论文标题
在碰撞风力的汤姆森散射中对光学到紫外线变异性建模
Modeling the Optical to Ultraviolet Polarimetric Variability from Thomson Scattering in Colliding Wind Binaries
论文作者
论文摘要
巨大的恒星二进制是测量质量和恒星风质量率的关键实验室。一个主要的挑战是推断观看倾向并提取有关碰撞风相互作用(CWI)区域的信息。高度电离风中电子散射的极化变异性提供了有关系统几何形状的重要诊断信息。我们首次结合了\ citet {brown_polarisation_1978}的众所周知的广义处理,以使二进制的二极化以及用半分析溶液进行几何和表面密度CWI冲击界面的二个极化,从而根据Canto等人进行了一些基于Canto等人的风度,包括我们的CANCATION CANCUNTION。我们的CANCOUSTINCES中的一些简化包括了一些临时,并在范围内进行了一些范围。强大的结论。一个是,当风几乎相等(例如,o \,+\,o二进制)时,极化会随着二元分离而相对温和的下降。另一个是,尽管汤姆森(Thomson)散射是灰色的不透明度,但连续极化可以在紫外线波长下显示色素效应,但在更长的波长下大部分是恒定的。最后,当一条风占主导地位时,例如在WR+OB二进制文件中,在OB分量更发光的波长下,极化将更大,并且通常在WR分量更发光的波长下较小。这种行为之所以出现,是因为从WR恒星的角度来看,球形的散射信封的失真是远离WR恒星的小扰动。相比之下,OB恒星的极化贡献由CWI冲击的几何形状主导。
Massive star binaries are critical laboratories for measuring masses and stellar wind mass-loss rates. A major challenge is inferring viewing inclination and extracting information about the colliding wind interaction (CWI) region. Polarimetric variability from electron scattering in the highly ionized winds provides important diagnostic information about system geometry. We combine for the first time the well-known generalized treatment of \citet{brown_polarisation_1978} for variable polarization from binaries with the semi-analytic solution for the geometry and surface density CWI shock interface between the winds based on Canto et al 1996. Our calculations include some simplifications in the form of inverse square-law wind densities and the assumption of axisymmetry, but in so doing arrive at several robust conclusions. One is that when the winds are nearly equal (e.g., O\,+\,O binaries), the polarization has a relatively mild decline with binary separation. Another is that despite Thomson scattering being a gray opacity, the continuum polarization can show chromatic effects at ultraviolet wavelengths but will be mostly constant at longer wavelengths. Finally, when one wind dominates the other, as for example in WR+OB binaries, the polarization is expected to be larger at wavelengths where the OB component is more luminous, and generally smaller at wavelengths where the WR component is more luminous. This behavior arises because from the perspective of the WR star, the distortion of the scattering envelope from spherical is a minor perturbation situated far from the WR star. By contrast, the polarization contribution from the OB star is dominated by the geometry of the CWI shock.