Identification of the Optical Counterpart of the Fast X-Ray Transient EP240414a

The Astrophysical Journal Letters American Astronomical Society 978:2 (2025) L21

Authors:

S Srivastav, T-W Chen, JH Gillanders, L Rhodes, SJ Smartt, ME Huber, A Aryan, S Yang, A Beri, AJ Cooper, M Nicholl, KW Smith, HF Stevance, F Carotenuto, KC Chambers, A Aamer, CR Angus, MD Fulton, T Moore, IA Smith, DR Young, T de Boer, H Gao, C-C Lin

Abstract:

Fast X-ray transients (FXTs) are extragalactic bursts of X-rays first identified in archival X-ray data and are now routinely discovered in real time by the Einstein Probe, which is continuously surveying the night sky in the soft (0.5–4 keV) X-ray regime. In this Letter, we report the discovery of the second optical counterpart (AT 2024gsa) to an FXT (EP 240414a). EP 240414a is located at a projected radial separation of 27 kpc from its likely host galaxy at z = 0.4018 ± 0.0010. The optical light curve of AT 2024gsa displays three distinct components. The initial decay from our first observation is followed by a rebrightening episode, displaying a rapid rise in luminosity to an absolute magnitude Mr ∼ −21 after two rest-frame days. While the early optical luminosity and decline rate are similar to those of luminous fast blue optical transients, the color temperature of AT 2024gsa is distinctly red and we show that the peak flux is inconsistent with a thermal origin. The third component peaks at Mi ∼ −19 at ≳16 rest-frame days post-FXT, and is compatible with an emerging supernova. We fit the riz-band data with a series of power laws and find that the decaying components are in agreement with gamma-ray burst afterglow models, and that the rebrightening may originate from refreshed shocks. By considering EP 240414a in context with all previously reported known-redshift FXT events, we propose that Einstein Probe FXT discoveries may predominantly result from (high-redshift) gamma-ray bursts, and thus appear to be distinct from the previously discovered lower-redshift, lower-luminosity population of FXTs.

Peculiar radio-bright behaviour of the Galactic black hole transient 4U 1543-47 in the 2021-2023 outburst

(2025)

Authors:

X Zhang, W Yu, F Carotenuto, SE Motta, R Fender, JCA Miller-Jones, TD Russell, A Bahramian, P Woudt, AK Hughes, GR Sivakoff

The ubiquity of variable radio emission and spin-down rates in pulsars

(2025)

Authors:

ME Lower, A Karastergiou, S Johnston, PR Brook, S Dai, M Kerr, RN Manchester, LS Oswald, RM Shannon, C Sobey, P Weltevrede

Long-term optical variations in Swift J1858.6–0814: evidence for ablation and comparisons to radio properties

Monthly Notices of the Royal Astronomical Society Oxford University Press (OUP) 536:4 (2025) 3421-3430

Authors:

L Rhodes, DM Russell, P Saikia, K Alabarta, J van den Eijnden, AH Knight, MC Baglio, F Lewis

X-Ray and Optical Polarization Aligned with the Radio Jet Ejecta in GX 339–4

The Astrophysical Journal Letters American Astronomical Society 978:2 (2025) L19

Authors:

G Mastroserio, B De Marco, MC Baglio, F Carotenuto, S Fabiani, TD Russell, F Capitanio, Y Cavecchi, S Motta, DM Russell, M Dovčiak, M Del Santo, K Alabarta, A Ambrifi, S Campana, P Casella, S Covino, G Illiano, E Kara, EV Lai, G Lodato, A Manca, I Mariani, A Marino

Abstract:

We present the first X-ray polarization measurements of GX 339–4. IXPE observed this source twice during its 2023–2024 outburst, once in the soft-intermediate state and again during a soft state. The observation taken during the intermediate state shows a significant (4σ) polarization degree PX = 1.3% ± 0.3% and polarization angle θX = −74° ± 7° only in the 3–8 keV band. FORS2 at the Very Large Telescope observed the source simultaneously, detecting optical polarization in the B, V, R, and I bands (between ∼0.1% and ∼0.7%), all roughly aligned with the X-ray polarization. We also detect a discrete jet knot from radio observations with the Australia Telescope Compact Array taken later in time; this knot would have been ejected from the system around the same time as the hard-to-soft X-ray state transition, and a bright radio flare occurred ∼3 months earlier. The proper motion of the jet knot provides a direct measurement of the jet orientation angle on the plane of the sky at the time of the ejection. We find that both the X-ray and optical polarization angles are aligned with the direction of the ballistic jet.