论文标题
XMM-Newton和Chandra的观察结果Fermi-Lat Pulsar 4FGL J1015.5-6030
XMM-Newton and Chandra observations of the candidate Fermi-LAT pulsar 4FGL J1015.5-6030
论文作者
论文摘要
4FGL J1015.5-6030是一个未识别的费米 - 拉特源,它具有明亮的X射线源,其X射线频谱与年轻的Pulsar的X射线频谱一致,但没有发现脉动。在这里,我们报告了4FGL J1015.5-6030的XMM-Newton定时和Chandra成像观测值。我们发现来自来源的明显周期性没有明显的周期性,并在其34 $ \%$的脉冲分数上放置3 $σ$上限。 Chandra的观察结果从延长的发射中解析了点源。我们发现该点源的频谱非常适合黑体模型,温度$ kt = 0.205 \ pm0.009 $ keV,还有一个弱的幂律组件,这与带有磁层成分的热发射中子星一致。从点源及其频谱的延长发射跨越了几个弧度的角度尺度,其频谱非常适合具有光子指数$γ= 1.70 \ pm0.05 $的幂律模型。扩展的发射频谱和0.5-10的keV光度为4 $ \ times10^{32} $ erg s $^{ - 1} $(在2 kpc的距离为2 kpc)与脉冲星nebula的一致。基于与其他GEV和X射线脉冲星的比较,我们发现这种推定的Pulsar可能是中年(即$τ\ sim 0.1 $ -1 $ -1 Myr)带有$ \ dot {e} \ sim10^\ sim10^{34} {34} {34} -10^{35} $ erg s $ erg s $ $ eRG s $^s $^1}的无线电pulsar。
4FGL J1015.5-6030 is an unidentified Fermi-LAT source hosting a bright, extended X-ray source whose X-ray spectrum is consistent with that of a young pulsar, yet no pulsations have been found. Here we report on XMM-Newton timing and Chandra imaging observations of the X-ray counterpart of 4FGL J1015.5-6030. We find no significant periodicity from the source and place a 3$σ$ upper-limit on its pulsed fraction of 34$\%$. The Chandra observations resolve the point source from the extended emission. We find that the point source's spectrum is well fit by a blackbody model, with temperature $kT=0.205\pm0.009$ keV, plus a weak power-law component, which is consistent with a thermally emitting neutron star with a magnetospheric component. The extended emission spans angular scales of a few arcseconds up to about 30$''$ from the point source and its spectrum is well fit by a power-law model with a photon index $Γ=1.70\pm0.05$. The extended emission's spectrum and 0.5-10 keV luminosity of 4$\times10^{32}$ erg s$^{-1}$ (at a plausible distance of 2 kpc) are consistent with that of a pulsar wind nebula. Based on a comparison to other GeV and X-ray pulsars, we find that this putative pulsar is likely a middle-aged (i.e., $τ\sim 0.1$--1 Myr) radio-quiet pulsar with $\dot{E}\sim10^{34}-10^{35}$ erg s$^{-1}$.