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NEBULAR AND AURORAL EMISSION LINES OF [Ar Ⅳ] IN THE OPTICAL SPECTRA OF PLANETARY NEBULAE

机译:行星状星云光学光谱中的[ArⅣ]的本构和自发发射线

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Recent R-matrix calculations of electron impact excitation rates in Ar Ⅳ are used to calculate the emission-line ratio: ratio diagrams (R_1; R_2), (R_1, R_3), and (R_1, R_4), where R_1=I(4711 A)/I(4740 A), R_2 = I(7238 A)/I(4711 + 4740 A), R_3 = 7(7263 A)/I(4711 + 4740 A), and R_4 = I(7171 A)/I(4711 + 4740 A), for a range of electron temperatures (T_e = 5000-20,000 K) and electron densities (N_e = 10-10~6 cm~(-3)) appropriate to gaseous nebulae. These diagrams should, in principle, allow the simultaneous determination of T_e and N_e from measurements of the [Ar Ⅳ] lines in a spectrum. Plasma parameters deduced for a sample of planetary nebulae from (R_1, R_3) and (R_1, R_4), using observational date obtained with the Hamilton echelle spectrograph on the 3 m Shane Telescope at the Lick Observatory, are found to show excellent internal consistency and to be in generally good agreement with the values of T_e and N_e estimated from other line ratios in the echelle spectra. These results provide observational support for the accuracy of the theoretical ratios and, hence, the atomic data adopted in their derivation. In addition, they imply that the 7171 A line is not as seriously affected by telluric absorption as previously thought. However, the observed values of R_2 are mostly larger than the theoretical high-temperature and density limit, which is due to blending of the Ar Ⅳ 7237.54 A line with the strong C Ⅱ transition at 7236 A
机译:最近使用ArⅣ中电子冲击激发率的R矩阵计算来计算发射线比率:比率图(R_1; R_2),(R_1,R_3)和(R_1,R_4),其中R_1 = I(4711) A)/ I(4740 A),R_2 = I(7238 A)/ I(4711 + 4740 A),R_3 = 7(7263 A)/ I(4711 + 4740 A)和R_4 = I(7171 A)/ I(4711 + 4740 A),适用于适合气态星云的电子温度范围(T_e = 5000-20,000 K)和电子密度(N_e = 10-10〜6 cm〜(-3))。这些图原则上应允许从光谱中[ArⅣ]线的测量中同时确定T_e和N_e。使用Lick天文台3 m Shane望远镜上的汉密尔顿埃切尔光谱仪获得的观测日期,从(R_1,R_3)和(R_1,R_4)的行星状星云样本推导出的血浆参数被发现具有出色的内部一致性,并且通常与从echelle光谱中其他线比率估计的T_e和N_e值非常吻合。这些结果为理论比率的准确性以及由此推导的原子数据的准确性提供了观察性支持。此外,它们暗示7171 A线不受碲吸收的严重影响。然而,R_2的观测值大多大于理论上的高温和高密度极限,这是由于将ArⅣ7237.54 A谱线与7236 A处的强CⅡ过渡相混合所致。

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