Can tidal disruption event models reliably measure black hole masses?

Monthly Notices of the Royal Astronomical Society Oxford University Press (OUP) (2026) stag1285

Authors:

CR Angus, AJ Smith, D Magill, P Ramsden, N Sarin, M Nicholl, B Mockler, E Hammerstein, R Stein, Y Yao, T de Boer, KC Chambers, ME Huber, C-C Lin, TB Lowe, EA Magnier, SJ Smartt, RJ Wainscoat

Abstract:

Abstract Tidal disruption event (TDE) light curves are increasingly used to infer the masses of quiescent supermassive black holes (MBH), offering a powerful probe of low-mass black hole demographics independent of host-galaxy scaling relations. However, most semi-analytic TDE models invoke assumptions aligned with a full stellar disruption, despite theoretical expectations that partial disruptions dominate the TDE population. In this work we test the robustness of current TDE models using three repeating partial TDEs (rpTDEs), in which the multiple flares produced by the same surviving stellar core must yield consistent black hole masses. We present spectroscopic observations establishing AT 2023adr as a rpTDE, making it the third such spectroscopically confirmed event. We independently model the flares of the three rpTDEs; 2020vdq, 2022dbl, and 2023adr, applying fallback-accretion fits, stream–stream collision scaling relations, luminosity-based empirical relations, accretion disc models, and cooling-envelope fits. After accounting for statistical and model-specific systematics, we find that all TDE models generally return self-consistent MBH values between flares, and are broadly consistent with host-galaxy MBH proxies, recovering MBH to within 0.3–0.5 dex. However, the convergence of fallback models towards unphysical stellar masses and impact parameters reveals limitations in existing fallback model grids. We also show that light curve coverage, particularly in the near-ultraviolet, is critical for constraining model parameters. This has direct implications for interpreting the thousands of TDE light curves expected from upcoming surveys such as the Rubin Observatory’s Legacy Survey of Space and Time, where from MOSFiT simulations, we find that MBH may be underestimated on average by 0.1 – 0.5 dex depending on peak light curve coverage and the availability of follow-up data.

Spectropolarimetric detection of baryonic mass loading in a transient relativistic jet: application to the black hole X-ray binary Swift J1727.8−1613

Monthly Notices of the Royal Astronomical Society Oxford University Press (OUP) (2026) stag1283

Authors:

AK Hughes, RP Fender, GR Sivakoff, FJ Cowie, I Heywood, JH Matthews, K Savard, F Carotenuto, TD Russell, CM Wood, MC Baglio, S Corbel, SE Motta

Abstract:

Abstract Radio emission during X-ray binary outbursts is dominated by synchrotron radiation from relativistic jets, but is usually studied through total-intensity diagnostics such as flux density, spectra, variability, and proper motion. Radio spectropolarimetry provides a complementary probe of the magneto-ionic plasma through Faraday rotation and depolarisation. When the Faraday rotating material is local to the source, these effects can constrain the jet plasma composition and mass content, but this approach is rarely applied to transient jetted sources. We present MeerKAT L-band spectropolarimetry of the black hole X-ray binary Swift J1727 during its 2023 outburst, focusing on the brightest radio flaring interval, when relativistic jets were being launched intermittently. Using multiple spectropolarimetric techniques, we identify transient Faraday-complex structure coincident with the major radio flares. The close temporal association with the flaring activity, together with the stability of the foreground Faraday screen, favours an origin local to the jet rather than in the ISM or in a separate local screen external to the emitting plasma. Since internal Faraday rotation is suppressed in a pure electron–positron plasma, the data favour a dominant electron–proton component. Interpreting the characteristic Faraday thickness as internal rotation, and anchoring the magnetic-field and size scales with synchrotron self-absorption arguments, we infer a characteristic Faraday-rotating mass of order Mrot ~ 1021 g, corresponding to only a small fraction, frot ~ 10−3, of the accreted mass available during the flare. These results show that time-domain spectropolarimetry can turn transient Faraday complexity into a diagnostic of jet composition, mass loading, and plasma evolution in X-ray binary outbursts, and potentially other transient jetted sources.

Extreme particle acceleration in X-ray binaries is linked to their jets

(2026)

Authors:

Laura Olivera-Nieto, Fraser J Cowie, Sera Markoff, Rob Fender, Justine Crook-Mansour

Spectropolarimetric detection of baryonic mass loading in a transient relativistic jet: application to the black hole X-ray binary Swift J1727.8$-$1613

(2026)

Authors:

AK Hughes, RP Fender, GR Sivakoff, FJ Cowie, I Heywood, JH Matthews, K Savard, F Carotenuto, TD Russell, CM Wood, MC Baglio, S Corbel, SE Motta

Euclid Quick Data Release (Q1)

Astronomy & Astrophysics EDP Sciences 711 (2026) a8

Authors:

