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The neutron star transient and millisecond pulsar in M28: from sub-luminous accretion to rotation-powered quiescence

机译:m28中的中子星瞬态和毫秒脉冲星:来自   副发光增加旋转动力静止

摘要

The X-ray transient IGR J18245-2452 in the globular cluster M28 contains thefirst neutron star (NS) seen to switch between rotation-powered andaccretion-powered pulsations. We analyse its 2013 March-April 25d-long outburstas observed by Swift, which had a peak bolometric luminosity of ~6% of theEddington limit (L$_{E}$), and give detailed properties of the thermonuclearburst observed on 2013 April 7. We also present a detailed analysis of new andarchival Chandra data, which we use to study quiescent emission from IGRJ18245-2452 between 2002 and 2013. Together, these observations cover almostfive orders of magnitude in X-ray luminosity (L$_X$, 0.5-10 keV). The Swiftspectrum softens during the outburst decay (photon index $\Gamma$ from 1.3above L$_X$/L$_{E}$=10$^{-2}$ to ~2.5 at L$_X$/L$_{E}$=10$^{-4}$), similar toother NS and black hole (BH) transients. At even lower luminosities, deepChandra observations reveal hard ($\Gamma$=1-1.5), purely non-thermal andhighly variable X-ray emission in quiescence. We therefore find evidence for aspectral transition at L$_X$/L$_{E}$~10$^{-4}$, where the X-ray spectralsoftening observed during the outburst decline turns into hardening as thesource goes to quiescence. Furthermore, we find a striking variability patternin the 2008 Chandra light curves: rapid switches between a high-L$_X$ "active"state (L$_X\simeq$3.9x10$^{33}$ erg/s) and a low-L$_X$ "passive" state(L$_X\simeq$5.6x10$^{32}$ erg/s), with no detectable spectral change. We putour results in the context of low luminosity accretion flows around compactobjects and X-ray emission from millisecond radio pulsars. Finally, we discusspossible origins for the observed mode switches in quiescence, and explore ascenario where they are caused by fast transitions between the magnetosphericaccretion and pulsar wind shock emission regimes.
机译:球状星团M28中的X射线瞬态IGR J18245-2452包含第一个中子星(NS),该星在旋转动力和增生动力脉冲之间切换。我们分析了Swift观测到的2013年3月至4月25天长的突突,其辐射热峰值约为爱丁顿极限(L $ _ {E} $)的6%,并给出了2013年4月7日观测到的热核爆的详细属性我们还提供了对新的Andarcharch Chandra数据的详细分析,这些数据用于研究IGRJ18245-2452在2002年至2013年之间的静态发射。这些观测结果一起涵盖了X射线光度的几乎五个数量级(L $ _X $,0.5 -10 keV)。爆发频谱衰减时,Swiftspectrum变软(光子索引$ \ Gamma $从L $ _X $ / L $ _ {E} $ = 10 $ ^ {-2} $以上的1.3升至L $ _X $ / L $ _的〜2.5 {E} $ = 10 $ ^ {-4} $),类似于其他NS和黑洞(BH)瞬变。在更低的光度下,深钱德拉的观测结果显示出硬的($ \ Gamma $ = 1-1.5),纯粹的非热态和静态的高度可变X射线发射。因此,我们发现在L $ _X $ / L $ _ {E} $〜10 $ ^ {-4} $处出现纵横过渡的证据,在该处,在爆发下降期间观察到的X射线光谱软化随着光源进入静止状态而变硬。此外,我们在2008年的Chandra光曲线中发现了惊人的可变性模式:在高L $ _X $“活动”状态(L $ _X \ simeq $ 3.9x10 $ ^ {33} $ erg / s)和低L $ _X $个“被动”状态(L $ _X \ simeq $ 5.6x10 $ ^ {32} $ erg / s),没有可检测到的光谱变化。我们的结果是在紧凑物体周围的低发光体积聚流和毫秒级无线电脉冲星发出的X射线的情况下得出的。最后,我们讨论了静态观测模式切换的可能起源,并探讨了由磁层吸积和脉冲星风冲击发射机制之间的快速过渡引起的情景。

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