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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 Quick Data Release (Q1)

Astronomy & Astrophysics EDP Sciences 714 (2026) a210

Authors:

M Giulietti, I Prandoni, L Bisigello, G Rodighiero, M Talia, F Gentile, G Girardi, M Bondi, L Wang, A La Marca, PAC Cunha, R Hill, A Abghari, D Scott, G Zamorani, GA Mamon, A Lapi, M Behiri, G Santhosh, HJA Rottgering, R Gilli, R Scaramella, G Gandolfi, S Andreon, N Auricchio, C Baccigalupi, M Baldi, A Balestra, S Bardelli, P Battaglia, A Biviano, M Bolzonella, E Branchini, M Brescia, J Brinchmann, S Camera, G Cañas-Herrera, V Capobianco, C Carbone, J Carretero, S Casas, M Castellano, G Castignani, S Cavuoti, KC Chambers, A Cimatti, C Colodro-Conde, G Congedo, CJ Conselice, L Conversi, Y Copin, A Costille, F Courbin, HM Courtois, M Cropper, A Da Silva, H Degaudenzi, G De Lucia, C Dolding, H Dole, F Dubath, CAJ Duncan, X Dupac, S Dusini, S Escoffier, M Farina, R Farinelli, F Faustini, S Ferriol, F Finelli, S Fotopoulou, M Frailis, E Franceschi, M Fumana, L Gabarra, S Galeotta, K George, B Gillis, C Giocoli, J Gracia-Carpio, A Grazian, F Grupp, S Gwyn, WG Hartley, SVH Haugan, S Hemmati, J Hoar, W Holmes, A Hornstrup, M Huertas-Company, K Jahnke, M Jhabvala, B Joachimi, E Keihänen, S Kermiche, A Kiessling, M Kilbinger, B Kubik, M Kümmel, M Kunz, H Kurki-Suonio, AMC Le Brun, S Ligori, PB Lilje, V Lindholm, I Lloro, M Magliocchetti, G Mainetti, D Maino, E Maiorano, O Mansutti, S Marcin, O Marggraf, M Martinelli, N Martinet, F Marulli, RJ Massey, N Mauri, E Medinaceli, S Mei, Y Mellier, M Meneghetti, E Merlin, G Meylan, P Monaco, A Mora, M Moresco, C Moretti, L Moscardini, R Nakajima, C Neissner, RC Nichol, S-M Niemi, C Padilla, S Paltani, F Pasian, K Pedersen, WJ Percival, V Pettorino, A Pezzotta, S Pires, G Polenta, M Poncet, LA Popa, C Porciani, L Pozzetti, F Raison, A Renzi, J Rhodes, G Riccio, I Risso, E Romelli, M Roncarelli, R Saglia, Z Sakr, D Sapone, B Sartoris, JA Schewtschenko, M Schirmer, P Schneider, T Schrabback, A Secroun, G Seidel, S Serrano, P Simon, C Sirignano, G Sirri, L Stanco, J-L Starck, J Steinwagner, P Tallada-Crespí, AN Taylor, HI Teplitz, I Tereno, N Tessore, S Toft, R Toledo-Moreo, F Torradeflot, I Tutusaus, L Valenziano, J Valiviita, T Vassallo, A Veropalumbo, Y Wang, J Weller, A Zacchei, E Zucca, V Allevato, M Ballardini, E Bozzo, C Burigana, R Cabanac, M Calabrese, A Cappi, JA Escartin Vigo, R Maoli, J Martín-Fleitas, S Matthew, M Maturi, RB Metcalf, M Pöntinen, V Scottez, M Sereno, M Tenti, M Viel, M Wiesmann, Y Akrami, IT Andika, S Anselmi, M Archidiacono, F Atrio-Barandela, D Bertacca, M Bethermin, A Blanchard, L Blot, M Bonici, S Borgani, ML Brown, S Bruton, A Calabro, B Camacho Quevedo, F Caro, CS Carvalho, T Castro, F Cogato, S Conseil, AR Cooray, O Cucciati, S Davini, G Desprez, A Díaz-Sánchez, JJ Diaz, S Di Domizio, JM Diego, MY Elkhashab, A Enia, Y Fang, A Finoguenov, A Franco, K Ganga, J García-Bellido, T Gasparetto, V Gautard, E Gaztanaga, F Giacomini, F Gianotti, G Gozaliasl, M Guidi, CM Gutierrez, A Hall, C Hernández-Monteagudo, H Hildebrandt, J Hjorth, JJE Kajava, Y Kang, V Kansal, D Karagiannis, K Kiiveri, J Kim, CC Kirkpatrick, S Kruk, L Legrand, M Lembo, F Lepori, GF Lesci, J Lesgourgues, L Leuzzi, TI Liaudat, A Loureiro, J Macias-Perez, F Mannucci, CJAP Martins, L Maurin, M Miluzio, G Morgante, K Naidoo, P Natoli, A Navarro-Alsina, S Nesseris, D Paoletti, F Passalacqua, K Paterson, L Patrizii, A Pisani, D Potter, S Quai, M Radovich, S Sacquegna, M Sahlén, DB Sanders, E Sarpa, A Schneider, D Sciotti, E Sellentin, F Shankar, A Shulevski, LC Smith, JG Sorce, K Tanidis, C Tao, G Testera, R Teyssier, S Tosi, A Troja, M Tucci, A Venhola, D Vergani, G Verza, P Vielzeuf, NA Walton

