An Archival Optical Counterpart Search for Extragalactic Fast X-Ray Transients Discovered by Einstein Probe

The Astrophysical Journal American Astronomical Society 999:2 (2026) 239

Authors:

Run-Duo Liang, Wen-Xiong Li, Liang-Duan Liu, Ken W Smith, Stephen J Smartt, Qin-Yu Wu, Niu Li, Arne Rau, Ling-Zhi Wang, Armin Rest, Ning-Chen Sun, Franz E Bauer, Ezequiel Treister, Jia-Sheng Huang, Jennifer Chacón, Seán J Brennan, Matt Nicholl, Ting-Wan Chen, Amar Aryan, Sheng Yang, Albert KH Kong, Sofia Rest, Qi-Nan Wang, James H Gillanders

Abstract:

Extragalactic fast X-ray transients (eFXTs) represent a rapidly growing class of high-energy phenomena, whose physical origins remain poorly understood. With its wide-field, sensitive all-sky monitoring, the Einstein Probe (EP) has greatly increased the discovery rate of eFXTs. The search for and identification of the optical counterparts of eFXTs are vital for understanding their classification and constraining their physical origin. Yet, a considerable fraction of eFXTs still lack secure classifications due to the absence of timely follow-up observations. We carry out a systematic search of publicly available optical survey data and transient databases (including the Zwicky Transient Facility and the Transient Name Server) for optical counterparts to eFXT candidates detected by EP. In this paper, we describe our ongoing program and report the first results. Specifically, we identified the eFXT EP240506a to be associated with a UV/optical counterpart, AT 2024ofs. Spectroscopy of its host galaxy with the Very Large Telescope yields a redshift of z = 0.120 ± 0.002. By combining archival survey data with early-time multiwavelength observations, we find that the luminosity and light-curve evolution of AT 2024ofs are consistent with a core-collapse supernova origin. From detectability simulations, we estimate a local event rate density ρ0=8.8−3.9+21.2yr−1Gpc−3 for EP240506a-like events, and completeness-corrected rate of about 36–78 yr−1 Gpc−3 for EP-detected X-ray transients associated with supernovae. Our results demonstrate the potential of EP to uncover prompt high-energy emission from core-collapse supernovae and underscore the critical importance of timely follow-up of future eFXT events.

Massive stars exploding in a He-rich circumstellar medium

Astronomy & Astrophysics EDP Sciences 707 (2026) a157

Authors:

Y-Z Cai, A Pastorello, K Maeda, J-W Zhao, Z-Y Wang, Z-H Peng, A Reguitti, L Tartaglia, AV Filippenko, Y Pan, G Valerin, B Kumar, Z Wang, M Fraser, JP Anderson, S Benetti, S Bose, TG Brink, E Cappellaro, T-W Chen, X-L Chen, N Elias-Rosa, A Esamdin, A Gal-Yam, M González-Bañuelos, M Gromadzki, CP Gutiérrez, C Inserra, A Iskandar, T Kangas, E Kankare, T Kravtsov, H Kuncarayakti, L-P Li, C-X Liu, X-K Liu, P Lundqvist, K Matilainen, S Mattila, S Moran, TE Müller-Bravo, T Nagao, T Petrushevska, G Pignata, I Salmaso, SJ Smartt, J Sollerman, S Srivastav, MD Stritzinger, L-T Wang, S-Y Yan, Y Yang, Y-P Yang, W Zheng, X-Z Zou, L-Y Chen, X-L Du, Q-L Fang, A Fiore, F Ragosta, S Zha, J-J Zhang, X-W Liu, J-M Bai, B Wang, X-F Wang

Abstract:

