SIMBAD references

2024ApJ...976...99S - Astrophys. J., 976, 99 (2024/November-3)

GTC Optical/Near-infrared Upper Limits and NICER X-Ray Analysis of SGR J1935+2154 for the Outburst in 2022.

SHAO Y.-X., ZHOU P., LI X.-D., ZHANG B.-B., CASTRO-TIRADO A.J., WANG P., LI D., ZHANG Z.-H., ZHANG Z.-J., HU Y.-D. and PANDEY S.B.

Abstract (from CDS):

The Galactic magnetar SGR J1935+2154 has undergone another outburst since 2022 October 10. We present the results of searching for an optical/near-infrared (NIR) counterpart of SGR J1935+2154 before and during this outburst. No counterpart was detected at the magnetar's position in $r^{\prime} $ and $z^{\prime} $ bands, providing stringent upper limits of $r^{\prime} \gtrsim 28.65$ and $z^{\prime} \gtrsim 26.27$. Using archival X-ray data from NICER, we investigated the properties of the bursts and the spectral evolution of persistent emission. The burst flux F showed a power-law distribution of N ∝ F–0.76±0.10 for flux ≳2.6 × 10–9erg cm–2 s–1, while the temperature and radius followed a log-normal distribution with ${kT}={1.63}_{-0.50}^{+0.73}\ \mathrm{keV}$ and ${R}_{\mathrm{bb}}={4.35}_{-1.35}^{+1.95}\ \mathrm{km}$, respectively. The persistent flux evolution experienced a quick decay and an enhancement ∼27 days after the Burst Alert Telescope trigger. Using the NIR and X-ray emission, together with the Gran Telescopio Canarias optical/NIR upper limits, we discussed the origin of the NIR emission from the magnetar based on the fallback disk model and magnetosphere model. We found that either model cannot be ruled out with currently available data. Further mid-infrared observations are needed to find out the mechanism for producing the NIR emission from SGR J1935+2154.

Abstract Copyright: © 2024. The Author(s). Published by the American Astronomical Society.

Journal keyword(s): Magnetars - Neutron stars - Soft gamma-ray repeaters - X-ray bursts - X-ray transient sources

Status at CDS : Large table(s) will be appraised for possible ingestion in VizieR.

Simbad objects: 8

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