Abstract:

We present and investigate the properties of a sample of radio-selected, Euclid -dark galaxies, identified from LOFAR HBA observations at 144 MHz within the Euclid Deep Field-North (EDF-N), covering approximately 10 deg 2 . Starting from 1051 radio sources lacking optical counterparts down to a 5σ depth of 23.9 in the y band in previous surveys (but detected with Spitzer /IRAC), we identified 166 galaxies with no emission at a depth of more than 3σ from Euclid Quick Release 1 (Q1) images, reaching a 5σ depth of 23.9 in the H E band, and no matches in the Euclid Q1 catalogue. To minimise contamination from nearby sources, we selected a sub-sample of 88 isolated galaxies. By exploiting multi-band images and catalogues available for the EDF-N, we inferred the physical properties of our sample via SED fitting. The resulting redshift distribution spans 0.4 ≤ z ph ≤ 5.0. We made use of recent sub-arcsecond imaging from the International LOFAR Telescope over an area of 2.5 deg × 2.5 deg to constrain the nature of the compact radio emission in our targets through brightness-temperature estimates. By combining this information with the radio excess relative to the infrared/radio-correlation (IRRC), we searched for possible active galactic nucleus (AGN) activity in our sample. Approximately 30% of our sources show a radio excess relative to star formation. This fraction increases to 40% when including AGNs identified via their brightness temperature. The Euclid -dark sources detected in the far-infrared (FIR) are consistent with a population of heavily obscured (⟨ A V ISM ⟩ = 5.0) massive (⟨log 10 ( M ⋆ / M ⊙ )⟩ = 11.6) star forming galaxies (SFGs) with high star formation rates (⟨log 10 (SFR/ M ⊙ yr −1 )⟩ = 3.3). Their location above the star-forming main sequence is consistent with the high-mass and high-SFR end of similar near-infrared (NIR)-dark galaxy populations selected at higher radio frequencies reported in the literature. We performed a UV-to-radio median stacking analysis, dividing the sources with LOFAR ILT imaging according to the presence of radio excess. Both sub-samples are detected in the H E band at 3σ and 9σ for the radio-excess and non–radio-excess sources, respectively. The two stacked populations exhibit similar global physical properties and differ primarily in their radio emission, with values consistent with those observed for individual sources, albeit with less extreme SFRs. These preliminary results indicate that, compared to similar selections carried out over smaller fields, the wide area covered by Euclid enables the identification of a higher fraction of systems in which intense star formation and AGN activity coexist, likely capturing a key phase of galaxy–black hole co-evolution.
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Euclid preparation

Astronomy & Astrophysics EDP Sciences 714 (2026) a342

Authors:

L Paganin, M Bonici, C Carbone, S Camera, I Tutusaus, S Davini, J Bel, S Tosi, D Sciotti, S Di Domizio, I Risso, G Testera, D Sapone, Z Sakr, A Amara, S Andreon, N Auricchio, C Baccigalupi, M Baldi, S Bardelli, P Battaglia, R Bender, F Bernardeau, A Biviano, C Bodendorf, D Bonino, E Branchini, M Brescia, J Brinchmann, V Capobianco, VF Cardone, J Carretero, S Casas, M Castellano, G Castignani, S Cavuoti, G Cañas-Herrera, KC Chambers, A Cimatti, C Colodro-Conde, G Congedo, CJ Conselice, L Conversi, Y Copin, L Corcione, A Costille, F Courbin, HM Courtois, M Crocce, M Cropper, A Da Silva, H Degaudenzi, G De Lucia, AM Di Giorgio, J Dinis, H Dole, F Dubath, CAJ Duncan, X Dupac, S Dusini, A Ealet, S Escoffier, M Farina, R Farinelli, S Farrens, S Ferriol, F Finelli, M Frailis, E Franceschi, S Galeotta, B Garilli, K George, W Gillard, B Gillis, C Giocoli, J Graciá-Carpio, A Grazian, F Grupp, L Guzzo, SVH Haugan, W Holmes, I Hook, F Hormuth, A Hornstrup, S Ilić, K Jahnke, B Joachimi, E Keihänen, S Kermiche, A Kiessling, M Kilbinger, T Kitching, B Kubik, M Kümmel, M Kunz, H Kurki-Suonio, 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, HJ McCracken, E Medinaceli, S Mei, Y Mellier, M Meneghetti, E Merlin, G Meylan, M Moresco, L Moscardini, E Munari, 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, B Sartoris, P Schneider, T Schrabback, M Scodeggio, A Secroun, G Seidel, S Serrano, C Sirignano, G Sirri, L Stanco, J-L Starck, J Steinwagner, C Surace, P Tallada-Crespí, D Tavagnacco, AN Taylor, I Tereno, N Tessore, S Toft, R Toledo-Moreo, F Torradeflot, EA Valentijn, L Valenziano, J Valiviita, T Vassallo, A Veropalumbo, Y Wang, J Weller, A Zacchei, G Zamorani, J Zoubian, E Zucca, A Boucaud, E Bozzo, C Burigana, M Calabrese, D Di Ferdinando, G Fabbian, N Mauri, V Scottez, M Tenti, M Viel, M Wiesmann, Y Akrami, V Allevato, S Anselmi, M Ballardini, A Blanchard, S Borgani, S Bruton, R Cabanac, A Calabro, A Cappi, CS Carvalho, T Castro, S Contarini, AR Cooray, J Coupon, G Desprez, A Díaz-Sánchez, JA Escartin Vigo, PG Ferreira, I Ferrero, F Fornari, L Gabarra, K Ganga, J García-Bellido, E Gaztanaga, F Giacomini, G Gozaliasl, A Gregorio, A Hall, H Hildebrandt, J Hjorth, JJE Kajava, V Kansal, D Karagiannis, CC Kirkpatrick, L Legrand, A Loureiro, J Macias-Perez, G Maggio, M Magliocchetti, F Mannucci, R Maoli, CJAP Martins, S Matthew, L Maurin, RB Metcalf, M Migliaccio, P Monaco, G Morgante, S Nadathur, L Patrizii, A Pezzotta, V Popa, C Porciani, D Potter, M Pöntinen, P-F Rocci, M Sahlén, A Schneider, M Schultheis, M Sereno, C Tao, R Teyssier, A Troja, M Tucci, C Valieri, D Vergani, G Verza, P Vielzeuf

Abstract:

Aims. In this paper we present cosmological parameter forecasts for the Euclid 6 × 2 pt statistics, which include the galaxy clustering and weak lensing main probes together with previously neglected cross-covariance and cross-correlation signals between imaging-photometric and spectroscopic data. The aim is understanding the impact of such cross-terms on the expected Euclid performance. Methods. We adopted the Fisher information matrix approach to produce 6 × 2 pt cosmological forecasts from Euclid , considering two different techniques known as the harmonic and hybrid approaches, respectively. In the first, we treat all the different Euclid probes in the same way, i.e., we consider only angular 2 pt statistics for spectroscopic and photometric galaxy distributions, as well as for weak lensing, fully analyzing all their possible cross-covariances and cross-correlations in the spherical harmonic domain. In the second, thanks to lessons learned from the harmonic approach, we do not account for negligible cross-covariances between the 3D spectroscopic galaxy distribution and the 2D photometric/imaging data, but consider the combination of their cross-correlation with the autocorrelation signals. Results. We find that both cross-covariance and cross-correlation signals between the two Euclid main probes, i.e., the spectroscopic galaxy sample and the photometric-imaging data, have a negligible impact on the cosmological parameter constraints and therefore on the Euclid performance. In the case of the hybrid approach, we attribute this result to the effect of the cross-correlation between weak lensing and photometric data, which is dominant with respect to other cross-correlation signals, and to the better performance of the full anisotropic 3D spectroscopic galaxy clustering with respect to the projected clustering. In the case of the 2D harmonic approach, we attribute this result to two main theoretical limitations of the 2D projected statistics implemented in this work according to the analysis of the official Euclid forecasts: the high shot noise and the limited redshift range of the spectroscopic sample, with respect to the photometric sample, together with the suppression of radial information from subdominant contributions such as redshift-space distortions and lensing magnification. Therefore, our analysis suggests that 2D and 3D Euclid data can be safely treated as independent, with a great saving in computational resources.
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Euclid: Field-level inference of primordial non-Gaussianity and cosmic initial conditions

Astronomy and Astrophysics 711 (2026)

Authors:

A Andrews, J Jasche, G Lavaux, F Leclercq, F Finelli, Y Akrami, M Ballardini, D Karagiannis, J Valiviita, N Bartolo, G Cañas-Herrera, S Casas, BR Granett, F Pace, D Paoletti, N Porqueres, Z Sakr, D Sapone, N Aghanim, A Amara, S Andreon, C Baccigalupi, M Baldi, S Bardelli, D Bonino, E Branchini, M Brescia, J Brinchmann, S Camera, V Capobianco, C Carbone, J Carretero, 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, G De Lucia, AM Di Giorgio, J Dinis, F Dubath, CAJ Duncan, X Dupac, S Dusini, M Farina, S Farrens, F Faustini, S Ferriol, M Frailis, E Franceschi, S Galeotta, B Gillis, C Giocoli, P Gómez-Alvarez, A Grazian, F Grupp, SVH Haugan, W Holmes, F Hormuth, A Hornstrup, P Hudelot, S Ilić, K Jahnke, M Jhabvala, B Joachimi, E Keihänen, S Kermiche, A Kiessling, B Kubik, M Kunz, H Kurki-Suonio, S Ligori, PB Lilje, V Lindholm, I Lloro, E Maiorano, O Mansutti, O Marggraf, K Markovic, M Martinelli, N Martinet, F Marulli, R Massey, E Medinaceli, S Mei, Y Mellier, M Meneghetti, E Merlin, G Meylan, M Moresco, L Moscardini, C Neissner

Abstract:

A primary target of the Euclid space mission is to constrain early-universe physics by searching for deviations from a primordial Gaussian random field. A significant detection of primordial non-Gaussianity would rule out the simplest models of cosmic inflation and transform our understanding of the origin of the Universe. This paper forecasts how well field-level inference of galaxy redshift surveys can constrain the amplitude of local primordial non-Gaussianity, f NLlocal, within a Bayesian hierarchical framework, in the upcoming Euclid data. We designed and simulated mock datasets and performed Markov chain Monte Carlo analyses using a full-field forward modelling approach. By including the formation history of the cosmic matter field in the analysis, the method takes into account all available probes of primordial non-Gaussianity, and goes beyond statistical summary estimators of f NLlocal. Probes include, for example, two-point and higher-order statistics, peculiar velocity fields, and scale-dependent galaxy biases. Furthermore, the method simultaneously handles systematic survey effects, such as selection effects, survey geometries, and galaxy biases. The forecast shows that, using simulated Euclid data, the method can achieve a precision of σ(f NLlocal) = 2.6 (68.3% confidence level), assuming a grid resolution of ΔL = 31.25 h −1 Mpc and a cut-off scale of k NF = 0.1 h Mpc−1. We also provide data products, including realistic simulations with non-zero values of f NLlocal and maps of adiabatic curvature fluctuations. The results underscore the feasibility and advantages of field-level inference to constrain f NLlocal in galaxy redshift surveys. Our approach consistently captures all the information available in the large-scale structure to constrain f NLlocal, and resolves the degeneracy between early-universe physics and late-time gravitational effects, while mitigating the impact of systematic and observational effects.
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Euclid: Quick Data Release (Q1) – Secondary nuclei in early-type galaxies