We present a photometric and spectroscopic analyses of the Type Ibn supernova (SN) 2024acyl. It rises to an absolute magnitude peak of M o = −17.58 ± 0.15 mag in 10.6 days, and displays a rapid linear post-peak light-curve decline in all bands (e.g. γ 0 − 60 ( V ) = 0.097 ± 0.002 mag day −1 ), similar to most SNe Ibn. The optical pseudobolometric light curve peaks at (3.5 ± 0.8)×10 42 erg s −1 , with a total radiated energy of (5.0 ± 0.4)×10 48 erg. The spectra are dominated by a blue continuum at early stages, with narrow P-Cygni He  I lines and flash-ionisation emission lines of C  III , N  III , and He  II . The P-Cygni He  I features gradually evolve and become emission-dominated in late-time spectra. The H α line is detected throughout the entire spectral evolution, which indicates that the circumstellar material (CSM) is helium-rich with some residual amount of hydrogen. Our multi-band light-curve modelling yields estimates of the ejecta mass of M ej = 0.49 +0.11 −0.09 M ⊙ with a kinetic energy of E k = 0.06 +0.01 −0.01 × 10 51 erg, and a 56 Ni mass of M Ni = 0.018 M ⊙ . The inferred CSM properties are characterised by a mass of M CSM = 0.51 +0.05 −0.04 M ⊙ , an inner radius of R 0 =17.8 +3.6 −3.0 AU, and a density of ρ CSM = (8.3 +2.7 −1.2 ) × 10 −12 g cn −3 . The multi-epoch spectra are well reproduced by the CMFGEN/ he4p0 model, corresponding to a He-ZAMS mass of 4 M ⊙ (H-ZAMS mass 18.11 M ⊙ , pre-SN mass 3.16 M ⊙ ). These findings are consistent with a scenario of an SN powered by ejecta-CSM interaction originating from a low-mass helium star that evolved within an interacting binary system where the CSM with some residual hydrogen may originate from the mass-transfer process. We also discuss an extreme scenario involving the possible merger of a helium white dwarf. In addition, a channel of core-collapse explosion of a late-type Wolf-Rayet (WR) star with hydrogen, or a transitional star between an Of and a WR type (e.g. an Ofpe/WN9 star) with fallback accretion cannot be entirely ruled out.

Origin of radio polarization in pulsar polar caps

Astronomy & Astrophysics EDP Sciences 707 (2026) A316-A316

Authors:

Jan Benáček, Axel Jessner, Martin Pohl, Tatiana Rievajová, Lucy S Oswald

Abstract:

Context. It is crucial to know the polarization properties of coherent radio waves that escape from pulsar polar caps to calculate the radiative transfer through the magnetosphere and to predict observable radio properties. Aims. We describe pair cascades in the pulsar polar cap, and we determine for the first time the Stokes parameters of the escaping radio waves from first-principle kinetic simulations for a pulsar with a magnetic obliquity of 60°. Methods. We present 3D particle-in-cell kinetic simulations that include quantum-electrodynamic pair cascades in a charge-limited flow from the stellar surface. Results. Our model quantitatively and qualitatively explains the observed pulsar radio powers and spectra, the pulse profiles, polarization curves, their temporal variability, the strong Stokes- L and weak Stokes- V polarization components, the decline in the linear polarization with frequency, and the nonexistence of a radius-to-frequency relation. The observable properties of radio emission from the polar cap can vary and include single- or double-peaked profiles. Most of the Stokes V curves from our simulations appear to be antisymmetric, but symmetric curves are also present at some viewing angles. Although the polarization-angle (PA) swing of the radiation from the polar cap fits the rotating vector model (RVM) for most viewing angles, the angles obtained from the RVM do not correspond to the dipole geometry of the magnetic field. Instead, the PA is directly related to the plasma flows in the polar cap. Furthermore, we found that the radiation is associated with escaping plasma bunches and can propagate freely along channels of low plasma density, in addition to being reflected at the channel boundaries. Conclusions. Our simulations demonstrate that pair discharges close to the surface of the polar cap cause the radio emission of pulsars and determine the majority of their typically observed properties. The merits of RVM for estimations of the magnetic field geometry from observations need to be reevaluated.

SN 2024hpj: A perspective on SN 2009ip-like events

Astronomy & Astrophysics EDP Sciences 707 (2026) a80

Authors:

I Salmaso, A Pastorello, E Borsato, S Benetti, MT Botticella, Y-Z Cai, N Elias-Rosa, A Farina, M Fraser, L Galbany, M González-Bañuelos, CP Gutiérrez, M Huang, P Lundqvist, T Kangas, TL Killestein, T Kravtsov, K Matilainen, A Morales-Garoffolo, A Mura, G Pignata, A Reguitti, TM Reynolds, S Smartt, S Srivastav, L Tartaglia, G Valerin, Z-Y Wang

Abstract:

Supernovae (SNe) IIn are terminal explosions of massive stars that are surrounded by a dense circumstellar medium (CSM). Among SNe IIn, a notable subset is the SN 2009ip-like, which exhibits an initial, fainter peak attributed to stellar variability in the late evolutionary stages, followed by a brighter peak, interpreted as the SN explosion itself. In this context, we analysed the spectrophotometric evolution of SN 2024hpj, an object with a triple-peaked light curve and spectra typical of a SN IIn but with a complex line profile composed of broad P-Cygni features topped by narrow emissions. Comparing it with other SN 2009ip-like events in the literature, as well as with other unpublished objects (SNe 2019mry, 2022ytx, 2024uzf, and 2025csc), we identify star-forming regions as their preferred formation environment. On the other hand, the diversity of spectrophotometric features within the sample suggests that variations in CSM mass and distribution may influence the observed characteristics. We identify four sub-classes based on the luminosity and rapidity of the light curve evolution, which provides insights into possible differences in the progenitors, while a statistical analysis of their observed rate indicates progenitor masses around 25 − 31 M ⊙ or lower.