L Quilley, I Damjanov, V de Lapparent, A Paulino-Afonso, H Domínguez Sánchez, A Ferré-Mateu, M Huertas-Company, M Kümmel, D Delley, C Spiniello, M Baes, L Wang, U Kuchner, F Tarsitano, R Ragusa, M Siudek, C Tortora, N Aghanim, B Altieri, A Amara, S Andreon, N Auricchio, H Aussel, C Baccigalupi, M Baldi, A Balestra, S Bardelli, P Battaglia, R Bender, A Biviano, A Bonchi, D Bonino, E Branchini, M Brescia, J Brinchmann, S Camera, G Cañas-Herrera, V Capobianco, C Carbone, J Carretero, S Casas, FJ Castander, 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, C Dolding, H Dole, CAJ Duncan, X Dupac, S Dusini, S Escoffier, M Fabricius, M Farina, R Farinelli, F Faustini, S Ferriol, P Fosalba, S Fotopoulou, M Frailis, E Franceschi, S Galeotta, K George, B Gillis, C Giocoli, J Gracia-Carpio, BR Granett, A Grazian, F Grupp, SVH Haugan, H Hoekstra, W Holmes, IM Hook, F Hormuth, A Hornstrup, P Hudelot, K Jahnke, M Jhabvala, B Joachimi, E Keihänen, S Kermiche, A Kiessling, B Kubik, M Kunz, H Kurki-Suonio, Q Le Boulc’h, AMC Le Brun, D Le Mignant, P Liebing, S Ligori, PB Lilje, V Lindholm, I Lloro, G Mainetti, D Maino, E Maiorano, O Mansutti, S Marcin, O Marggraf, M Martinelli, N Martinet, F Marulli, R Massey, S Maurogordato, HJ McCracken, E Medinaceli, S Mei, M Melchior, Y Mellier, M Meneghetti, E Merlin, G Meylan, A Mora, M Moresco, L Moscardini, R Nakajima, 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, R Saglia, Z Sakr, AG Sánchez, D Sapone, B Sartoris, JA Schewtschenko, P Schneider, M Scodeggio, A Secroun, G Seidel, M Seiffert, S Serrano, P Simon, C Sirignano, G Sirri, L Stanco, 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, G Verdoes Kleijn, A Veropalumbo, Y Wang, J Weller, A Zacchei, G Zamorani, FM Zerbi, IA Zinchenko, E Zucca, V Allevato, M Ballardini, M Bolzonella, E Bozzo, C Burigana, R Cabanac, A Cappi, D Di Ferdinando, JA Escartin Vigo, L Gabarra, WG Hartley, J Martín-Fleitas, S Matthew, N Mauri, RB Metcalf, A Pezzotta, M Pöntinen, C Porciani, I Risso, V Scottez, M Sereno, M Tenti, M Viel, M Wiesmann, Y Akrami, IT Andika, S Anselmi, M Archidiacono, F Atrio-Barandela, C Benoist, K Benson, D Bertacca, M Bethermin, L Bisigello, A Blanchard, L Blot, S Borgani, ML Brown, S Bruton, F Buitrago, A Calabro, B Camacho Quevedo, F Caro, CS Carvalho, T Castro, Y Charles, F Cogato, T Contini, AR Cooray, O Cucciati, S Davini, F De Paolis, G Desprez, A Díaz-Sánchez, JJ Diaz, S Di Domizio, JM Diego, P-A Duc, A Enia, Y Fang, AG Ferrari, PG Ferreira, A Finoguenov, A Franco, K Ganga, J García-Bellido, T Gasparetto, V Gautard, R Gavazzi, E Gaztanaga, F Giacomini, G Gozaliasl, M Guidi, CM Gutierrez, A Hall, C Hernández-Monteagudo, H Hildebrandt, J Hjorth, O Ilbert, JJE Kajava, Y Kang, V Kansal, D Karagiannis, K Kiiveri, CC Kirkpatrick, S Kruk, L Legrand, M Lembo, F Lepori, G Leroy, GF Lesci, J Lesgourgues, L Leuzzi, TI Liaudat, A Loureiro, J Macias-Perez, G Maggio, M Magliocchetti, EA Magnier, C Mancini, F Mannucci, R Maoli, CJAP Martins, L Maurin, M Miluzio, P Monaco, C Moretti, G Morgante, K Naidoo, A Navarro-Alsina, S Nesseris, F Passalacqua, K Paterson, L Patrizii, A Pisani, D Potter, S Quai, M Radovich, P-F Rocci, S Sacquegna, M Sahlén, DB Sanders, E Sarpa, C Scarlata, J Schaye, A Schneider, D Sciotti, E Sellentin, F Shankar, LC Smith, SA Stanford, K Tanidis, G Testera, R Teyssier, S Tosi, A Troja, M Tucci, C Valieri, A Venhola, D Vergani, G Verza, P Vielzeuf, NA Walton, JG Sorce, E Soubrie, D Scott

Abstract:

We present the results of the single-component Sérsic profile fitting for the magnitude-limited sample of I E < 23 galaxies within the 63.1 deg 2 area of the Euclid Quick Data Release (Q1). The associated morphological catalogue includes two sets of structural parameters fitted using SourceXtractor++ : one for VIS I E images and one for a combination of three NISP images in Y E , J E , and H E bands. We compared the resulting Sérsic parameters to other morphological measurements provided in the Q1 data release and to the equivalent parameters based on higher-resolution Hubble Space Telescope imaging. These comparisons confirmed the consistency and the reliability of the fits to Q1 data. Our analysis of colour gradients shows that NISP profiles systematically have smaller effective radii ( R e ) and larger Sérsic indices ( n ) than in VIS. In addition, we highlight trends in NISP-to-VIS parameter ratios with both magnitude and n VIS . From the 2D bimodality of the ( u − r ) colour-log( n ) plane, we defined a ( u − r ) lim ( n ) that separates early- and late-type galaxies (ETGs and LTGs). We used the two sub-populations to examine the variations of n across well-known scaling relations at z < 1. The ETGs display a steeper size–stellar mass relation than the LTGs, indicating a difference in the main drivers of their mass assembly. Similarly, LTGs and ETGs occupy different parts of the stellar mass–star-formation rate plane, with ETGs at higher masses than LTGs and further below the main sequence of star-forming galaxies. This clear separation highlights the link known between the shutdown of star formation and morphological transformations in the Euclid imaging data set. In conclusion, our analysis demonstrates both the robustness of the Sérsic fits available in the Q1 morphological catalogue and the wealth of information they provide for studies of galaxy evolution with Euclid .