Astronomy and Astrophysics 711 (2026)

Authors:

M Fabricius, R Saglia, F Balzer, LR Ecker, J Thomas, R Bender, J Gracia-Carpio, M Magliocchetti, O Marggraf, A Rawlings, JG Sorce, K Voggel, L Wang, A van der Wel, B Altieri, A Amara, S Andreon, N Auricchio, C Baccigalupi, M Baldi, A Balestra, S Bardelli, A Biviano, E Branchini, M Brescia, J Brinchmann, S Camera, G Cañas-Herrera, V Capobianco, C Carbone, J Carretero, M Castellano, G Castignani, S Cavuoti, KC Chambers, A Cimatti, C Colodro-Conde, G Congedo, CJ Conselice, L Conversi, Y Copin, F Courbin, HM Courtois, M Cropper, H Degaudenzi, G De Lucia, C Dolding, H Dole, F Dubath, CAJ Duncan, X Dupac, S Dusini, S Escoffier, M Farina, R Farinelli, S Ferriol, F Finelli, M Frailis, E Franceschi, M Fumana, S Galeotta, K George, B Gillis, C Giocoli, A Grazian, F Grupp, SVH Haugan, J Hoar, H Hoekstra, W Holmes, IM Hook, F Hormuth, A Hornstrup, K Jahnke, M Jhabvala, B Joachimi, E Keihänen, S Kermiche, A Kiessling, B Kubik, K Kuijken, M Kümmel, M Kunz, H Kurki-Suonio, AMC Le Brun, S Ligori, PB Lilje, V Lindholm, I Lloro, G Mainetti, D Maino, E Maiorano, O Mansutti, M Martinelli, N Martinet, F Marulli, RJ Massey, E Medinaceli, S Mei, Y Mellier

Abstract:

Massive early-type galaxies (ETGs; M > 1011 M⊙) are believed to form primarily through mergers of less massive progenitors, which leave behind numerous traces of violent formation histories, such as stellar streams and shells. A particularly striking signature of these mergers is the formation of supermassive black hole (SMBH) binaries, which can create depleted stellar cores through interactions with stars on radial orbits – a process known as core scouring. The secondary SMBH in such systems may still carry a dense stellar envelope and thereby remain observable for some time as a secondary nucleus while it sinks towards the shared gravitational potential of the merged galaxy. Direct observations of secondary nuclei on sub-kiloparsec scales remain rare, with only a few notable cases, such as NGC 5419. Investigating such features and building up statistics requires both high spatial resolution and wide-field coverage, a capability uniquely provided by Euclid. In this study, we leverage Euclid’s Q1 Early Release data to systematically search for secondary nuclei in ETGs. We present a preliminary sample of 666 candidate systems distributed over 504 hosts (some of which contain multiple secondary nuclei). The vast majority of these fall at separations of 3 kpc to 15 kpc, indicative of normal mergers. However, 44 fall at projected separations of less than 2 kpc. We argue that this most interesting subset of secondary nucleus candidates – those at very close angular separations – are unlikely to be a consequence of chance alignments. We show that their stellar masses are mostly too large for them to be globular clusters and that a significant subset are unresolved even at Euclid’s spatial resolution, rendering them too small to be dwarf galaxies. These objects may represent the highest-density nuclei of a previously merged galaxy currently sinking into the centre of the new common gravitational potential, and thus they likely host a secondary SMBH. We also demonstrate that convolutional neural networks offer a viable avenue to detect multiple nuclei in the 30 times larger sky coverage of the future Euclid DR1. Finally, we argue that our method can detect the remnants of a recoil event from two merged SMBHs, as two of our secondary nuclei candidates are unresolved at the Euclid spatial resolution, appear at projected physical separations of less than 2 kpc, and appear in hosts of M > 1011 M⊙, which makes them viable candidates.
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Euclid: Quick Data Release (Q1) – The connection between galaxy close encounters and radio activity

