共查询到20条相似文献，搜索用时 62 毫秒
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星族合成方法及发射线星系核区中的恒星组分 总被引：1，自引：0，他引：1
论述星族合成方法对研究复合恒星体系的重要意义。综述了星族合成的三种基本方法，着重介绍了以星团光谱为样本的星族合成方法及其应用，最后，作为一个例子，我们利用ＣＳＰＳ方法给出发射线星系Ｍｒｋ４９９谱的合成结果。 相似文献
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非团环境中的大质量恒星以及大质量双星的起源是理解大质量恒星形成和演化的关键问题之一. 年轻大质量星团内的动力学交会过程是产生大质量逃逸星的重要途径之一. 选取了银河系内年轻大质量星团NGC 3603外围的两个碰撞星风系统候选体MTT68A和MTT71作为研究对象, 通过分析\emphChandra X射线观测以及\emphGaia第2批数据发布(DR2)中的天体测量结果, 研究它们作为相互作用的大质量双星系统的起源. X射线数据的分析表明, 它们的X射线能谱中存在Fe XXV发射线成分; 相较于普通O型星, 以双温等离子体模型拟合得到偏高的高温成分温度($\gtrsim$2.0keV), 并且X射线光度与热光度的比值也较高($\gtrsim10^{-5.8 相似文献
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动力学过程和恒星演化及二者的互相影响都会对球状星团的演化产生重要影响.由于金属丰度会影响恒星的演化轨迹,与之相伴随的恒星质量损失率的变化也会对球状星团的动力学过程造成影响.通过一系列N体模拟研究金属丰度对球状星团的质量损失率、半径等的影响,并分析其原因,同时研究了大质量恒星以及星团初始数密度分布的影响.模拟中采用的球状星团模型初始成员星数目N=50000,运行于类银河系的引力势中并考虑成员星的演化.结果显示,由于低金属丰度恒星拥有较快的演化时标,所以贫金属球状星团在早期会拥有较高的质量损失,但与此同时它们的核塌缩时间会比后者显著推迟,因此在核塌缩之后其质量损失会被富金属星团反超.另外由于大质量恒星演化导致的质量损失较大,所以大质量星的存在会使金属丰度更加显著地影响球状星团早期的扩张以及随后的核塌缩过程,同时星团的初始数密度分布也对该效应有着不可忽视的影响. 相似文献
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双星间的快速物质交换是一个非常复杂的过程,它涉及到双星演化的两个基本问题:物质交换的动力学不稳定性和公共包层的形成和演化.这两个问题是双星演化中最不清楚的两个基本问题.本论文通过建立相互作用双星之间的快速(绝热)物质损失模型,研究双星演化中物质交换的不稳定性判据和对公共包层的演化结局作出理论限制.利用恒星绝热物质损失模型得到的结果,还有很多潜在应用.比如,促进含双星的大样本恒星演化研究,改进演化星族合成方法等.恒星绝热物质损失模型的建立,基于主星在快速物质损失过程中,恒星内部的热量来不及交换, 相似文献
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利用星团谱样本的星族合成方法,分析了７个ＢＣＤＧ的光学谱,研究蓝致密矮星系（ＢＣＤＧ）内部的恒星形成历史、能源机制和尘埃分布情况．星族合成结果不仅能够解释ＢＣＤＧ的主要观测特征,解决ＢＣＤＧ研究中存在的一些问题,而且揭示了ＢＣＤＧ的一些未知的特性．谱合成结果表明：ＢＣＤＧ是年老的天体,其内部较早已经有恒星形成发生,恒星形成呈爆发式的,在ｔ＝５×１０７～１０９ｙｒ时的恒星形成率较高,最近（ｔ＝１０７ｙｒ）的恒星形成率开始下降;光谱分析显示大量大质量的年轻恒星提供了ＢＣＤＧ中心区的主要能源．利用扣除恒星吸收影响的发射线光谱,计算了发射线产生区的内红化值,发现它明显大于由连续谱计算得到的内红化值,这种差异的可能解释是ＢＣＤＧ内部尘埃对连续谱和发射线的产生区遮挡程度不同．最后,比较了ＢＣＧ和ＢＣＤＧ星族合成结果,提出了矮星系间一种可能的演化序列． 相似文献
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疏散星团是探究银河系结构与演化的良好示踪体,一直以来颇受关注.之前关于疏散星团的研究中,仅有一小部分疏散星团有金属丰度参数,而且,金属丰度的测量,是基于不同质量的观测数据,采用了不同的方法.收集了一个年龄大于2 Gyr的老年疏散星团样本,通过整理这些星团成员星的金属丰度数据,一方面,以星团NGC 2682为例,对比了不同光谱巡天项目给出的星团成员星金属丰度的系统差异;另一方面,计算了星团成员星金属丰度的平均值和中位值,作为该疏散星团的金属丰度推荐值.此外,还利用该样本探究了银盘径向金属丰度梯度随时间的演化,结果表明,早期银盘有着更加陡峭的径向金属丰度梯度,随着演化时间的增加,银盘径向金属丰度梯度逐渐趋于平缓,为银盘化学演化模型提供了更加严格的观测约束. 相似文献
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J.-M. Carquillat J.-L. Prieur 《Monthly notices of the Royal Astronomical Society》2007,380(3):1064-1078
Red clump giant (RCG) stars can be used as distance indicators to trace the mass distribution of the Galactic bar. We use RCG stars from 44 bulge fields from the OGLE-II microlensing collaboration data base to constrain analytic triaxial models for the Galactic bar. We find the bar major-axis is oriented at an angle of 24°–27° to the Sun–Galactic Centre line-of-sight. The ratio of semimajor and semiminor bar axis scalelengths in the Galactic plane x 0 , y 0 , and vertical bar scalelength z 0 , is x 0 : y 0 : z 0 = 10 : 3.5 : 2.6 , suggesting a slightly more prolate bar structure than the working model of Gerhard which gives the scalelength ratios as x 0 : y 0 : z 0 = 10 : 4 : 3 . 相似文献
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Amina Helmi 《Astronomy and Astrophysics Review》2008,15(3):145-188
Stellar halos may hold some of the best preserved fossils of the formation history of galaxies. They are a natural product
of the merging processes that probably take place during the assembly of a galaxy, and hence may well be the most ubiquitous
