首页> 外文期刊>Astronomy and astrophysics >SNR 1E 0102.2-7219 as an X-ray calibration standard in the 0.5?1.0 keV bandpass and its application to the CCD instruments aboard Chandra, Suzaku, Swift and XMM-Newton
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SNR 1E 0102.2-7219 as an X-ray calibration standard in the 0.5?1.0 keV bandpass and its application to the CCD instruments aboard Chandra, Suzaku, Swift and XMM-Newton

机译:SNR 1E 0102.2-7219作为0.5?1.0 keV带通中的X射线校准标准,并在Chandra,Suzaku,Swift和XMM-Newton上的CCD仪器中应用

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Context. The flight calibration of the spectral response of charge-coupled device (CCD) instruments below 1.5 keV is difficult in general because of the lack of strong lines in the on-board calibration sources typically available. This calibration is also a function of time due to the effects of radiation damage on the CCDs and/or the accumulation of a contamination layer on the filters or CCDs. Aims. We desire a simple comparison of the absolute effective areas of the current generation of CCD instruments onboard the following observatories: Chandra ACIS-S3, XMM-Newton (EPIC-MOS and EPIC-pn), Suzaku XIS, and Swift XRT and a straightforward comparison of the time-dependent response of these instruments across their respective mission lifetimes. Methods. We have been using 1E 0102.2-7219, the brightest supernova remnant in the Small Magellanic Cloud, to evaluate and modify the response models of these instruments. 1E 0102.2-7219 has strong lines of O, Ne, and Mg below 1.5 keV and little or no Fe emission to complicate the spectrum. The spectrum of 1E 0102.2-7219 has been well-characterized using the RGS gratings instrument on XMM-Newton and the HETG gratings instrument on Chandra. As part of the activities of the International Astronomical Consortium for High Energy Calibration (IACHEC), we have developed a standard spectral model for 1E 0102.2-7219 and fit this model to the spectra extracted from the CCD instruments. The model is empirical in that it includes Gaussians for the identified lines, an absorption component in the Galaxy, another absorption component in the SMC, and two thermal continuum components with different temperatures. In our fits, the model is highly constrained in that only the normalizations of the four brightest lines/line complexes (the O?vii Heα triplet, O?viii Lyα line, the Ne?ix Heα triplet, and the Ne?x Lyα line) and an overall normalization are allowed to vary, while all other components are fixed. We adopted this approach to provide a straightforward comparison of the measured line fluxes at these four energies. We have examined these measured line fluxes as a function of time for each instrument after applying the most recent calibrations that account for the time-dependent response of each instrument. Results. We performed our effective area comparison with representative, early mission data when the radiation damage and contamination layers were at a minimum, except for the XMM-Newton EPIC-pn instrument which is stable in time. We found that the measured fluxes of the O?vii Heαr line, the O?viii Lyα line, the Ne?ix Heαr line, and the Ne?x Lyα line generally agree to within ±10% for all instruments, with 38 of our 48 fitted normalizations within ± 10% of the IACHEC model value. We then fit all available observations of 1E 0102.2-7219 for the CCD instruments close to the on-axis position to characterize the time dependence in the 0.5?1.0 keV band. We present the measured line normalizations as a function of time for each CCD instrument so that the users may estimate the uncertainty in their measured line fluxes for the epoch of their observations.
机译:上下文。低于1.5 keV的电荷耦合器件(CCD)仪器的光谱响应的飞行校准通常很困难,因为通常可用的板载校准源中缺少强线。由于辐射损坏对CCD和/或滤光器或CCD上污染层的积累,该校准也是时间的函数。目的我们希望对以下观测站上的当前CCD仪器的绝对有效面积进行简单比较:Chandra ACIS-S3,XMM-Newton(EPIC-MOS和EPIC-pn),Suzaku XIS和Swift XRT,并进行直接比较这些仪器在其各自的任务寿命中随时间变化的响应。方法。我们一直在使用1E 0102.2-7219(麦哲伦星云中最亮的超新星遗迹)来评估和修改这些仪器的响应模型。 1E 0102.2-7219在1.5 keV以下具有强的O,Ne和Mg谱线,很少或没有Fe发射,使光谱复杂化。使用XMM-Newton上的RGS光栅仪器和Chandra上的HETG光栅仪器已很好地表征了1E 0102.2-7219的光谱。作为国际高能校准天文学联合会(IACHEC)活动的一部分,我们已经开发了1E 0102.2-7219的标准光谱模型,并将该模型与从CCD仪器中提取的光谱进行拟合。该模型是经验模型,因为它包括已识别线的高斯,银河中的吸收分量,SMC中的另一个吸收分量以及两个温度不同的热连续体分量。在我们的拟合中,该模型受到严格限制,因为仅对四个最亮的线/线复合体(O?viiHeα三重态,O?viiiLyα系,Ne?ixHeα三重态和Ne?xLyα系)进行归一化)和总体规格化允许变化,而所有其他组件均固定不变。我们采用这种方法来提供这四种能量下测得的线通量的直接比较。在应用了考虑了每种仪器随时间变化的响应的最新校准之后,我们已经检查了每种仪器的这些测得的线通量与时间的关系。结果。当辐射破坏和污染层最小时,我们用代表性的早期任务数据进行了有效面积比较,但时间稳定的XMM-Newton EPIC-pn仪器除外。我们发现,对于所有仪器,O?viiHeαr谱线,O?viiiLyα谱线,Ne?ixHeαr谱线和Ne?xLyα谱线的测量通量通常都在±10%以内在IACHEC模型值的±10%范围内进行了48个拟合的归一化。然后,我们将1E 0102.2-7219的所有可用观测值拟合到靠近轴上位置的CCD仪器,以表征0.5?1.0 keV频带中的时间依赖性。我们介绍了每种CCD仪器的测量线归一化与时间的关系,以便用户可以估计其观测时期的测量线通量中的不确定性。

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