The Transitional Type Ibn/IIn SN 2022pda, with Pre-explosion Outbursts and a Double-peaked Light Curve

The Astrophysical Journal Letters American Astronomical Society 1004:2 (2026) l37

Authors:

Y-Z Cai, A Pastorello, R Chiba, TJ Moriya, A Reguitti, L Tartaglia, S Moran, S Campana, Z-Y Wang, J-W Zhao, JP Anderson, S Benetti, SJ Brennan, E Cappellaro, KC Chambers, T-W Chen, Z-H Chen, T de Boer, Y-Z Dong, J Duarte, N Elias-Rosa, M Fraser, W-P Gan, H Gao, M Gromadzki, G Hosseinzadeh, DA Howell, C Inserra, T Kangas, E Kankare, T Kravtsov, L-P Li, C-C Lin, TB Lowe, P Lundqvist, EA Magnier, K Matilainen, PA Mazzali, C McCully, P Minguez, TE Müller-Bravo, M Newsome, E Padilla Gonzalez, C Pellegrino, PJ Pessi, T Petrushevska, G Pignata, RP Santos, S Schulze, SJ Smartt, IA Smith, KW Smith, J Sollerman, S Srivastav, MD Stritzinger, G Terreran, G Valerin, R Wainscoat, S-Q Wang, DR Young, L Galbany, Z Li, I Salmaso, S Zha, J-M Bai, B Wang, X-F Wang, J-J Zhang

Abstract:

We report the results of a photometric and spectroscopic follow-up campaign of the unusual interacting supernova (SN) 2022pda. Precursor variability lasting ∼100 days is observed before the explosion. The SN light curve has a double-peak shape. It reached a first maximum of Mr = −19.6 ± 0.2 mag, followed by an initial 2 month decline and a second, broad peak lasting about 6 months. The early spectra show a blue continuum with dominant H and He emission lines. A high-resolution pre-maximum spectrum shows that the profile of the He i λ 5876 line consists of a moderately narrow (∼1900 km s−1) P Cygni absorption superposed on a broader (∼3300 km s−1) component. In the blue region, several spectral features are identified, including C iii/N iii/O ii blends. Two broad bumps at 4600–5200 Å and 6400–6800 Å regions reveal a complex profile, which are likely due to blends of H, He, and other emission lines. Late-time spectra are still dominated by prominent and broad H and He lines in emission. Shock-driven model fits to the bolometric light curve suggest that the SN is powered by interaction with a massive CSM with enhanced mass-loss rates ∼5 M⊙yr−1, expelled during two events that occurred ∼1 and ∼0.2 yr before the explosion. The overall SN evolution indicates that SN 2022pda is a transitional event between an H-rich SN IIn (SN 2009ip-like) and an He-rich SN Ibn. Our findings suggest that the progenitor was likely a luminous blue variable transitioning towards a Wolf–Rayet stage.

TITAN DR1: An Improved, Validated, and Systematically Controlled Recalibration of ATLAS Photometry toward Type Ia Supernova Cosmology

The Astrophysical Journal American Astronomical Society 1004:2 (2026) 173

Authors:

Elijah G Marlin, Yukei S Murakami, Dillon Brout, Jack W Tweddle, Brodie Popovic, Ken W Smith, Stephen J Smartt, Daniel M Scolnic, David Jones, Erik R Peterson, Adam G Riess, Maria Vincenzi, Nora F Sherman, Maria Acevedo, Jasper Milstein, Mitchell Dixon, Armin Rest

Abstract:

ATLAS (Asteroid Terrestrial Last Alert System) is a time-domain survey using four telescopes, covering the entire sky. It has observed 8378 spectroscopically confirmed Type Ia supernovae (SNe Ia), with thousands of cosmology-grade light curves (to be released as TITAN DR1). To prepare this massive, low-redshift dataset for cosmology, we evaluate and cross-calibrate ATLAS forced photometry using tertiary stars from the DES (Dark Energy Survey) Y6 release. The 5000 deg2 DES footprint overlaps regions both in and out of the PS1 (Pan-STARRS DR1) footprint, allowing tests of the primary calibrator for the ATLAS Refcat2 catalog. Initial offsets are at the ∼40 mmag scale. To improve this, we determine Δ zero-point offsets for two cases: (1) pixel-to-pixel offsets within individual CCDs (reduced from ∼8 to ∼4 mmag rms) and (2) chip-to-chip offsets across the nine CCDs and filters (reduced from ∼17 to ∼3 mmag rms). We also identify the largest systematic uncertainty as a transmission-function color dependence, requiring shifts in the assumed ATLAS filters at the ∼30 mmag level if uncorrected. We validate our calibration using (a) CALSPEC standards, (b) an independent tertiary catalog, and (c) distance moduli of cross-matched SNe Ia, all showing improved consistency. Overall, we estimate combined calibration-related systematics at the ∼5–10 mmag level, supporting competitive cosmological constraints with the TITAN SN Ia dataset.

