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Detection and luminosity-dependent evolution of the high-energy hump in the Be/X-ray pulsar 1A 1118-61

Published 15 Jun 2026 in astro-ph.HE | (2606.16805v1)

Abstract: Context. Accreting X-ray pulsars exhibit strong luminosity-dependent changes in their broad-band spectra. At high luminosities, their spectra are usually described by a power-law continuum with a high-energy cutoff, whereas low-luminosity observations have revealed a two-hump spectral morphology. Aims. We aim to trace the luminosity-dependent spectral evolution of the Be/X-ray pulsar 1A 1118-61 and to constrain the luminosity range over which the high-energy hump becomes clearly distinguishable. Methods. We use dense SRG/ART-XC and Insight-HXMT monitoring, together with three broad-band NuSTAR observations of 1A 1118-61 obtained during its 2026 outburst, to trace the luminosity-dependent evolution of the spectral shape. The ART-XC data follow the decay from a peak luminosity of ≃7×10<sup>37\simeq7\times10<sup>{37} erg s<sup>−1<sup>{-1} to a low-luminosity plateau at ≃(3\simeq(3-8)×10<sup>358)\times10<sup>{35} erg s<sup>−1<sup>{-1} in the 4-35 keV band, while the NuSTAR observations provide broad-band spectra during the bright phase, the decline, and the plateau. We describe the continuum with a phenomenological two-component Comptonization model. Results. As the source faded, the broad-band continuum developed a distinct high-energy hump, giving rise to a two-hump morphology with broad maxima near ∼\sim10 keV and ∼\sim30-40 keV. The ART-XC monitoring constrains the transition to this morphology to L4−35≃(0.8L_{4-35}\simeq(0.8-1.8)×10<sup>361.8)\times10<sup>{36} erg s<sup>−1<sup>{-1}. We also find a break in the luminosity dependence of the flux ratio between the two continuum humps around L4−35∼10<sup>37L_{4-35}\sim10<sup>{37} erg s<sup>−1<sup>{-1}. A cyclotron line at ≃55\simeq55 keV is detected in the high-energy hump, with no significant luminosity dependence of its centroid energy. We discuss this behavior in the context of resonant interactions in the magnetized accretion flow.

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