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PROFILE SHAPES FOR OPTICALLY THICK X-RAY EMISSION LINES FROM STELLAR WINDS

机译:星状风的光学X射线放射线的轮廓形状

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We consider the consequences of appreciable line optical depth for the profile shape of X-ray emission lines formed in stellar winds. The hot gas is thought to arise in distributed wind shocks, and the line formation is predominantly via collisional excitation followed by radiative decay. Such lines are often modeled as optically thin, but the theory has difficulty matching resolved X-ray line profiles. We suggest that for strong lines of abundant metals, newly created photons may undergo resonance scattering, modifying the emergent profile. Using Sobolev theory in a spherically symmetric wind, we show that thick-line resonance scattering leads to emission profiles that still have blueshifted centroids, like the thin lines, but are considerably less asymmetric in appearance. We focus on winds in the constant-expansion domain and derive an analytic form for the profile shape in the limit of large line and photoabsorptive optical depths. In this limit the emission profile reduces to a universal shape and has a centroid shift of ― 0.24v_∞, with a half-width at half-maximum (HWHM) of 0.63v_∞. Using published data for Chandra observations of five emission lines from the O star ζ Pup, we find that the observed HWHMs are somewhat smaller than predicted by our theory; however, the centroid shifts of all five lines are consistent with our theoretical result. These optical depth effects can potentially explain the more nearly symmetric emission lines observed in ζ Ori, θ~1 Ori C, and δ Ori by Chandra, although an alternative explanation is required to account for the unshifted peak line emission. We also consider enhanced reabsorption by continuous opacity as line photons multiply scatter within an optically thick line, and find, for lines with optical depths of a few, that such reabsorption can further reduce the line asymmetry. It also reduces the line equivalent width, but probably not enough to alleviate the problem of subsolar metallicities inferred from O star X-ray spectra by ASCA, unless the width of the resonance regions are super-thermally enhanced.
机译:我们考虑了明显的光学深度对于恒星风中形成的X射线发射线轮廓形状的影响。据认为,热气是在分散的风冲击中产生的,线的形成主要是通过碰撞激发,然后是辐射衰减。通常将此类线建模为光学上较细的线,但该理论很难匹配解析的X射线线轮廓。我们建议对于大量金属的强线,新创建的光子可能会发生共振散射,从而改变出射轮廓。在球形对称风中使用Sobolev理论,我们证明了粗线共振散射会导致发射轮廓仍然像蓝线一样具有蓝移质心,但是外观上的不对称性大大降低。我们将重点放在恒定扩展域中的风中,并在大线和光吸收光学深度的极限中得出轮廓形状的解析形式。在此限制下,发射轮廓减小为通用形状,并且质心偏移为〜0.24v_∞,半峰半宽(HWHM)为0.63v_∞。使用已发表的数据对Chandra观测到的O星ζPup的5条发射线进行观测,我们发现观测到的HWHM略小于我们的理论预测的值。但是,所有五条线的质心偏移都与我们的理论结果一致。这些光学深度效应可以潜在地解释Chandra在ζOri,θ〜1 Ori C和δOri中观察到的更加对称的发射线,尽管需要其他解释来解释未移动的峰值线发射。我们还考虑了由于线光子在光学粗线内增加散射而通过连续的不透明度增强的重吸收,并且发现对于光学深度为几的线,这种重吸收可以进一步减少线的不对称性。它也减小了线的等效宽度,但可能不足以缓解由ASCA从O星X射线光谱推断出的次太阳金属性的问题,除非共振区域的宽度得到了超高温增强。

著录项

  • 来源
    《The Astrophysical journal》 |2002年第1期|p.954-964|共11页
  • 作者

    R. IGNACE; K. G. GAYLEY;

  • 作者单位

    Department of Physics and Astronomy, 203 Van Allen Hall, University of Iowa, Iowa City, IA 52242;

  • 收录信息
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类 天文学;
  • 关键词

  • 入库时间 2022-08-18 01:52:05

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