Observational Biases and Improved Modelling of Off-axis Relativistic Jets

(2026)

Authors:

AJ Cooper, AP Scott, L Rhodes, F Carotenuto, AK Hughes, JH Matthews, K Savard, FJ Cowie, EL Elley, C Lilje, R Fender

Towards improved synchrotron self absorption energy estimates: accounting for inhomogeneous and non-spherical emitting regions

Monthly Notices of the Royal Astronomical Society Oxford University Press (OUP) (2026) stag1113

Authors:

FJ Cowie, RP Fender

Abstract:

Abstract Synchrotron self absorption (SSA) is seen across a variety of astrophysical sources, and observation of an SSA peak in the spectrum is a powerful tool for estimating the physical conditions and the minimum energy of the emitting region. We begin with the (re)derivation of the usual SSA parameter estimates, carefully considering dependencies and assumptions, obtaining the most accurate traditional SSA minimum energy equations currently available. Traditional methods rely on the assumption that the emitting region is quasi-spherical and homogeneous. However, many observations of SSA show that the spectral index at frequencies below the peak is less than the expected +2.5 (non-thermal) or +2 (thermal). We argue that an inhomogeneous emitting region is the most likely explanation in many cases. Power law inhomogeneous cylindrical slab and broken power law inhomogeneous sphere models are used to investigate how the presence of inhomogeneity affects parameter estimates using traditional SSA methods. We find that in some cases inhomogeneity can lead to traditional SSA methods underestimating the minimum energy and the size of the emitting region by over an order of magnitude. Quantitative correction factors are found which can be applied to traditional estimates to correct for inhomogeneity, depending on the value of the observed flattened spectral index and the range in frequency over which this value is observed. Furthermore, we derive simple correction factors for non-spherical homogeneous emitting regions. Finally, we explore the effects of inhomogeneity on measurements of polarisation around the spectral peak, and on lightcurves for expanding emitting regions.

Chasing Gamma-Ray Signals from Binary Neutron Star Coalescences with the Cherenkov Telescope Array: Prospects and Observing Strategies

The Astrophysical Journal American Astronomical Society 1004:1 (2026) 46

Authors:

