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arXiv 1902.03979astro-ph.GA
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星系共振环。在广阔的太阳邻域中运动的模拟

Galactic resonance rings. Modelling of motions in the wide solar neighborhood

Anna M. Melnik

摘要:

银河系的模型与分析费勒斯酒吧可以重现的剩余速度的OB协会在人马座,英仙座和本地系统的恒星气体复合体位于3千秒差距的太阳附近。考虑了密度分布为幂指数n=1和2的费勒斯椭球。局部系统中速度再现的成功是由于大的速度色散,其通过产生较小的系统运动来削弱共振效应。模型星系形成核,内和外共振环R1和R2。外环R2设法捕获比环R1多两倍的颗粒。棒的外Lindblad共振(OLR)位于太阳圆外0.4 kpc处,R_OLR= R_0 +0.4 kpc,对应于棒的角速度Ω_b=50 km s-1 kpc-1。太阳相对于棒的位置角theta_b,提供模型和观测速度之间的一致性是40-52度。不幸的是,考虑的模型不能再现船底座和天鹅座恒星气体复合体的剩余速度。比角动量L的重新分布在杆的Lindblad共振(ILR和OLR)附近发现:L的平均值在半径处增加(减小),比共振的半径小(大)一点,这与存在两种相互垂直的周期轨道有关。

英文摘要:

Models of the Galaxy with analytical Ferrers bars can reproduce the residual velocities of OB-associations in the Sagittarius, Perseus and Local System stellar-gas complexes located within 3 kpc solar neighborhood. Ferrers ellipsoids with density distribution defined by power indices n=1 and 2 are considered. The success in the reproduction of the velocity in the Local System is due to the large velocity dispersion which weakens the resonance effects by producing smaller systematic motions. Model galaxies form nuclear, inner and outer resonance rings R1 and R2. The outer rings R2 manage to catch twice more particles than the rings R1. The outer Lindblad resonance of the bar (OLR) is located 0.4 kpc beyond the solar circle, R_OLR=R0+0.4 kpc, corresponding to the bar angular velocity of Omega_b=50 km s-1 kpc-1. The solar position angle with respect to the bar, theta_b, providing the agreement between model and observed velocities is 40-52 degrees. Unfortunately, models considered cannot reproduce the residual velocities in the Carina and Cygnus stellar-gas complexes. The redistribution of the specific angular momentum, L, is found near the Lindblad resonances of the bar (ILR and OLR): the average value of L increases (decreases) at the radii a bit smaller (larger) than those of the resonances that can be connected with the existence of two types of periodic orbits elongated perpendicular to each other there.

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