论文标题

使用高强度的XMM-Newton观测值,依赖于时尺的X射线到NGC 4593的UV时间延迟

Timescale-dependent X-ray to UV time lags of NGC 4593 using high-intensity XMM-Newton observations with Swift and AstroSat

论文作者

Beard, Max W. J., McHardy, Ian M., Kumari, Kavita, Dewangan, Gulab C., Papadakis, Iossif, Bhattacharya, Dipankar, Singh, Kulinder Pal, Kynoch, Daniel, Pahari, Mayukh

论文摘要

我们提出了NGC 4593的140K观察结果,XMM-Newton提供了同时且连续的PN X射线和OM UV(UVW12910Å)Lightcurves,它们比以前的观察值更好地样本了短期尺度的变化。这些观察结果与先前报道的22d Swift X射线和紫外线/光学监测,以及Astrosat X射线(SXT)的4D,FAR(FUV1541Å),近距离(NUV2632Å)UV允许它们之间的滞后测量值,并在它们之间进行滞后测量和XMM较高的XMM。从XMM中,我们发现UVW1落后于X射线29.5 $ \ pm $ 1.3KS,$ \ sim $ half先前从SWIFT监视中确定的滞后。 \ textit {swift}数据的重新检查显示了双峰滞后分布,并有长长和短滞后的证据。但是,如果我们以5D宽度的Lowess过滤来减轻Swift Lightcurves,则仅保留较短的滞后(23.8 $ \ pm $ 21.2ks)。与PN和SXT相比,NUV观察结果确认了XMM发现的$ \ sim $ 30KS滞后,并且在应用4D过滤以删除长时间计算组件后,FUV显示了$ \ sim $ 23KS的滞后。所得的新的UVW1,FUV和NUV滞后频谱延伸至X射线频带,而无需额外的X射线以延长紫外线滞后偏移,如果X射线的重新处理产生,则意味着重新处理器的直接照明。通过参考先前的SWIFT和HST滞后测量,我们获得了光学滞后频谱的X射线,该光谱与使用Kynreverb Disc-Repropersing代码的模型一致,假设接受的质量为$ 7.63 \ times10^{6} M _ {\ odot} $ 7.63 \ times10^{6} {\ odot} $,并获得了旋转接近最大值。以前指出的BLR在Balmer和Paschen Continua中的滞后贡献仍然很突出。

We present a 140ks observation of NGC 4593 with XMM-Newton providing simultaneous and continuous PN X-ray and OM UV (UVW1 2910Å) lightcurves which sample short-timescale variations better than previous observations. These observations were simultaneous with 22d of Swift X-ray and UV/optical monitoring, reported previously, and 4d of AstroSat X-ray (SXT), far (FUV 1541Å), and near (NUV 2632Å) UV allowing lag measurements between them and the highly-sampled XMM. From the XMM we find that UVW1 lags behind the X-rays by 29.5$\pm$1.3ks, $\sim$half the lag previously determined from the Swift monitoring. Re-examination of the \textit{Swift} data reveals a bimodal lag distribution, with evidence for both the long and short lags. However if we detrend the Swift lightcurves by LOWESS filtering with a 5d width, only the shorter lag (23.8$\pm$21.2ks) remains. The NUV observations, compared to PN and SXT, confirm the $\sim$30ks lag found by XMM and, after 4d filtering is applied to remove the long-timescale component, the FUV shows a lag of $\sim$23ks. The resultant new UVW1, FUV, and NUV lag spectrum extends to the X-ray band without requiring additional X-ray to UV lag offset, which if the UV arises from reprocessing of X-rays, implies direct illumination of the reprocessor. By referencing previous Swift and HST lag measurements, we obtain an X-ray to optical lag spectrum which agrees with a model using the KYNreverb disc-reprocessing code, assuming the accepted mass of $7.63\times10^{6}M_{\odot}$ and a spin approaching maximum. Previously noted lag contribution from the BLR in the Balmer and Paschen continua are still prominent.

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