S Abe, J Abhir, A Abhishek, F Acero, A Acharyya, R Adam, A Aguasca-Cabot, I Agudo, I Albanese, J Alfaro, C Alispach, R Alves Batista, E Amato, G Ambrosi, D Ambrosino, F Ambrosino, L Angel, C Aramo, A Arbet-Engels, C Arcaro, C Arena, TTH Arnesen, K Asano, H Ashkar, C Bakshi, C Balazs, M Balbo, A Baquero Larriva, V Barbosa Martins, JA Barrio, C Bartolini, I Batković, R Batzofin, N Bavdaz, J Becerra González, G Beck, W Benbow, E Bernardini, MG Bernardini, J Bernete, A Berti, B Bertucci, V Beshley, P Bhattacharjee, S Bhattacharyya, C Bigongiari, A Biland, E Bissaldi, M Blaña, O Blanch, J Blazek, C Boisson, G Bonnoli, Z Bosnjak, E Bottacini, M Böttcher, E Bronzini, G Brunelli, J Buces Sáez, A Bulgarelli, T Bulik, L Burmistrov, PG Calisse, A Campoy-Ordaz, BK Cantlay, G Capasso, A Caproni, R Capuzzo-Dolcetta, M Cardillo, S Caroff, A Carosi, E Carquin, S Casanova, E Cascone, F Cassol, G Castignani, F Catalani, D Cerasole, M Cerruti, A Cerviño Cortínez, PM Chadwick, S Chaty, AW Chen, Y Chen, M Chernyakova, A Chiavassa, G Chon, J Chudoba, L Chytka, GM Cicciari, A Cifuentes Santos, CH Coimbra Araujo, JL Contreras, B Cornejo, J Cortina, A Costa, G Cotter, P Cristofari, O Cuevas, Z Curtis-Ginsberg, A D’Aì, G D’Amico, F D’Ammando, P D’Avanzo, P Da Vela, L David, F Dazzi, M de Bony de Lavergne, V De Caprio, EM de Gouveia Dal Pino, B De Lotto, M de Naurois, V de Souza, L del Peral, MV del Valle, C Delgado, D della Volpe, D Depaoli, A Dettlaff, L Di Bella, T Di Girolamo, A Di Piano, F Di Pierro, R Di Tria, L Di Venere, R Dima, A Dinesh, E Do Souto Espiñeira, D Dominis Prester, A Donini, D Dorner, J Dörner, M Doro, L Ducci, VV Dwarkadas, J Ebr, C Eckner, K Egberts, L Eisenberger, D Elsässer, G Emery, C Escañuela Nieves, P Escarate, M Escobar Godoy, J Escudero Pedrosa, P Esposito, D Falceta-Goncalves, E Fedorova, S Fegan, K Feijen, Q Feng, G Ferrand, E Fiandrini, A Fiasson, M Filipovic, V Fioretti, L Foffano, G Fontaine, F Frías García-Lago, Y Fukazawa, Y Fukui, G Galanti, G Galaz, S Gallozzi, V Gammaldi, S García Soto, M Garczarczyk, C Gasbarra, D Gasparrini, M Gaug, G Ghirlanda, JG Giesbrecht Formiga Paiva, N Giglietto, F Giordano, M Giroletti, R Giuffrida, J-F Glicenstein, P Goldoni, JM González, J Goulart Coelho, T Gradetzke, J Granot, R Grau, D Green, JG Green, J Grube, J Hackfeld, D Hadasch, A Hahn, P Hamal, W Hanlon, S Hara, VM Harvey, T Hassan, K Hayashi, B Hess, L Heckmann, N Hiroshima, B Hnatyk, R Hnatyk, D Horan, P Horvath, D Hrupec, S Hussain, M Iarlori, T Inada, F Incardona, S Inoue, F Iocco, A Iuliano, Jahanvi, M Jamrozy, P Janecek, F Jankowsky, C Jarnot, I Jaroschewski, P Jean, V Jilek, I Jiménez Martínez, J Jimenez Quiles, W Jin, E Joshi, J Jurysek, V Karas, H Katagiri, J Kataoka, S Kaufmann, T Keita, D Kerszberg, M Kherlakian, DB Kieda, R Kissmann, T Kleiner, Y Kobayashi, K Kohri, D Kolar, N Komin, A Kong, K Kosack, D Kostunin, G Kowal, H Kubo, J Kushida, A La Barbera, N La Palombara, B Lacave, M Láinez, A Lamastra, J Lapington, S Lazarević, J-P Lenain, F Leone, E Leonora, G Leto, E Lindfors, S Lombardi, F Longo, R López-Coto, M López-Moya, A López-Oramas, J Lozano Bahilo, PL Luque-Escamilla, E Lyard, O Macias, P Majumdar, M Makariev, D Mandat, S Mangano, A Marchetti, M Mariotti, S Markoff, I Márquez, G Marsella, J Martí, D Martín Domínguez, M Martínez, O Martinez, G Maurin, D Mazin, D Melkumyan, S Menon, E Mestre, DM-A Meyer, D Miceli, M Miceli, M Michailidis, T Miener, JM Miranda, R Moderski, M Molero, C Molfese, E Molina, K Morik, A Morselli, E Moulin, AL Müller, K Munari, T Murach, A Muraczewski, H Muraishi, T Nakamori, L Nava, R Nemmen, J Niemiec, D Nieto, M Nievas Rosillo, M Nikołajuk, L Nikolić, K Noda, D Nosek, V Novotny, S Nozaki, A Okumura, RA Ong, R Orito, M Orlandini, E Orlando, S Orlando, J Otero-Santos, I Oya, M Ozlati Moghadam, A Pagliaro, M Palatiello, A Pandey, G Panebianco, D Paneque, FR Pantaleo, JM Paredes, B Patricelli, A Pe’er, M Pech, M Pecimotika, M Peresano, E Peretti, J Pérez-Romero, G Peron, F Perrotta, M Persic, O Petruk, F Pfeifle, E Pietropaolo, M Pihet, L Pinchbeck, F Pintore, G Pirola, C Pittori, F Podobnik, M Pohl, V Pollet, G Ponti, E Prandini, G Principe, M Prouza, E Pueschel, G Pühlhofer, ML Pumo, M Punch, A Quirrenbach, S Rainò, R Rando, S Recchia, A Reimer, O Reimer, I Reis, A Reisenegger, W Rhode, M Ribó, C Ricci, T Richtler, J Rico, L Riitano, V Rizi, E Roache, G Rodriguez Fernandez, JJ Rodríguez-Vázquez, P Romano, G Romeo, J Rosado, A Rosales de Leon, A Roy, I Sadeh, L Saha, T Saito, M Sánchez-Conde, P Sangiorgi, H Sano, R Santos-Lima, V Sapienza, S Sarkar, FG Saturni, A Scherer, F Schiavone, P Schipani, P Schovanek, F Schussler, M Seglar Arroyo, O Sergijenko, H Siejkowski, A Simongini, V Sliusar, A Slowikowska, I Sofia, H Sol, S Spinello, A Stamerra, S Stanič, T Starecki, R Starling, Ł Stawarz, T Stolarczyk, Y Suda, A Sunny, T Suomijarvi, R Takeishi, SJ Tanaka, F Tavecchio, T Tavernier, Y Terada, M Teshima, V Testa, WW Tian, Y Tian, L Tibaldo, O Tibolla, SJ Tingay, CJ Todero Peixoto, F Tombesi, D Tonev, F Torradeflot, DF Torres, N Tothill, G Tovmassian, G Tripodo, A Trois, A Tsiahina, A Tutone, L Vaclavek, M Vacula, C van Eldik, J Vandenbroucke, V Vassiliev, M Vázquez Acosta, M Vecchi, S Vercellone, SD Vergani, I Viale, A Viana, A Vigliano, J Vignatti, CF Vigorito, J Villanueva, E Visentin, V Voitsekhovskyi, S Vorobiov, I Vovk, T Vuillaume, R Walter, M Wechakama, M White, A Wierzcholska, M Will, F Wohlleben, A Wolter, F Xotta, T Yamamoto, R Yamazaki, T Yoshikoshi, M Zacharias, G Zaharijas, R Zanmar Sanchez, D Zavrtanik, M Zavrtanik, A Zech, VI Zhdanov, M Živec, J Zuriaga-Puig, A Colombo

