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arXiv 1301.5599astro-ph.CO
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巨大的HII区H 1013没有温度波动

No temperature fluctuations in the giant HII region H 1013

G. Stasinska, C. Morisset, S. Simon-Diaz, F. Bresolin, D. Schaerer, B. Brandl

摘要:

虽然在HII区域的碰撞激发线可以很容易地探测星系中星际介质的化学成分,但可能存在的重要温度波动对导出的丰度产生了一些疑问。为了给这个问题提供新的见解,我们对位于M101星系中的巨大HII区H 1013进行了详细的研究,该区域存在许多观测数据,并被认为存在t^2 = 0.03-0.06的温度波动。我们首先用斯皮策太空望远镜获得的中红外光谱补充了现有的光学观测数据集。结合光学数据,该光谱提供了关于这个巨大的HII区域的温度结构的前所未有的信息。基于经验温度诊断的初步分析表明,温度波动应该相当微弱。然后,我们使用基于光电离代码Cloudy的pyCloudy包进行了详细的建模。我们已经能够产生的光电离模型所观察到的血红蛋白表面亮度分布和电离恒星星族的已知属性比可以占大多数的线比在其不确定性的约束。由于观测的限制既强又多,这就反对H 1013存在显著的温度波动。我们最佳模型的氧丰度为12 + log O/H = 8.57,而Esteban等人(2009)和Bresolin(2007)分别主张的值为8.73和8.93,这是基于他们得出的显著温度波动。然而,我们的模型是不能够再现的氧复合线的强度。这不能归因于观测的不确定性,需要温度波动以外的解释。

英文摘要:

While collisionally excited lines in HII regions allow one to easily probe the chemical composition of the interstellar medium in galaxies, the possible presence of important temperature fluctuations casts some doubt on the derived abundances. To provide new insights into this question, we have carried out a detailed study of a giant HII region, H 1013, located in the galaxy M101, for which many observational data exist and which has been claimed to harbour temperature fluctuations at a level of t^2 = 0.03-0.06. We have first complemented the already available optical observational datasets with a mid-infrared spectrum obtained with the Spitzer Space Telescope. Combined with optical data, this spectrum provides unprecedented information on the temperature structure of this giant HII region. A preliminary analysis based on empirical temperature diagnostics suggests that temperature fluctuations should be quite weak. We have then performed a detailed modelling using the pyCloudy package based on the photoionization code Cloudy. We have been able to produce photoionization models constrained by the observed Hb surface brightness distribution and by the known properties of the ionizing stellar population than can account for most of the line ratios within their uncertainties. Since the observational constraints are both strong and numerous, this argues against the presence of significant temperature fluctuations in H 1013. The oxygen abundance of our best model is 12 + log O/H = 8.57, as opposed to the values of 8.73 and 8.93 advocated by Esteban et al. (2009) and Bresolin (2007), respectively, based on the significant temperature fluctuations they derived. However, our model is not able to reproduce the intensities of the oxygen recombination lines . This cannot be attributed to observational uncertainties and requires an explanation other than temperature fluctuations.

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