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首页> 外文期刊>The Astrophysical journal >Polarimetric Variations of Binary Stars. II. Numerical Simulations for Circular and Eccentric Binaries in Mie Scattering Envelopes
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Polarimetric Variations of Binary Stars. II. Numerical Simulations for Circular and Eccentric Binaries in Mie Scattering Envelopes

机译:双星的极化变化。二。 Mie散射包络中的圆形和偏心二元数值模拟

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Following a previous paper on Thomson scattering, we present numerical simulations of the periodic polarimetric variations produced by a binary star placed at the center of an empty spherical cavity inside a circumbinary ellipsoidal and optically thin envelope made of dust grains. Mie single scattering (on spherical dust grains) is considered, along with pre- and postscattering extinction factors, which produce a time-varying optical depth and affect the morphology of the periodic variations. The orbits are circular or eccentric. The mass ratio (and luminosity ratio) is equal to 1.0. We are interested in the effects that various parameters (grain characteristics, geometry of the envelope, orbital eccentricity, etc.) will have on the average polarization, the amplitude of the polarimetric variations, and the morphology of the variability. We show that the absolute amplitudes of the variations are smaller for Mie scattering than for Thomson scattering, which makes harder the detection of polarimetric variations for binary stars surrounded by dust grains. The average polarization produced depends on the grains' composition and size and on the wavelength of observation. Among the four grain types that we have studied (astronomical silicates, graphite, amorphous carbon, and dirty ice), the highest polarizations are produced by grains with sizes in the range a ~ 0.1–0.2 μm (x = 2πa/λ ~ 1.0–2.0 for λ = 7000 ?). Composition and size also determine if the polarization will be positive or negative. In general, the variations are double periodic (seen twice per orbit). In some cases, because spherical dust grains have an asymmetric scattering function, the polarimetric curves produced show single-periodic variations (seen once per orbit) in addition to the double-periodic ones. A mixture of grains of different sizes does not affect those conclusions. Circumstellar disks produce polarimetric variations of greater amplitude (up to ~0.3% in our simulations) than circumbinary envelopes (usually 0.1%). Other geometries (circumbinary flared disks or prolate envelopes and noncoplanar envelopes) do not present particularly interesting polarimetric characteristics. Another goal of these simulations is to see if the 1978 BME (Brown, McLean, & Emslie) formalism, which uses a Fourier analysis of the polarimetric variations to find the orbital inclination for Thomson-scattering envelopes, can still be used for Mie scattering. We find that this is the case, if the amplitude of the variations is sufficient and the true inclination is itrue 45°. For eccentric orbits, the first-order coefficients of the Fourier fit, instead of second-order ones, can be used to find almost all inclinations.
机译:继上一篇有关Thomson散射的论文之后,我们介绍了由双星产生的周期极化变化的数值模拟,该双星位于由粉尘颗粒制成的外接椭圆形和光学薄壳内部的空球形腔的中心。考虑了米氏单次散射(在球形尘埃上),以及前和后散射消光因子,它们会产生随时间变化的光学深度并影响周期性变化的形态。轨道是圆形或偏心的。质量比(和光度比)等于1.0。我们对各种参数(晶粒特征,包络线的几何形状,轨道偏心率等)对平均极化,极化变化幅度和变异性形态的影响感兴趣。我们表明,对于Mie散射,变化的绝对幅度要小于Thomson散射,这使得检测被尘埃颗粒包围的双星的偏振变化更加困难。产生的平均极化取决于晶粒的组成和大小以及观察的波长。在我们研究的四种晶粒类型(天文硅酸盐,石墨,无定形碳和脏冰)中,最大的极化是由尺寸在a〜0.1–0.2μm(x =2πa/λ〜1.0–m)范围内的晶粒产生的。 λ= 7000时为2.0)。成分和大小也决定极化是正还是负。通常,变化是双周期的(每个轨道两次)。在某些情况下,由于球形尘埃颗粒具有不对称的散射功能,因此所产生的极化曲线除双周期的外,还显示出单周期的变化(每个轨道见过一次)。不同大小的谷物混合物不会影响这些结论。相比于包络线包络(通常为0.1%),星际圆盘产生的极化变化幅度更大(在我们的模拟中高达0.3%)。其他几何形状(周向张开的圆盘或扁形的包膜和非共面的包膜)没有特别有趣的极化特性。这些模拟的另一个目标是查看1978年的BME(布朗,麦克林和埃姆斯利)形式主义是否仍然可以用于米氏散射,该形式主义通过对偏振变化的傅立叶分析来找到汤姆森散射包络线的轨道倾角。我们发现,如果变化幅度足够大且真实倾斜度为真实45°,便是这种情况。对于偏心轨道,可以使用傅立叶拟合的一阶系数而不是二阶系数来查找几乎所有的倾角。

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