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arXiv 1003.1407astro-ph.SRastro-ph.IM
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红超巨星的辐射流体动力学模拟:II。参宿四上对流的模拟匹配干涉观测

Radiative hydrodynamics simulations of red supergiant stars: II. simulations of convection on Betelgeuse match interferometric observations

A. Chiavassa, X. Haubois, J. S. Young, B. Plez, E. Josselin, G. Perrin, B. Freytag

摘要:

上下文红超巨星参宿四是一颗不规则变星。对流可能在理解这种变化方面发挥重要作用。干涉观测可以用复杂的恒星对流模拟来解释。目标。我们比较的可见度曲线和闭合相位从我们的三维模拟的RSG对流CO5BOLD的参宿四的各种干涉观测从光学H波段,以表征和测量对流模式在这颗星。方法.我们使用3D辐射流体动力学(RHD)模拟计算强度图在不同的过滤器,因此,我们推导出干涉观测使用后处理辐射转移代码OPTIM3D。合成的能见度曲线和关闭阶段进行了比较,观察。结果我们提供了一个强大的检测在光学和H波段上的参宿四表面上的颗粒图案的基础上观察到的可见性点和关闭阶段的优秀拟合。此外,我们确定,参宿四表面在H波段覆盖的小到中等规模(5 - 15质量)对流相关的表面结构和一个大的(30质量)对流细胞。在这个光谱区域,H2O分子是主要的吸收体,并对小结构和可见度曲线的第一个零点(即视恒星半径)的位置有贡献。

英文摘要:

Context. The red supergiant (RSG) Betelgeuse is an irregular variable star. Convection may play an important role in understanding this variability. Interferometric observations can be interpreted using sophisticated simulations of stellar convection. Aims. We compare the visibility curves and closure phases obtained from our 3D simulation of RSG convection with CO5BOLD to various interferometric observations of Betelgeuse from the optical to the H band in order to characterize and measure the convection pattern on this star. Methods. We use 3D radiative-hydrodynamics (RHD) simulation to compute intensity maps in different filters and we thus derive interferometric observables using the post-processing radiative transfer code OPTIM3D. The synthetic visibility curves and closure phases are compared to observations. Results. We provide a robust detection of the granulation pattern on the surface of Betelgeuse in the optical and in the H band based on excellent fits to the observed visibility points and closure phases. Moreover, we determine that the Betelgeuse surface in the H band is covered by small to medium scale (5-15 mas) convection-related surface structures and a large (30 mas) convective cell. In this spectral region, H2O molecules are the main absorbers and contribute to the small structures and to the position of the first null of the visibility curve (i.e. the apparent stellar radius).

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