首页> 外文期刊>The Astrophysical journal >The Composition Gradient in M101 Revisited. II. Electron Temperatures and Implications for the Nebular Abundance Scale
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The Composition Gradient in M101 Revisited. II. Electron Temperatures and Implications for the Nebular Abundance Scale

机译:重访了M101中的成分渐变。二。电子温度及其对神经元丰度标度的意义

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We use high signal-to-noise ratio spectra of 20 H II regions in the giant spiral galaxy M101 to derive electron temperatures for the H II regions and robust metal abundances over radii R = 0.19-1.25R0 (6-41 kpc). We compare the consistency of electron temperatures measured from the [O III] λ4363, [N II] λ5755, [S III] λ6312, and [O II] λ7325 auroral lines. Temperatures from [O III], [S III], and [N II] are correlated with relative offsets that are consistent with expectations from nebular photoionization models. However, the temperatures derived from the [O II] λ7325 line show a large scatter and are nearly uncorrelated with temperatures derived from other ions. We tentatively attribute this result to observational and physical effects, which may introduce large random and systematic errors into abundances derived solely from [O II] temperatures. Our derived oxygen abundances are well fitted by an exponential distribution over six disk scale lengths, from approximately 1.3 (O/H)☉ in the center to 1/15 (O/H)☉ in the outermost region studied [for solar 12 + log(O/H) = 8.7]. We measure significant radial gradients in N/O and He/H abundance ratios, but relatively constant S/O and Ar/O. Our results are in approximate agreement with previously published abundances studies of M101 based on temperature measurements of a few H II regions. However, our abundances are systematically lower by 0.2-0.5 dex than those derived from the most widely used strong-line "empirical" abundance indicators, again consistent with previous studies based on smaller H II region samples. Independent measurements of the Galactic interstellar oxygen abundance from ultraviolet absorption lines are in good agreement with the Te-based nebular abundances. We suspect that most of the disagreement with the strong-line abundances arises from uncertainties in the nebular models that are used to calibrate the "empirical" scale, and that strong-line abundances derived for H II regions and emission-line galaxies are as much as a factor of 2 higher than the actual oxygen abundances. However, other explanations, such as the effects of temperature fluctuations on the auroral line based abundances, cannot be completely ruled out. These results point to the need for direct abundance determinations of a larger sample of extragalactic H II regions, especially for objects more metal-rich than solar.
机译:我们使用巨型旋涡星系M101中20个H II区的高信噪比光谱来得出H II区的电子温度和半径R = 0.19-1.25R0(6-41 kpc)时的稳健金属丰度。我们比较了从[O III]λ4363,[N II]λ5755,[S III]λ6312和[O II]λ7325极光线测得的电子温度的一致性。来自[O III],[S III]和[N II]的温度与相对偏移相关,该偏移与星云光电离模型的预期一致。但是,源自[O II]λ7325线的温度显示出较大的散射,并且几乎与源自其他离子的温度不相关。我们暂时将此结果归因于观测和物理效应,这可能会将大量随机和系统误差引入仅源自[O II]温度的丰度。我们得出的氧丰度很好地拟合了六个圆盘刻度长度上的指数分布,从中心的大约1.3(O / H)☉到研究的最外面区域的1/15(O / H)[[对于太阳12 + log (O / H)= 8.7]。我们在N / O和He / H丰度比中测量了显着的径向梯度,但是S / O和Ar / O相对恒定。我们的结果与之前发表的基于一些H II区温度测量的M101丰度研究相吻合。但是,与从最广泛使用的强线“经验”丰度指标得出的丰度相比,我们的丰度系统地降低了0.2-0.5 dex,这再次与先前基于较小的H II区域样本的研究一致。来自紫外线吸收谱线的银河星际氧丰度的独立测量与基于Te的星云状丰度非常吻合。我们怀疑,与强线丰度的大部分不同之处在于用于校准“经验”尺度的星云模型的不确定性,并且源自H II区和发射线星系的强线丰度与比实际氧气含量高2倍。但是,不能完全排除其他解释,例如温度波动对基于极光线的丰度的影响。这些结果表明需要直接测定较大的银河外H II区样品的丰度,特别是对于比太阳更富金属的物体。

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