling, M Kilbinger, B Kubik, M Kümmel, M Kunz, H Kurki-Suonio, S Ligori, PB Lilje, V Lindholm, I Lloro, G Mainetti, E Maiorano, O Mansutti, K Markovic, M Martinelli, N Martinet, F Marulli, E Medinaceli, S Mei, Y Mellier, M Meneghetti, G Meylan, M Moresco, L Moscardini, R Nakajima, S-M Niemi, JW Nightingale, C Padilla, S Paltani, F Pasian, K Pedersen, 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, AG Sánchez, D Sapone, B Sartoris, R Scaramella, M Schirmer, P Schneider, A Secroun, G Seidel, S Serrano, C Sirignano, G Sirri, J Skottfelt, L Stanco, J-L Starck, J Steinwagner, P Tallada-Crespí, AN Taylor, HI Teplitz, R Toledo-Moreo, F Torradeflot, I Tutusaus, L Valenziano, T Vassallo, G Verdoes Kleijn, A Veropalumbo, Y Wang, J Weller, M Wetzstein, G Zamorani, E Zucca, A Biviano, M Bolzonella, A Boucaud, E Bozzo, C Burigana, M Calabrese, JA Escartin Vigo, J Gracia-Carpio, N Mauri, A Pezzotta, M Pöntinen, C Porciani, V Scottez, M Tenti, M Viel, M Wiesmann, Y Akrami, V Allevato, S Anselmi, M Ballardini, L Blot, S Borgani, S Bruton, R Cabanac, A Calabro, A Cappi, T Castro, KC Chambers, S Contarini, AR Cooray, S Davini, B De, G Desprez, A Díaz-Sánchez, S Di Domizio, H Dole, S Escoffier, AG Ferrari, I Ferrero, F Fornari, L Gabarra, K Ganga, J García-Bellido, E Gaztanaga, F Giacomini, F Gianotti, G Gozaliasl, A Hall, S Hemmati, H Hildebrandt, J Hjorth, A Jimenez Muñoz, JJE Kajava, V Kansal, D Karagiannis, CC Kirkpatrick, J Le Graet, L Legrand, A Loureiro, J Macias-Perez, G Maggio, M Magliocchetti, F Mannucci, R Maoli, CJAP Martins, S Matthew, L Maurin, RB Metcalf, P Monaco, C Moretti, G Morgante, NA Walton, L Patrizii, V Popa, D Potter, P Reimberg, I Risso, P-F Rocci, RP Rollins, M Sahlén, A Schneider, M Sereno, P Simon, A Spurio Mancini, K Tanidis, C Tao, G Testera, R Teyssier, S Toft, S Tosi, A Troja, M Tucci, C Valieri, J Valiviita, D Vergani, G Verza

Euclid: A complete Einstein ring in NGC 6505

Astronomy & Astrophysics EDP Sciences 694 (2025) a145

Authors:

CM O’Riordan, LJ Oldham, A Nersesian, T Li, TE Collett, D Sluse, B Altieri, B Clément, KGC Vasan, S Rhoades, Y Chen, T Jones, C Adami, R Gavazzi, S Vegetti, DM Powell, JA Acevedo Barroso, IT Andika, R Bhatawdekar, AR Cooray, G Despali, JM Diego, LR Ecker, A Galan, P Gómez-Alvarez, L Leuzzi, M Meneghetti, RB Metcalf, M Schirmer, S Serjeant, C Tortora, M Vaccari, G Vernardos, M Walmsley, A Amara, S Andreon, N Auricchio, H Aussel, C Baccigalupi, M Baldi, A Balestra, S Bardelli, A Basset, P Battaglia, R Bender, D Bonino, E Branchini, M Brescia, J Brinchmann, A Caillat, 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, M Cropper, 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, F Faustini, S Ferriol, N Fourmanoit, M Frailis, E Franceschi, M Fumana, S Galeotta, W Gillard, B Gillis, C Giocoli, BR Granett, A Grazian, F Grupp, L Guzzo, SVH Haugan, J Hoar, H Hoekstra, W Holmes, I Hook, F Hormuth, A Hornstrup, P Hudelot, K Jahnke, M Jhabvala, B Joachimi, E Keihänen, S Kermiche, A Kiessling, M Kilbinger, R Kohley, B Kubik, M Kümmel, M Kunz, H Kurki-Suonio, O Lahav, R Laureijs, D Le Mignant, S Ligori, PB Lilje, V Lindholm, I Lloro, G Mainetti, E Maiorano, O Mansutti, O Marggraf, K Markovic, M Martinelli, N Martinet, F Marulli, R Massey, E Medinaceli, S Mei, M Melchior, Y Mellier, E Merlin, G Meylan, M Moresco, L Moscardini, R Nakajima, RC Nichol, 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, H-W Rix, E Romelli, M Roncarelli, E Rossetti, B Rusholme, R Saglia, Z Sakr, AG Sánchez, D Sapone, B Sartoris, P Schneider, T Schrabback, A Secroun, G Seidel, S Serrano, C Sirignano, G Sirri, L Stanco, J Steinwagner, P Tallada-Crespí, I Tereno, R Toledo-Moreo, F Torradeflot, I Tutusaus, L Valenziano, T Vassallo, G Verdoes Kleijn, A Veropalumbo, Y Wang, J Weller, A Zacchei, G Zamorani, E Zucca, C Burigana, P Casenove, A Mora, V Scottez, M Viel, M Jauzac, H Dannerbauer