component of galaxies, independently of their Hubble type. This review focuses on our current understanding of the spatial
structure, the kinematics and chemistry of halo stars in the Milky Way. In recent years, we have experienced a change in paradigm
thanks to the discovery of large amounts of substructure, especially in the outer halo. I discuss the implications of the
currently available observational constraints and fold them into several possible formation scenarios. Unraveling the formation
of the Galactic halo will be possible in the near future through a combination of large wide field photometric and spectroscopic
surveys, and especially in the era of Gaia. 相似文献
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We study the gravitational lensing effects of spiral galaxies by taking a model of the Milky Way and computing its lensing properties. The model is composed of a spherical Hernquist bulge, a Miyamoto–Nagai disc and an isothermal halo. As a strong lens, a spiral galaxy like the Milky Way can give rise to four different imaging geometries. They are (i) three images on one side of the galaxy centre ('disc triplets'), (ii) three images with one close to the centre ('core triplets'), (iii) five images and (iv) seven images. Neglecting magnification bias, we show that the core triplets, disc triplets and fivefold imaging are roughly equally likely. Even though our models contain edge-on discs, their image multiplicities are not dominated by disc triplets. The halo is included for completeness, but it has a small effect on the caustic structure, the time delays and brightnesses of the images.
The Milky Way model has a maximum disc (i.e. the halo is not dynamically important in the inner parts). Strong lensing by nearly edge-on disc galaxies breaks the degeneracy between the relative contributions of the disc and halo to the overall rotation curve. If a spiral galaxy has a submaximum disc, then the astroid caustic shrinks dramatically in size, whilst the radial caustic shrinks more modestly. This causes changes in the relative likelihood of the image geometries, specifically (i) core triplets are now ∼9/2 times more likely than disc triplets, (ii) the cross-section for threefold imaging is reduced by a factor of ∼2/3, whilst (iii) the cross-section for fivefold imaging is reduced by ∼1/2. Although multiple imaging is less likely (the cross-sections are smaller), the average total magnification is greater. The time delays are smaller, as the total projected lensing mass is reduced. 相似文献
The Milky Way model has a maximum disc (i.e. the halo is not dynamically important in the inner parts). Strong lensing by nearly edge-on disc galaxies breaks the degeneracy between the relative contributions of the disc and halo to the overall rotation curve. If a spiral galaxy has a submaximum disc, then the astroid caustic shrinks dramatically in size, whilst the radial caustic shrinks more modestly. This causes changes in the relative likelihood of the image geometries, specifically (i) core triplets are now ∼9/2 times more likely than disc triplets, (ii) the cross-section for threefold imaging is reduced by a factor of ∼2/3, whilst (iii) the cross-section for fivefold imaging is reduced by ∼1/2. Although multiple imaging is less likely (the cross-sections are smaller), the average total magnification is greater. The time delays are smaller, as the total projected lensing mass is reduced. 相似文献