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在太阳附近有两个不同的晕群。III。来自恒星年龄和轨道参数的证据

Two distinct halo populations in the solar neighborhood. III. Evidence from stellar ages and orbital parameters

William J. Schuster, Edmundo Moreno, Poul E. Nissen, Barbara Pichardo

摘要:

在本系列的论文I和II中,在太阳附近发现了两种不同的恒星晕群。对67颗晕星和16颗厚盘星进行了精确的相对年龄和轨道参数的测定,这些恒星的金属丰度范围为-1.4 < [Fe/H] < -0.4,以更好地理解这两种晕族在银河系形成和演化中的背景。通过比较恒星在logT_{eff} -log(g)图中的位置和从Y ^2模型中插值到每颗恒星精确的[Fe/H]和[alpha/Fe]值的等时线,可以得到恒星的年龄。考虑并纠正了T_{eff}和log(g)中可能存在的系统误差。以论文I中的空间速度作为初始条件,利用一个详细的、观测约束的包括棒臂和旋臂的银河系模型进行了轨道积分。“高α”晕星的年龄比"低α“晕星大2-3 Gyr。轨道参数显示出“高α”和“低α”晕星之间的非常明显的差异。“低阿尔法"的r_{max}为30-40 kpc,z_{max}为大约。18千秒差距,而e_{max}的聚集值大于0.85,而“高α”的,r_{max}的约16千秒差距,z_{max}的6-8千秒差距,和e_{max}或多或少均匀分布在0.4-1.0。一个双原位加吸积形成的情况下,最好的解释这两个晕人口的存在和特点,但一个剩余的缺陷是,这个模型是不一致的r_{max}的获得原位“高α”组件;预测值太小。看来,Cen ω可能对“低α”成分的存在作出了重大贡献;最近的模型,包括动力摩擦和潮汐剥离,产生了与“低α”成分一样大的轨道参数。

英文摘要:

In Papers I and II of this series, the existence of two distinct halo populations of stars have been found in the solar neighborhood. Precise relative ages and orbital parameters are determined for 67 halo and 16 thick-disk stars having metallicities in the range -1.4 < [Fe/H] < -0.4 to better understand the context of the two halo populations in the formation and evolution of the Galaxy. Ages are derived by comparing the positions of stars in the logT_{eff}-log(g) diagram with isochrones from the Y^2 models interpolated to the exact [Fe/H] and [alpha/Fe] values of each star. Possible systematic errors in T_{eff} and log(g) are considered and corrected. With space velocities from Paper I as initial conditions, orbital integrations have been carried out using a detailed, observationally constrained Milky Way model including a bar and spiral arms. The `high-alpha' halo stars have ages 2-3 Gyr larger than the `low-alpha' ones. The orbital parameters show very distinct differences between the `high-alpha' and `low-alpha' halo stars. The `low-alpha' ones have r_{max}'s to 30-40 kpc, z_{max}'s to approx. 18 kpc, and e_{max}'s clumped at values greater than 0.85, while the `high-alpha' ones, r_{max}'s to about 16 kpc, z_{max}'s to 6-8 kpc, and e_{max} more or less uniformly distributed over 0.4-1.0. A dual in situ-plus-accretion formation scenario best explains the existence and characteristics of these two halo populations, but one remaining defect is that this model is not consistent regarding the r_{max}'s obtained for the in situ `high-alpha' component; the predicted values are too small. It appears that omega Cen may have contributed in a significant way to the existence of the `low-alpha' component; recent models, including dynamical friction and tidal stripping, have produced orbital parameters as great as those of the `low-alpha' component.

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