{"title":"The Metallicity–Electron Temperature Relationship in H ii Regions","authors":"D. Balser, T. Wenger","doi":"10.3847/1538-4357/ad2458","DOIUrl":null,"url":null,"abstract":"\n H ii region heavy-element abundances throughout the Galactic disk provide important constraints to theories of the formation and evolution of the Milky Way. In LTE, radio recombination line (RRL) emission and free–free continuum emission are accurate extinction-free tracers of the H ii region electron temperature. Since metals act as coolants in H ii regions via the emission of collisionally excited lines, the electron temperature is a proxy for metallicity. Shaver et al. found a linear relationship between metallicity and electron temperature with little scatter. Here we use CLOUDY H ii region simulations to (1) investigate the accuracy of using RRLs to measure the electron temperature and (2) explore the metallicity–electron temperature relationship. We model 135 H ii regions with different ionizing radiation fields, densities, and metallicities. We find that electron temperatures derived under the assumption of LTE are about 20% systematically higher owing to non-LTE effects, but overall LTE is a good assumption for centimeter-wavelength RRLs. Our CLOUDY simulations are consistent with the Shaver et al. metallicity–electron temperature relationship, but there is significant scatter since earlier spectral types or higher electron densities yield higher electron temperatures. Using RRLs to derive electron temperatures assuming LTE yields errors in the predicted metallicity as large as 10%. We derive correction factors for log(O/H) + 12 in each CLOUDY simulation. For lower metallicities the correction factor depends primarily on the spectral type of the ionizing star and ranges from 0.95 to 1.10, whereas for higher metallicities the correction factor depends on the density and is between 0.97 and 1.05.","PeriodicalId":504209,"journal":{"name":"The Astrophysical Journal","volume":"400 2","pages":""},"PeriodicalIF":0.0000,"publicationDate":"2024-01-31","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"The Astrophysical Journal","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.3847/1538-4357/ad2458","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 0
Abstract
H ii region heavy-element abundances throughout the Galactic disk provide important constraints to theories of the formation and evolution of the Milky Way. In LTE, radio recombination line (RRL) emission and free–free continuum emission are accurate extinction-free tracers of the H ii region electron temperature. Since metals act as coolants in H ii regions via the emission of collisionally excited lines, the electron temperature is a proxy for metallicity. Shaver et al. found a linear relationship between metallicity and electron temperature with little scatter. Here we use CLOUDY H ii region simulations to (1) investigate the accuracy of using RRLs to measure the electron temperature and (2) explore the metallicity–electron temperature relationship. We model 135 H ii regions with different ionizing radiation fields, densities, and metallicities. We find that electron temperatures derived under the assumption of LTE are about 20% systematically higher owing to non-LTE effects, but overall LTE is a good assumption for centimeter-wavelength RRLs. Our CLOUDY simulations are consistent with the Shaver et al. metallicity–electron temperature relationship, but there is significant scatter since earlier spectral types or higher electron densities yield higher electron temperatures. Using RRLs to derive electron temperatures assuming LTE yields errors in the predicted metallicity as large as 10%. We derive correction factors for log(O/H) + 12 in each CLOUDY simulation. For lower metallicities the correction factor depends primarily on the spectral type of the ionizing star and ranges from 0.95 to 1.10, whereas for higher metallicities the correction factor depends on the density and is between 0.97 and 1.05.
整个银河系盘的 H ii 区域重元素丰度为银河系的形成和演化理论提供了重要的约束条件。在 LTE 中,射电重组线(RRL)发射和自由连续面发射是 H ii 区域电子温度的精确无消光追踪器。由于金属通过碰撞激发线的发射在 H ii 区域充当冷却剂,因此电子温度可以代表金属度。Shaver 等人发现金属性与电子温度之间呈线性关系,且散射很小。在这里,我们利用 CLOUDY H ii 区域模拟来:(1)研究使用 RRL 测量电子温度的准确性;(2)探索金属性与电子温度之间的关系。我们模拟了 135 个具有不同电离辐射场、密度和金属性的 H ii 区域。我们发现,由于非 LTE 效应,在 LTE 假设下得出的电子温度系统性地高了约 20%,但总体而言,LTE 对于厘米波长的 RRL 是一个很好的假设。我们的 CLOUDY 模拟与 Shaver 等人的金属性-电子温度关系一致,但由于较早的光谱类型或较高的电子密度会产生较高的电子温度,因此存在明显的差异。使用RRL来推导假定LTE的电子温度,会产生高达10%的金属性预测误差。我们在每一次CLOUDY模拟中都得出了log(O/H) + 12的修正系数。对于较低的金属性,校正因子主要取决于电离星的光谱类型,范围在 0.95 到 1.10 之间;而对于较高的金属性,校正因子则取决于密度,范围在 0.97 到 1.05 之间。