Publications of the Astronomical Society of Japan · 2019 · 10 citations · 53 references
Natural SciencesAstronomyPhysicsAstrophysicsSpectroscopyX-ray AstronomyExtragalactic X-ray SourcesSolar FlaresX-ray SpectroscopyX-ray TimingEmission FluxesHard X-ray BackgroundHard X-ray Solar FlaresPhoton EmissionStellar X-ray RadiationX-ray Emission From Active StarsX-ray Source DetectionX-ray Spectral Analysis
Abstract X-ray observations play a crucial role in understanding the emission mechanism and relevant physical phenomena of magnetars. We report on X-ray observations made in 2016 of a young magnetar, SGR 1900+14, which is famous for a giant flare in 1998 August. Simultaneous observations were conducted with XMM-Newton and NuSTAR on 2016 October 20 with 23 and 123 ks exposures, respectively. The NuSTAR hard X-ray coverage enabled us to detect the source up to 70 keV. The 1–10 keV and 15–60 keV fluxes were $3.11(3)\times 10^{-12} \, {\rm erg \, s^{-1} \, cm^{-2}}$ and $6.8(3)\times 10^{-12} \, {\rm erg \, s^{-1} \, cm^{-2}}$, respectively. The 1–70 keV spectra were fitted well by a blackbody plus power-law model with a surface temperature of $kT=0.52(2) \, {\rm keV}$, a photon index of the hard power-law of Γ = 1.21(6), and a column density of $N_{\,\rm H}=1.96(11)\times 10^{22} \, {\rm cm^{-2}}$. Compared with previous observations with Suzaku in 2006 and 2009, the 1–10 keV flux showed a decrease by 25%–40%, while the spectral shape did not show any significant change with differences of kT and NH being within 10% of each other. Through timing analysis, we found that the rotation period of SGR 1900+14 on 2016 October 20 was $5.22669(3) \, {\rm s}$. The long-term evolution of the rotation period shows a monotonic decrease in the spin-down rate $\dot{P}$ lasting for more than 15 yr. We also found characteristic behavior of the hard-tail power-law component of SGR 1900+14. The energy-dependent pulse profiles vary in morphology with a boundary of 10 keV. The phase-resolved spectra show the differences between photon indices (Γ = 1.02–1.44) as a function of the pulse phase. Furthermore, the photon index is positively correlated with the X-ray flux of the hard power-law component, which could not be resolved by the previous hard X-ray observations.
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