Humps on the Profiles of the Radial-Velocity Distribution and the Age of the Galactic Bar

IF 1.1 4区 物理与天体物理 Q3 ASTRONOMY & ASTROPHYSICS Astronomy Letters-A Journal of Astronomy and Space Astrophysics Pub Date : 2024-12-29 DOI:10.1134/S1063773724700385
A. M. Melnik, E. N. Podzolkova
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Abstract

We studied the model of the Galaxy with a bar which reproduces well the distributions of the observed radial, \(V_{R}\), and azimuthal, \(V_{T}\), velocities derived from the Gaia DR3 data along the Galactocentric distance \(R\). The model profiles of the distributions of the velocity \(V_{R}\) demonstrate a periodic increase and the formation of a hump (elevation) in the distance range of 6–7 kpc. The average amplitude and period of variations in the velocity \(V_{R}\) are \(A=1.76\pm 0.15\) km s\({}^{-1}\) and \(P=2.1\pm 0.1\) Gyr. We calculated angles \(\theta_{01}\), \(\theta_{02}\), and \(\theta_{03}\) which determine orientations of orbits relative to the major axis of the bar at the time intervals: 0–1, 1–2, and 2–3 Gyr from the start of simulation. Stars whose orbits change orientations as follows: \(0^{\circ}<\theta_{01}<45^{\circ}\), \(-45^{\circ}<\theta_{02}<0^{\circ}\), and \(0^{\circ}<\theta_{03}<45^{\circ}\), make a significant contribution to the hump formation. The fraction of orbits trapped into libration among orbits lying both inside and outside the outer Lindblad resonance (OLR) is 28\(\%\). The median period of oscillations of librating orbits is 2.0 Gyr. The median period \(P\) of long-term variations in the angular momentum and total energy of stars increases as the Jacobi energy approaches the values typical for the OLR but then sharply drops. The distribution of model stars over the period \(P\) has two maxima located at \(P=0.6\) and \(1.9\) Gyr. Stars with orbits lying both inside and outside the corotation radius (CR) concentrate to the first maximum. The distribution of stars whose orbits lie both inside and outside the OLR depends on their orientation: orbits elongated perpendicular to the bar concentrate to the first maximum but those stretched parallel to the bar concentrate to the second maximum. The fact that the observed profile of the \(V_{R}\)-velocity distribution derived from the Gaia DR3 data does not show a hump suggests that the age of the Galactic bar, counted from the moment of reaching its full power, must lie near one of two values: \(2.0\pm 0.3\) or \(4.0\pm 0.5\) Gyr.

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径向速度分布曲线上的驼峰和银条的年龄
我们研究了银河系的模型,该模型很好地再现了观测到的径向速度\(V_{R}\)和方位角速度\(V_{T}\)沿星系中心距离\(R\)的分布,这些分布来自盖亚DR3数据。速度分布的模型曲线\(V_{R}\)在6 ~ 7 kpc的距离范围内呈周期性增加,并形成驼峰(高程)。速度变化的平均振幅和周期\(V_{R}\)分别为\(A=1.76\pm 0.15\) km s \({}^{-1}\)和\(P=2.1\pm 0.1\) Gyr。我们计算了角度\(\theta_{01}\), \(\theta_{02}\)和\(\theta_{03}\),它们决定了轨道相对于杆的长轴的方向,时间间隔为:从模拟开始的0 - 1,1 - 2和2-3 Gyr。轨道改变方向的恒星如下:\(0^{\circ}<\theta_{01}<45^{\circ}\)、\(-45^{\circ}<\theta_{02}<0^{\circ}\)和\(0^{\circ}<\theta_{03}<45^{\circ}\),它们对驼峰的形成有重要贡献。在Lindblad外共振(OLR)内外的轨道中,被困在振动中的轨道的比例为28 \(\%\)。振动轨道的中位周期为2.0 Gyr。恒星角动量和总能量长期变化的中位周期\(P\)随着雅可比能量接近典型的OLR值而增加,但随后急剧下降。模型恒星在\(P\)期间的分布在\(P=0.6\)和\(1.9\) Gyr处有两个极大值。轨道在自转半径(CR)内外的恒星集中到第一个最大值。轨道同时位于OLR内外的恒星的分布取决于它们的方向:垂直于条形集中的轨道长到第一个最大值,而平行于条形集中的轨道长到第二个最大值。从盖亚DR3数据得出的观测到的\(V_{R}\) -速度分布的剖面并没有显示出一个驼峰,这一事实表明,从达到最大能量的那一刻开始计算的银条的年龄,一定位于两个值之一附近:\(2.0\pm 0.3\)或\(4.0\pm 0.5\) Gyr。
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来源期刊
CiteScore
1.70
自引率
22.20%
发文量
0
审稿时长
6-12 weeks
期刊介绍: Astronomy Letters is an international peer reviewed journal that publishes the results of original research on all aspects of modern astronomy and astrophysics including high energy astrophysics, cosmology, space astronomy, theoretical astrophysics, radio astronomy, extragalactic astronomy, stellar astronomy, and investigation of the Solar system.
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