旧恒星中的原子扩散和混合 - - VIII. 球状星团M4 (NGC 6121) 中的化学丰度变化
T Nordlander1,2,3, P Gruyters3,4, O Richard5
1Research School of Astronomy and Astrophysics, Australian National University, Canberra, ACT 2611, Australia.
概括
球状星团NGC 6121 (M4) 中恒星的化学丰度变化与包含原子扩散和额外混合的模型保持一致. 这些发现揭示了对古代恒星群体的恒星进化和核合成的见解.
科学领域:
- 天文学和天体物理学
- 恒星进化 恒星进化
- 银河系考古学 银河系考古学
背景情况:
- 在球状星团和开放星团内的恒星中观察到化学丰度的变化.
- 这些变化受到恒星金属性和进化阶段的影响.
- 原子扩散和额外的混合过程是恒星化学进化的关键因素.
研究的目的:
- 为了研究银河系球状星团NGC 6121 (M4) 中的化学丰度变化.
- 分析原子扩散和额外混合对恒星化学丰度的影响.
- 研究第二代恒星的组成及其污染源.
主要方法:
- 在NGC 6121中使用ESO VLT FLAMES高分辨率光谱仪对86颗恒星进行了详细的化学丰度分析.
- 从主顺序的转折点 (TOP) 到红色巨星分支 (RGB) 检查恒星.
- 将观察到的丰度变化与来自恒星结构和进化模型的预测进行比较.
主要成果:
- 确定了碳--氧 (C-N-O) 和-- (Mg-Al-Si) 的丰度反相关性.
- 确认了一个双模群体,丰度差异为1dex.
- 在TOP和RGB恒星之间观察到化学丰度的进化变化,与高效的额外混合相一致.
结论:
- 第二代恒星的化学组成表明,来自大质量恒星和非对称巨型分支恒星的污染.
- 观察到的丰度变化很弱,但当包括有效的额外混合时,与模型预测相匹配.
- 导出了2.63±0.10的初始丰度,略低于原始大爆炸核合成值.
相关概念视频
Behavior of Gas Molecules: Molecular Diffusion, Mean Free Path, and Effusion
29.0K
Although gaseous molecules travel at tremendous speeds (hundreds of meters per second), they collide with other gaseous molecules and travel in many different directions before reaching the desired target. At room temperature, a gaseous molecule will experience billions of collisions per second. The mean free path is the average distance a molecule travels between collisions. The mean free path increases with decreasing pressure; in general, the mean free path for a gaseous molecule will be...
29.0K
Maxwell-Boltzmann Distribution: Problem Solving
1.5K
Individual molecules in a gas move in random directions, but a gas containing numerous molecules has a predictable distribution of molecular speeds, which is known as the Maxwell-Boltzmann distribution, f(v).
This distribution function f(v) is defined by saying that the expected number N (v1,v2) of particles with speeds between v1 and v2 is given by
This distribution function f(v) is defined by saying that the expected number N (v1,v2) of particles with speeds between v1 and v2 is given by
1.5K
Molecular Orbital Theory II
19.2K
Molecular Orbital Energy Diagrams
19.2K
Atomic Nuclei: Nuclear Spin State Population Distribution
983
Near absolute zero temperatures, in the presence of a magnetic field, the majority of nuclei prefer the lower energy spin-up state to the higher energy spin-down state. As temperatures increase, the energy from thermal collisions distributes the spins more equally between the two states. The Boltzmann distribution equation gives the ratio of the number of spins predicted in the spin −½ (N−) and spin +½ (N+) states.
983
Diffusion on Chromatography Columns
554
In column chromatography, when an analyte is introduced as a narrow band at the top of the column, the solutes begin to separate and broaden, developing a Gaussian profile. This broadening occurs due to various factors, such as longitudinal diffusion.
Longitudinal diffusion occurs when the solute molecules in the mobile phase diffuse from the more concentrated center of the chromatographic band to the more dilute regions on either side, both towards and against the flow direction. This...
Longitudinal diffusion occurs when the solute molecules in the mobile phase diffuse from the more concentrated center of the chromatographic band to the more dilute regions on either side, both towards and against the flow direction. This...
554
Mass Spectrometry: Isotope Effect
2.1K
Most elements exist in nature as a mixture of isotopes. The isotopes differ in weight due to their respective number of neutrons. The molecular weight of a molecule is different depending on the specific isotope of its elements involved. As a result, the mass spectrum of the molecule exhibits peaks from the same fragment at multiple positions. The positions of these mass signals depend on the difference between the molecular mass. Furthermore, the intensity of these signals is dependent on the...
2.1K


