论文标题
氦天体物理学的氦线发射
Helium line emissivities for nebular astrophysics
论文作者
论文摘要
我们介绍了几种碰撞辐射模型的结果,这些模型描述了由重组形成的中性氦气中的主要纤维发射性,用于电子温度和密度的网格,这是典型的H II区域和行星星云。例如,需要准确的发射率,例如测量星云中的氦气丰度,并因此是其原始值。我们将我们的结果与以前模型获得的结果进行了比较,发现显着差异,远高于目标准确性1%。我们详细讨论了我们选择的一组原子率以及与以前模型所采用的原子率的差异。主要区别在于对电子和质子碰撞率的处理,我们讨论哪些过渡对这些速率的选择最不敏感,因此最适合于高精度丰度确定。我们将比较重点放在外案B近似上,其中仅考虑了他和他的$^+$,但也呈现出完整模型的结果,包括裸露的核,光兴趣和光电偶以及黑体或黑体或观察到的光谱在Orion Nebula的情况下,以表明哪些频谱受到了亮度的影响。对于这些过渡,应进行准确的辐射转移计算。我们为$ n \ le 5 $内的所有过渡以及$ n \ le 5 $和$ n'\ le 25 $状态之间的所有过渡提供了发射表[cm $^{ - 3} $] = 10 $^{2(0.5)6} $范围,以及在这些范围内插入任何$ t _ {\ rm e}的fortran代码。
We present the results of several collisional-radiative models describing optically-thin emissivities of the main lines in neutral helium formed by recombination, for a grid of electron temperatures and densities, typical of H II regions and Planetary Nebulae. Accurate emissivities are required for example to measure the helium abundance in nebulae and as a consequence its primordial value. We compare our results with those obtained by previous models, finding significant differences, well above the target accuracy of one percent. We discuss in some detail our chosen set of atomic rates and the differences with those adopted by previous models. The main differences lie in the treatment of electron and proton collision rates and we discuss which transitions are least sensitive to the choice of these rates and therefore best suited to high precision abundance determinations. We have focused our comparisons on the case B approximation where only He and He$^+$ are considered, but also present results of full models including the bare nuclei, photo-excitation and photo-ionisation and either black-body or observed illuminating spectrum in the case of the Orion nebula, to indicate which spectral lines are affected by opacity. For those transitions, accurate radiative transfer calculations should be performed. We provide tables of emissivities for all transitions within $n \le 5$ and all those between the $n \le 5$ and $n' \le 25$ states, in the log $T_{\rm e}$ [K]=10$^{3.0(0.1)4.6}$ and log $N_{\rm e}$ [cm$^{-3}$]=10$^{2(0.5)6}$ ranges, and a FORTRAN code to interpolate to any $T_{\rm e}, N_{\rm e}$ within these ranges.