论文标题
恒星风弓休克星云的极化模拟。 ii。尘埃散射的情况
Polarization simulations of stellar wind bow shock nebulae. II. The case of dust scattering
论文作者
论文摘要
我们使用Monte Carlo辐射传递代码滑移研究了从弓形冲击量增强密度的弓形冲击区域中散射产生的极化。弓冲击是由快速移动恒星与星际介质的风的相互作用形成的结构。我们先前的研究集中于电子散射在这些结构中产生的极化。我们表明极化高度依赖于倾斜角,并且多个散射改变了极化的形状和程度。与电子散射相反,灰尘散射是波长依赖性的,这会改变极化行为。在这里,我们探索不同的灰尘粒径和组成,并为每种情况产生极化光谱分布。我们发现极化的SED行为取决于灰尘成分和晶粒尺寸。包括灰尘发射会导致在较高的光学深度下以对弓休克的方向敏感的方式变化。在各种场景和某些假设下,我们的模拟可以限制已解决和未解决的弓形冲击散射区域的光学深度和灰尘特性。光学深度上的构成可以为观察到的弓形电击提供局部ISM密度的估计。我们还研究了粉尘晶粒的影响,以填补恒星和弓形冲击之间的区域。我们看到,随着恒星和弓冲击之间的灰尘密度增加,所有光学深度机制都会抑制所得的极化。
We study the polarization produced by scattering from dust in a bow shock-shaped region of enhanced density surrounding a stellar source, using the Monte Carlo radiative transfer code SLIP. Bow shocks are structures formed by the interaction of the winds of fast-moving stars with the interstellar medium. Our previous study focused on the polarization produced in these structures by electron scattering; we showed that polarization is highly dependent on inclination angle and that multiple scattering changes the shape and degree of polarization. In contrast to electron scattering, dust scattering is wavelength-dependent, which changes the polarization behaviour. Here we explore different dust particle sizes and compositions and generate polarized spectral energy distributions for each case. We find that the polarization SED behaviour depends on the dust composition and grain size. Including dust emission leads to polarization changes with temperature at higher optical depth in ways that are sensitive to the orientation of the bow shock. In various scenarios and under certain assumptions, our simulations can constrain the optical depth and dust properties of resolved and unresolved bow shock-shaped scattering regions.Constraints on optical depth can provide estimates of local ISM density for observed bow shocks. We also study the impact of dust grains filling the region between the star and bow shock. We see that as the density of dust between the star and bow shock increases, the resulting polarization is suppressed for all the optical depth regimes.