Euclid preparation

Astronomy & Astrophysics EDP Sciences 693 (2025) a59

Authors:

H Böhringer, G Chon, O Cucciati, H Dannerbauer, M Bolzonella, G De Lucia, A Cappi, L Moscardini, C Giocoli, G Castignani, Na Hatch, S Andreon, E Bañados, S Ettori, F Fontanot, H Gully, M Hirschmann, M Maturi, S Mei, L Pozzetti, T Schlenker, M Spinelli, N Aghanim, B Altieri, N Auricchio, C Baccigalupi, M Baldi, S Bardelli, C Bodendorf, D Bonino, E Branchini, M Brescia, J Brinchmann, S Camera, V Capobianco, C Carbone, J Carretero, S Casas, Fj Castander, M Castellano, S Cavuoti, A Cimatti, C Colodro-Conde, G Congedo, Cj Conselice, L Conversi, Y Copin, F Courbin, Hm Courtois, A Da Silva

Abstract:

Galaxy proto-clusters are receiving increased interest since most of the processes shaping the structure of clusters of galaxies and their galaxy population happen at the early stages of their formation. The Euclid Survey will provide a unique opportunity to discover a large number of proto-clusters over a large fraction of the sky (14 500 deg2). In this paper, we explore the expected observational properties of proto-clusters in the Euclid Wide Survey by means of theoretical models and simulations. We provide an overview of the predicted proto-cluster extent, galaxy density profiles, mass-richness relations, abundance, and sky-filling as a function of redshift. Useful analytical approximations for the functions of these properties are provided. The focus is on the redshift range z = 1.5-4. In particular we discuss the density contrast with which proto-clusters can be observed against the background in the galaxy distribution if photometric galaxy redshifts are used as supplied by the ESA Euclid mission together with the ground-based photometric surveys. We show that the obtainable detection significance is sufficient to find large numbers of interesting proto-cluster candidates. For quantitative studies, additional spectroscopic follow-up is required to confirm the proto-clusters and establish their richness.

Euclid preparation

Astronomy & Astrophysics EDP Sciences 693 (2025) a58

Authors:

M Archidiacono, J Lesgourgues, S Casas, S Pamuk, N Schöneberg, Z Sakr, G Parimbelli, A Schneider, F Hervas Peters, F Pace, Vm Sabarish, M Costanzi, S Camera, C Carbone, S Clesse, N Frusciante, A Fumagalli, P Monaco, D Scott, M Viel, A Amara, S Andreon, N Auricchio, M Baldi, S Bardelli, C Bodendorf, D Bonino, E Branchini, M Brescia, J Brinchmann, V Capobianco, Vf Cardone, J Carretero, M Castellano, S Cavuoti, A Cimatti, G Congedo, Cj Conselice, L Conversi, Y Copin, F Courbin, Hm Courtois, A Da Silva, H Degaudenzi, M Douspis, F Dubath, Caj Duncan, X Dupac, S Dusini, A Ealet

Abstract:

Context. The Euclid mission of the European Space Agency will deliver weak gravitational lensing and galaxy clustering surveys that can be used to constrain the standard cosmological model and extensions thereof. Aims. We present forecasts from the combination of the Euclid photometric galaxy surveys (weak lensing, galaxy clustering, and their cross-correlations) and its spectroscopic redshift survey with respect to their sensitivity to cosmological parameters. We include the summed neutrino mass, Σmν, and the effective number of relativistic species, Neff, in the standard Λ CDM scenario and in the dynamical dark energy (w0waCDM) scenario. Methods. We compared the accuracy of different algorithms predicting the non-linear matter power spectrum for such models. We then validated several pipelines for Fisher matrix and Markov chain Monte Carlo (MCMC) forecasts, using different theory codes, algorithms for numerical derivatives, and assumptions on the non-linear cut-off scale. Results. The Euclid primary probes alone will reach a sensitivity of σ (Σmν = 60 meV) = 56 meV in the Λ CDM+Σmν model, whereas the combination with cosmic microwave background (CMB) data from Planck is expected to achieve σ (Σmν) = 23 meV, offering evidence of a non-zero neutrino mass to at least the 2.6 σ level. This could be pushed to a 4 σ detection if future CMB data from LiteBIRD and CMB Stage-IV were included. In combination with Planck, Euclid will also deliver tight constraints on Δ Neff < 0.144 (95%CL) in the Λ CDM+Σmν+Neff model or even Δ Neff < 0.063 when future CMB data are included. When floating the dark energy parameters, we find that the sensitivity to Neff remains stable, but for Σmν, it gets degraded by up to a factor of 2, at most. Conclusions. This work illustrates the complementarity among the Euclid spectroscopic and photometric surveys and among Euclid and CMB constraints. Euclid will offer great potential in measuring the neutrino mass and excluding well-motivated scenarios with additional relativistic particles.

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