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Galactic mass and anisotropy profile with halo K-giant and blue horizontal branch stars from LAMOST/SDSS and Gaia

机译:哈洛k-giant和Lamost / SDSS和Gaia的蓝色水平分支星座的银河系和各向异性曲线

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A major uncertainty in the determination of the mass profile of the Milky Way using stellar kinematics in the halo is the poorly determined anisotropy parameter, β = 1 - (σ~2_θ + σ~2_Φ)/(2σ~2_r), where σ_r is the Galactocentric radial velocity dispersion, and σ_θ and σ_Φ are the tangential components of the velocity dispersion. We have used a sample of over 24,000 Galactic halo K giant and blue horizontal branch stars from the LAMOST stellar spectroscopic survey and SDSS/SEGUE, combined with proper motions from Gaia Data Release 2, to measure β(r_(gc)) over a wide range of Galactocentric distances r_(gc) from 5 to 80 kpc. Kinematic substructures have been carefully removed to reveal the underlying diffuse stellar halo prior to measuring β. We find that orbits are generally radial (β > 0) and β is constant out to distances of about 40 kpc, with a dependence on metallicity of the stars, such that β declines with lower metallicity. Similar behavior is seen in both the K giant and BHB samples.
机译:在晕圈中使用恒星运动学测定银河系的质量剖面的主要不确定性是确定的各向异性参数差,β= 1 - (Σ〜2_θ+σ〜2_φ)/(2σ〜2_R),其中σ_r是半乳腺辐射速度分散和σ_θ和σ_φ是速度分散的切向分量。我们使用了来自Lamost Stellar Spectroscopic测量和SDSS / Segue的24,000多个半乳清光环巨型和蓝色水平分支星的样本,与Gaia数据发布2的适当动作结合在一起,测量β(r_(gc))半球形距离范围距离(GC)为5至80 KPC。在测量β之前,已经小心地去除了运动副结构以显示下面的弥漫性恒星晕。我们发现轨道通常是径向(β> 0),β是恒定的约40kpc的距离,差异恒定的金属性,使得β随着较低金属性下降。在K巨头和BHB样品中看到类似的行为。

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