Astronomy and Astrophysics 711 (2026)

Authors:

M Magliocchetti, A La Marca, L Bisigello, M Bondi, F Ricci, S Fotopoulou, L Wang, R Scaramella, L Pentericci, I Prandoni, JG Sorce, HJA Rottgering, MJ Hardcastle, J Petley, F La Franca, K Rubinur, Y Toba, Y Zhong, M Mezcua, G Zamorani, F Shankar, B Altieri, S Andreon, N Auricchio, C Baccigalupi, M Baldi, S Bardelli, A Biviano, E Branchini, M Brescia, J Brinchmann, S Camera, G Cañas-Herrera, V Capobianco, C Carbone, J Carretero, M Castellano, G Castignani, S Cavuoti, KC Chambers, A Cimatti, C Colodro-Conde, G Congedo, CJ Conselice, L Conversi, Y Copin, A Costille, F Courbin, HM Courtois, M Cropper, A Da Silva, H Degaudenzi, G De Lucia, AM Di Giorgio, H Dole, F Dubath, CAJ Duncan, X Dupac, S Dusini, S Escoffier, M Farina, R Farinelli, F Faustini, S Ferriol, F Finelli, M Frailis, E Franceschi, P Franzetti, M Fumana, S Galeotta, K George, B Gillis, C Giocoli, J Gracia-Carpio, A Grazian, F Grupp, SVH Haugan, J Hoar, W Holmes, IM Hook, F Hormuth, A Hornstrup, K Jahnke, M Jhabvala, B Joachimi, E Keihänen, S Kermiche, A Kiessling, B Kubik, M Kümmel, H Kurki-Suonio, AMC Le Brun, S Ligori, PB Lilje, V Lindholm, I Lloro, G Mainetti, D Maino, E Maiorano, O Mansutti

Abstract:

Using the vast statistics provided by both Euclid and the LOFAR surveys, we present the first large-scale study of the connection among radio emission, its morphology, and the merging properties of the hosts of radio sources up to z ∼ 2. By dividing the radio sample into active galactic nuclei (AGNs) and star-forming galaxies, we find that radio-emitting AGNs show a clear preference for residing within galaxies undergoing a merging event. This is more significant for AGNs that present complex or extended radio emission; indeed, about half of them are associated with merging systems, while only ∼15% are hosted by a non-interacting galaxy. The observed trend is primarily driven by AGNs residing at z < 1, especially in the case of high – P144 MHz > 1024 W Hz−1 sr−1 – radio luminosities (∼56% in mergers versus ∼10% in non-mergers regardless of radio appearance). On the other hand, this preference seems to disappear at higher redshifts, where only bright AGNs with extended radio emission still prefer galaxies undergoing a merging event. The situation is reversed in the case of radio-emitting star-forming galaxies, which are preferentially associated with non-interacting systems. This is more significant as we move towards low-radio-luminosity/star-formation objects (P144 MHz < 1023 W Hz−1 sr−1) for which we find ∼40% in non-mergers versus ∼20% in mergers. These values hold regardless of redshift. We interpreted the above result for AGNs with their need to accrete outer gas from local encounters in order to trigger (radio) activity, especially in the case of extended radio emission such as hot spots and lobes. This is mostly observed at z < 1, since galaxies in the local Universe are more gas deprived than their higher redshift counterparts. Internal gas reservoirs instead seem sufficient to trigger star formation within the majority of galaxies, which indeed mostly appear as non-interacting systems at all redshifts probed.
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