Abstract:

The detection of gravitational waves (GWs) from a binary neutron star (BNS) merger by Advanced LIGO and Advanced Virgo (GW170817), together with its electromagnetic counterpart, the short gamma-ray burst GRB 170817A, heralded the birth of multimessenger astronomy. The detection of TeV emission from GRBs motivates follow-up observations with the Cherenkov Telescope Array Observatory (CTAO), which is ideal for detecting such signals due to its unprecedented sensitivity, rapid response, and wide-field survey capabilities. The aim of this work is to evaluate GeV–TeV GW follow-up strategies for CTAO using a multistep simulation pipeline and to estimate the expected rate of joint GW–GRB detections during observing run O5. Using a simulated sample of BNS systems with corresponding GW detections, gamma-ray emission is simulated through phenomenological prescriptions based on the observed population of short GRBs, including off-axis jet scenarios. CTAO observations are simulated to account for instrument response, sky tiling strategies, integration times, and varying observing conditions. Strategies with variable and constant integration times are investigated. We find that, via an optimized follow-up strategy, about 5% of simulated GW-associated short GRBs produce GeV–TeV radiation detectable by CTAO. Detectability is strongly influenced by the jet opening angle and viewing angle, suggesting that even rough estimates of the viewing angle in GW alerts could enhance targeting. This framework motivates future follow-ups of GW-detectable events, including neutron star–black hole mergers, and further supports the development of advanced strategies incorporating galaxy distributions and synergies with future detectors such as the Einstein Telescope.