论文标题

保持凉爽:银河系磁盘中的许多轨道迁移,但很少供暖

Keeping it Cool: Much Orbit Migration, yet Little Heating, in the Galactic Disk

论文作者

Frankel, Neige, Sanders, Jason, Ting, Yuan-Sen, Rix, Hans-Walter

论文摘要

银河系磁盘中的恒星现在可以处于与出生半径相距较远的半径,原因有两个:它的轨道要么通过径向加热而变得偏心,这会增加其径向动作$ j_r $(“模糊”);或仅仅是其角动量$ l_z $已经改变,从而改变了指导半径(``搅动'')。我们知道,径向轨道迁移在半乳酸低$ $α$磁盘中很强,并着手通过设计和应用参数化模型的分布$ p(L_z,J_R,j_r,\ Mathrm [Fe/H])$来量化这两种效果的相对重要性。该模型描述了年龄$τ$和金属性[fe/h]的恒星的轨道演变,假定的coeval恒星最初是在(近)圆形轨道上出生的,并且在给定的出生角动量和年龄上具有独特的[Fe/H]。我们将该模型适合于脱红色团块恒星,这考虑了调查的复杂选择函数。最佳拟合模型意味着$ \ sqrt {\langleΔl_z\ rangle^2} \大约619 \,\ mathrm {kpc〜km/s〜}(τ/°\ mathrm {6〜gyr} 0.5} 0.5} $ radial and radial and s radial consem, Δj_r\ rangle^2} \大约63 \,\ mathrm {kpc〜km/s〜}(τ/\ mathrm {6〜gyr})^0.6} $ 8 kpc。这表明磁盘的世俗轨道演变主要由角动量扩散,而径向加热较低。

A star in the Milky Way's disk can now be at a Galactocentric radius quite distant from its birth radius for two reasons: either its orbit has become eccentric through radial heating, which increases its radial action $J_R$ (`blurring'); or merely its angular momentum $L_z$ has changed and thereby its guiding radius (`churning'). We know that radial orbit migration is strong in the Galactic low-$α$ disk and set out to quantify the relative importance of these two effects, by devising and applying a parameterized model for the distribution $p(L_z, J_R, τ, \mathrm[Fe/H])$ in the stellar disk. This model describes the orbit evolution for stars of age $τ$ and metallicity [Fe/H], presuming coeval stars were initially born on (near-)circular orbits, and with a unique [Fe/H] at a given birth angular momentum and age. We fit this model to APOGEE red clump stars, accounting for the complex selection function of the survey. The best fit model implies changes of angular momentum of $\sqrt{\langle ΔL_z \rangle^2} \approx 619\, \mathrm{kpc~km/s~}(τ/\mathrm{6~Gyr})^{0.5}$, and changes of radial action as $\sqrt{\langle ΔJ_R \rangle^2} \approx 63\, \mathrm{kpc~km/s~} (τ/\mathrm{6~Gyr})^{0.6}$ at 8 kpc. This suggests that the secular orbit evolution of the disk is dominated by diffusion in angular momentum, with radial heating being an order of magnitude lower.

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