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首页> 外文期刊>The Astrophysical journal >A Tale of Two Stars: The Extreme O7 Iaf+ Supergiant AV 83 and the OC7.5 III((f)) star AV 69*
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A Tale of Two Stars: The Extreme O7 Iaf+ Supergiant AV 83 and the OC7.5 III((f)) star AV 69*

机译:两颗星的故事:Extreme O7 Iaf + Supergiant AV 83和OC7.5 III((f))星AV 69 *

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We present a detailed study of AV 83, an O7 Iaf+ supergiant, and AV 69 [OC7.5 III((f))] in the SMC. The stars have similar effective temperatures and luminosities but show very different wind signatures. For our study we have used the non-LTE line-blanketed atmosphere code developed by Hillier and Miller, which explicitly allows for line blanketing by C, N, O, S, Ar, Ne, Fe, and other elements. Our study finds that AV 83 has an effective temperature of approximately 33,000 K and log g ≈ 3.25. It has an extended photosphere as a result of a "low" effective surface gravity and a much denser wind than main-sequence O stars. We can match the spectrum only by using a slow velocity law with β ≈ 2, a value that is much larger than the values of around 1 predicted by standard radiation wind theory. Further, we show that the Hα emission profile in AV 83 is sensitive to the adopted surface gravity. To fit the spectrum of AV 83, we have considered conventional models in which the wind is smooth and alternate models in which the winds are highly clumped. Both types of winds yield a satisfactory fit to the majority of lines in the observed spectrum; however, strong UV photospheric lines and the P V resonance transitions favor a clumped wind. If clumping is important, it must begin at relatively low velocities (i.e., 30 km s-1, not 300 km s-1). In the smooth wind, the line force is too small to drive the wind. In the clumped wind, the line force is generally sufficient to drive the wind, although there are still some discrepancies around the sonic point. In AV 83, the N abundance is substantially enhanced relative to normal SMC abundances, while both C and O are SMC-like, consistent with the presence of internally processed CNO material at the stellar surface. The N III λ4640 multiplet, which is known to be produced by dielectronic recombination, is well reproduced by the models. These lines, and the adjacent C III λ4649 multiplet, show a significant sensitivity to surface gravity, as well as the usual sensitivity to abundance and effective temperature. Incoherent electron scattering, occurring within the photosphere, can explain the broad wings seen on these lines. We have modeled the Fe spectrum (Fe IV-Fe VI) in the UV in both AV 83 and AV 69. For stars with an effective temperature around 33,000 K, the Fe IV-to-Fe V line ratios form a useful effective temperature diagnostic and give results consistent with those found from optical and UV line diagnostics. The derived iron abundance, which is sensitive to the adopted microturbulent velocity, is 0.2-0.4 times the solar iron abundance in AV 83, while 0.2 solar gives a good fit for AV 69. The wind of AV 69 is substantially less dense than that of AV 83. Because of the lack of suitable diagnostics, it is impossible to constrain the mass-loss rate and velocity law independently. Its spectrum indicates that it has a similar effective temperature to AV 83 (Teff ≈ 34,000 K), a substantially higher gravity (log g = 3.5) than AV 83, and a CNO abundance pattern that has not been influenced by internal CNO processing. We show that the N/C abundance ratio is substantially below solar, in agreement with SMC nebular and stellar abundance studies. The differences between the spectra of AV 83 and AV 69, and between the derived masses and surface abundances, are striking. We have examined possible causes, and only one seems consistent with the observations and our current understanding of massive star evolution. AV 83 was most likely a fast rotator that experienced rotationally enhanced mass loss. The presence of enhanced N but almost normal C and O abundances is a direct indication of rotationally induced mixing. On the other hand, AV 69 is a slow rotator. As part of our analyses, we have systematically examined the influence of the H/He abundance ratio, the mass-loss rate, the velocity law, the Fe abundance, microturbulence, and clumping on the theoretical spectrum. We illustrate which lines provide usef
机译:我们目前对SMC中的AV 83,O7 Iaf +超巨蛋白和AV 69 [OC7.5 III((f))]进行了详细研究。这些恒星具有相似的有效温度和光度,但显示出非常不同的风特征。在我们的研究中,我们使用了Hillier和Miller开发的非LTE线路屏蔽气氛代码,该代码明确允许C,N,O,S,Ar,Ne,Fe和其他元素进行线路屏蔽。我们的研究发现,AV 83的有效温度约为33,000 K,log g≈3.25。由于“低”有效表面重力和比主序列O星密集得多的风,它具有更宽的光球范围。我们只能通过使用β≈2的慢速定律来匹配光谱,该值远大于标准辐射风理论预测的大约1的值。此外,我们显示AV 83中的Hα发射曲线对采用的表面重力敏感。为了适应AV 83的频谱,我们考虑了风平顺的常规模型和风高度成簇的替代模型。两种类型的风都可以很好地拟合观测到的谱线中的大多数谱线。但是,强紫外线光球线和P V共振跃迁有利于结团风。如果结块很重要,则必须从相对较低的速度开始(即30 km s-1,而不是300 km s-1)。在顺风中,线力过小而无法驱动风。在成团的风中,尽管声波点周围仍然存在一些差异,但线力通常足以驱动风。在AV 83中,相对于正常SMC丰度,N丰度大大提高了,而C和O都是SMC状的,这与恒星表面存在内部处理过的CNO材料一致。这些模型很好地再现了已知通过双电子复合产生的N IIIλ4640多重峰。这些线和相邻的C IIIλ4649多重峰显示出对表面重力的显着敏感性,以及对丰度和有效温度的通常敏感性。光球内部发生的非相干电子散射可以解释在这些线上看到的宽翅膀。我们对AV 83和AV 69的紫外线中的铁谱(Fe IV-Fe VI)进行了建模。对于有效温度约为33,000 K的恒星,Fe IV与Fe V的线比形成了有用的有效温度诊断并给出与光学和UV线诊断结果一致的结果。对采用的微湍流速度敏感的派生铁丰度是AV 83中太阳铁丰度的0.2-0.4倍,而0.2太阳光则非常适合AV69。AV69的风密度远小于AV 69的风密度。 AV 83.由于缺乏合适的诊断程序,因此不可能独立地限制质量损失率和速度定律。它的光谱表明它具有与AV 83相似的有效温度(Teff≈34,000 K),比AV 83具有更高的重力(log g = 3.5),并且不受内部CNO处理影响的CNO丰度模式。我们显示,N / C丰度比大大低于太阳能,这与SMC星状和恒星丰度研究一致。 AV 83和AV 69的光谱之间以及导出的质量和表面丰度之间的差异非常明显。我们已经检查了可能的原因,但只有一个似乎与观测结果和我们目前对大质量恒星演化的理解相符。 AV 83很可能是快速旋转的,其旋转损失增加。氮含量提高,但碳和氧含量几乎正常,这是旋转诱导混合的直接指示。另一方面,AV 69是慢速旋转器。作为分析的一部分,我们系统地研究了H / He丰度比,质量损失率,速度定律,Fe丰度,微湍流和结块对理论谱的影响。我们说明哪些行提供用

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