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arXiv 1105.0197astro-ph.SR
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球形恒星大气中的临边暗化

Limb darkening in spherical stellar atmospheres

Hilding R. Neilson, John B. Lester

摘要:

(略)背景。星缘暗化,I(μ = cosθ),是微透镜、食双星、行星凌日和干涉观测的重要限制,但通常被视为参数化曲线,例如线性加平方根定律。许多分析假设从模型恒星大气计算的边缘变暗系数。然而,以前的研究,使用来自平面平行模型的I(μ),已经发现对通量归一化曲线的拟合通过固定点,即恒星盘上的公共μ位置,对于Teff,log g和波长的所有值。目标。我们研究这个固定的μ点,以确定它是模型恒星大气的一个属性还是边缘变暗定律的一个属性。此外,我们使用这个临边暗化定律作为一种工具,以探测恒星大气的性质进行比较临边暗化的观测。方法.用平面平行和球对称Atlas模型(由三个基本参数L \star、M \star和R \star表征)计算的强度用于重新检查参数化曲线的固定μ点的存在。结果我们发现,我们的球形模型的强度没有一个固定的点,虽然曲线确实有一个最小的扩展在μ值类似的参数化曲线。我们还发现,参数化曲线有两个固定点,μ1和μ2,虽然μ2是如此接近的磁盘的边缘,它是错过了使用平面平行的大气。我们还发现,相对于平面平行模型,球对称模型似乎更好地与已发表的微透镜观测相一致。

英文摘要:

(Abridged) Context. Stellar limb darkening, I(μ = cosθ), is an important constraint for microlensing, eclipsing binary, planetary transit, and interferometric observations, but is generally treated as a parameterized curve, such as a linear-plus-square-root law. Many analyses assume limb-darkening coefficients computed from model stellar atmospheres. However, previous studies, using I(μ) from plane- parallel models, have found that fits to the flux-normalized curves pass through a fixed point, a common μ location on the stellar disk, for all values of T eff, log g and wavelength. Aims. We study this fixed μ-point to determine if it is a property of the model stellar atmospheres or a property of the limb-darkening laws. Furthermore, we use this limb-darkening law as a tool to probe properties of stellar atmospheres for comparison to limb- darkening observations. Methods. Intensities computed with plane-parallel and spherically-symmetric Atlas models (characterized by the three fundamental parameters L\star, M\star and R\star) are used to reexamine the existence of the fixed μ-point for the parametrized curves. Results. We find that the intensities from our spherical models do not have a fixed point, although the curves do have a minimum spread at a μ-value similar to the parametrized curves. We also find that the parametrized curves have two fixed points, μ1 and μ2, although μ2 is so close to the edge of the disk that it is missed using plane-parallel atmospheres. We also find that the spherically- symmetric models appear to agree better with published microlensing observations relative to plane-parallel models.

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