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arXiv · 2502.19743

Insight-HXMT observations on thermonuclear X-ray bursts from 4U~1608--52 in the low/hard state: the energy-dependant hard X-ray deficit and cooling saturation of the corona

Abstract

During thermonuclear bursts, it is suspected that {\bf the cooling of the corona by the burst emission} may be the cause of hard X-ray {\bf deficits}. Although this {\bf deficit} has been observed in nine sources, it has not been observed {\bf from} 4U~1608--52, a nearby prolific burster. Therefore, the authenticity and universality of the hard X-ray {\bf deficit} may be in question. To investigate this suspicion, Insight-HXMT performed cadence observations during the low/hard state of 4U~1608--52 in September 2022 and detected 10 thermonuclear X-ray bursts. Two of these bursts show a double-peaked structure in the soft X-ray band, which could be caused by the high temperature of the burst emission and a marginal photospheric radius expansion (PRE) around the burst peak time. This is indicated by their peak fluxes being up to the Eddington limit and having a large color factor at the peak of the bursts. The hard X-ray deficit is significantly observed during bursts at $>$ 30 keV. Furthermore, the fraction of this deficit shows saturation at 50\% for the first 8 bursts. This saturation may indicate that the corona is layered and only a part of the corona is cooled by the bursts. For example, the part close to the NS surface is cooled while the rest remains intact during bursts. This result provides a clue to the geometry of the corona, e.g., a possible scenario is that the corona has two forms: a quasi-spheric corona between the NS and the disk, and a disk-corona on both surfaces of the disk.

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Y. P. Chen, S. Zhang, L. Ji, S. N. Zhang, J. Q. Peng, L. D. Kong, Z. Chang, Q. C. Shui, L. Tao, J. L. Qu, M. Y. Ge, J. Li. 2025-02-27. Insight-HXMT observations on thermonuclear X-ray bursts from 4U~1608--52 in the low/hard state: the energy-dependant hard X-ray deficit and cooling saturation of the corona. https://doi.org/10.1093/mnras%2Fstae1257

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