论文标题
边缘星系中烹饪X结构的轨道成分
Orbital ingredients for cooking X-structures in edge-on galaxies
论文作者
论文摘要
X结构经常在托有所谓的B/PS(Boxy/Peanuts)凸起的星系中观察到,从边缘视图可见。它们是B/PS凸起的最著名的特征,出现在宿主星系的磁盘上突出的四个射线,可在B/PS凸起背景下区分。在某些作品中,它们的起源被认为与所谓的香蕉形轨道相连,并具有垂直共振2:1。这样的轨道中的一颗恒星在条形框架中每革命的垂直方向上执行两个振荡。最近的几项研究分析了在不同$ n $ body模型中产生的轨道集合的研究,这并不能证实X结构中谐振剂2:1轨道的主导地位。在我们的工作中,我们分析了两个$ n $ body型号,并显示了我们模型中的X结构是如何从中心逐渐组装的,从中心到外围,频率比小于2:1。此类轨道数量最多的是“ Farfalle”形(意大利面食)形式的形式,事实证明是非周期性的。我们得出的结论是,X结构仅是由其最高点的不同类型轨道的交叉或折叠引起的高密度区域的信封,并且没有与面内棒相似的“骨干”。比较了两个不同数值模型的轨道结构,我们表明,垂直振荡频率一定比率的一个或另一个轨道家族的主导地位与平面频率的一定比例取决于基础星系的参数,并最终决定了X结构的形态和X结构的形态和射线的开放角度。
X-structures are often observed in galaxies hosting the so-called B/PS (boxy/peanuts) bulges and are visible from the edge-on view. They are the most notable features of B/PS bulges and appear as four rays protruding from the disk of the host galaxy and distinguishable against the B/PS bulge background. In some works their origin is thought to be connected with the so-called banana-shaped orbits with a vertical resonance 2:1. A star in such an orbit performs two oscillations in the vertical direction per one revolution in the bar frame. Several recent studies that analyzed ensembles of orbits arising in different $N$-body models do not confirm the dominance of the resonant 2:1 orbits in X-structures. In our work we analyze two $N$-body models and show how the X-structure in our models is gradually assembled from the center to the periphery from orbits with less than 2:1 frequency ratio. The most number of such orbits is enclosed in a 'farfalle'-shape (Italian pasta) form and turns out to be non-periodic. We conclude that the X-structure is only the envelope of regions of high density caused by the crossing or folding of different types of orbits at their highest points, and does not have a "backbone" similar to that of the in-plane bar. Comparing the orbital structure of two different numerical models, we show that the dominance of one or another family of orbits with a certain ratio of the vertical oscillations frequency to the in-plane frequency depends on the parameters of the underlying galaxy and ultimately determines the morphology of the X-structure and the opening angle of its rays.