论文标题
磁性早期的B型星星IV:突破或泄漏? H $α$排放作为离心磁层中血浆传输的诊断
The Magnetic Early B-type Stars IV: Breakout or Leakage? H$α$ emission as a diagnostic of plasma transport in centrifugal magnetospheres
论文作者
论文摘要
具有强磁场的快速旋转的早期型恒星经常显示出源自离心机磁层(CMS)的H $α$发射,在磁性限制的磁性稳固性磁性下,在磁性强迫启动引起的磁性下降剂的情况下,它可以积聚到高增密。目前尚不知道CM等离子体是通过离心突破(CB)还是通过未识别的泄漏机制逃脱的。我们已经对目前已知显示CM图案排放的所有恒星的H $α$排放特性进行了首次全面检查。我们发现,发射的开始主要取决于CM的面积,在Kepler Corotation Radius $ r _ {\ rm K} $上,磁场的值$ b _ {\ rm k} $可以简单地预测。排放强度对CM区域和$ b _ {\ rm K} $非常敏感。发射开始和强度取决于有效温度,发光度或质量损失率。这些结果都有利于CB方案,但是任何CM诊断中缺乏固有的可变性表明CB必须是一个基本上是连续的过程,即\ \有效地充当泄漏机制。我们还表明,在广泛的发射强度和恒星参数中,发射曲线形状大致相当不变,即它们在广泛的发射强度和恒星参数上大致相似。尽管最大排放的半径与$ r _ {\ rm k} $紧密相关,但始终更大,矛盾的模型可以预测发射应达到$ r _ {\ rm k} $。
Rapidly rotating early-type stars with strong magnetic fields frequently show H$α$ emission originating in Centrifugal Magnetospheres (CMs), circumstellar structures in which centrifugal support due to magnetically enforced corotation of the magnetically confined plasma enables it to accumulate to high densities. It is not currently known whether the CM plasma escapes via Centrifugal Breakout (CB), or by an unidentified leakage mechanism. We have conducted the first comprehensive examination of the H$α$ emission properties of all stars currently known to display CM-pattern emission. We find that the onset of emission is dependent primarily on the area of the CM, which can be predicted simply by the value $B_{\rm K}$ of the magnetic field at the Kepler corotation radius $R_{\rm K}$. Emission strength is strongly sensitive to both CM area and $B_{\rm K}$. Emission onset and strength are {\em not} dependent on effective temperature, luminosity, or mass-loss rate. These results all favour a CB scenario, however the lack of intrinsic variability in any CM diagnostics indicates that CB must be an essentially continuous process, i.e.\ it effectively acts as a leakage mechanism. We also show that the emission profile shapes are approximately scale-invariant, i.e.\ they are broadly similar across a wide range of emission strengths and stellar parameters. While the radius of maximum emission correlates closely as expected to $R_{\rm K}$, it is always larger, contradicting models that predict that emission should peak at $R_{\rm K}$.