Scrutinizing the 2020 multiwavelength outburst of PKS 0903 - 57 through observations with H.E.S.S

Journal of High Energy Astrophysics Elsevier (2026) 100599

Authors:

A Acharyya, F Aharonian, F Ait Benkhali, A Alkan, H Ashkar, M Backes, V Barbosa Martins, R Batzofin, Y Becherini, D Berge, K Bernlöhr, B Bi, M Böttcher, C Boisson, J Bolmont, J Borowska, R Brose, A Brown, F Brun, B Bruno, T Bulik, C Burger-Scheidlin, S Casanova, J Celic, M Cerruti, S Chandra, A Chen, M Chernyakova, JO Chibueze, O Chibueze, B Cornejo, G Cotter, G Cozzolongo, J Damascene Mbarubucyeye, J de Assis Scarpin, M de Naurois, E de Oña Wilhelmi, AG Delgado Giler, J Devin, A Djannati-Ataï, J Djuvsland, A Dmytriiev, V Doroshenko, K Egg, S Einecke, J-P Ernenwein, C Escañuela Nieves, K Feijen, MD Filipovic, G Fontaine, S Funk, S Gabici, YA Gallant, M Genaro, JF Glicenstein, P Goswami, G Grolleron, L Haerer, L Heckmann, G Hermann, B Heß, JA Hinton, W Hofmann, TL Holch, M Holler, D Horns, M Jamrozy, F Jankowsky, I Jung-Richardt, E Kasai, K Katarzyński, D Kerszberg, R Khatoon, B Khélifi, W Kluźniak, N Komin, D Kostunin, RG Lang, A Lemière, J-P Lenain, A Luashvili, J Mackey, D Malyshev, V Marandon, G Martí-Devesa, R Marx, M Mayer, A Mehta, AMW Mitchell, R Moderski, MO Moghadam, L Mohrmann, A Montanari, E Moulin, D Moyeni, J Niemiec, L Olivera-Nieto, S Panny, M Panter, RD Parsons, U Pensec, S Pita, G Pühlhofer, A Quirrenbach, M Regeard, A Reimer, O Reimer, HX Ren, B Reville, F Rieger, G Rowell, B Rudak, K Sabri, V Sahakian, H Salzmann, M Sasaki, J Schäfer, F Schüssler, HM Schutte, JNS Shapopi, A Sharma, W Si Said, H Sol, S Spencer, Ł Stawarz, R Steenkamp, S Steinmassl, C Steppa, T Takahashi, T Tanaka, AM Taylor, C Van Eldik, M Vecchi, J Vink, T Wach, SJ Wagner, A Wierzcholska, M Zacharias, AA Zdziarski, A Zech, N Zywucka

Abstract:

The blazar PKS 0903 - 57 has recently been classified as a flat spectrum radio quasar at a redshift of z = 0.2621 . In March and April 2020, Fermi-LAT and AGILE reported tremendous activity in high-energy γ rays with the flux increasing by  ∼ 2 orders of magnitude compared to quiescence. The flare was observed with H.E.S.S. in very-high-energy γ rays for six nights with a total observation time of 13.1 h, resulting in the discovery of PKS 0903 - 57 in this energy band with an average flux of 1.5 × 10 − 10 ph cm − 2 s − 1 above an energy threshold of  ∼ 180 GeV corresponding to 60% of the Crab Nebula flux above the same threshold. The very-high-energy γ-ray flux was strongly variable. X-ray and optical data were collected with Swift and ATOM, and also indicate significant variability. The observed multiwavelength flux and spectral variability during the H.E.S.S. observation window suggest variability time scales on the order of a few hours and reveal complex correlation patterns. The lack of absorption beyond that of the extragalactic background light in the γ-ray domain suggests that the emission region was located outside of the broad-line region. A leptonic one-zone modeling of the six H.E.S.S. observation nights using the dusty torus as seed photons for the inverse-Compton scattering, results in a low magnetization of the emission region. This implies that shock acceleration is likely the main driver during the event.