Y. P. 益鹏 Zou 邹, J. S. 江水 Zhang 张, C. Henkel, D. Romano, W. 玮 Liu 刘, Y. H. 映慧 Zheng 郑, Y. T. 耀庭 Yan 闫, J. L. 家梁 Chen 陈, Y. X. 友鑫 Wang 汪, J. Y. 洁瑜 Zhao 赵
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A correlation of the 18 O/ 17 O ratios with heliocentric distance is not found, indicating that beam dilution and linear beam sizes are not relevant. For the subsample of IRAM 30 m high-mass star-forming regions with accurate parallax distances, an unweighted fit gives 18 O/ 17 O = (0.12 ± 0.02) R GC + (2.38 ± 0.13) with a correlation coefficient of R = 0.67. While the slope is consistent with our J = 1–0 measurement, the ratios are systematically lower. This should be caused by larger optical depths of C 18 O 2–1 lines with respect to the corresponding 1–0 transitions, which is supported by RADEX calculations and the fact that C 18 O/C 17 O is positively correlated with 13 CO/C 18 O. When we consider that optical depth effects with C 18 O J = 2–1 typically reach an optical depth of ∼0.5, the corrected 18 O/ 17 O ratios from the J = 1–0 and J = 2–1 lines are consistent. 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引用次数: 0
摘要
为了研究高质量恒星与中质量恒星的相对喷射量,并追踪银河系的化学演化,我们利用IRAM 30 m和10 m亚毫米望远镜对421个分子云样本进行了银河系18 O/ 17 O比的系统研究,覆盖了星系中心距离范围为1-22 kpc。本文给出的结果是基于J = 2-1跃迁,包括364个源,显示c18o和c17o检测。先前建议的18 O/ 17 O梯度被确认。对于用这两种设备检测到的41个源,得到了很好的一致性。没有发现18 O/ 17 O比值与日心距离的相关性,表明光束稀释和线性光束尺寸无关。对于具有精确视差距离的IRAM 30 m高质量恒星形成区域的子样本,未加权拟合得到18 O/ 17 O =(0.12±0.02)R GC +(2.38±0.13),相关系数R = 0.67。虽然斜率与我们的J = 1-0测量结果一致,但比率系统性地降低了。这应该引起更大的光学深度C 18 O 2 - 1线对应的1 - 0转换,由RADEX支持计算17和18 O / C O与13 CO / C 18 O .呈正相关,当我们考虑到光学深度影响C 18 O J = 2:1通常达成光学深度0.5∼,纠正17 18 O / O比率从J = 1 - 0和J = 2行是一致的。MWG-12模型提供了一个很好的数值拟合数据,其中包括旋转恒星和新星。
A Systematic Observational Study on Galactic Interstellar Ratio 18O/17O. II. C18O and C17O J = 2–1 Data Analysis
Abstract To investigate the relative amount of ejecta from high-mass versus intermediate-mass stars and to trace the chemical evolution of the Galaxy, we have performed a systematic study of Galactic interstellar 18 O/ 17 O ratios toward a sample of 421 molecular clouds with IRAM 30 m and the 10 m Submillimeter Telescope, covering a galactocentric distance range of ∼1–22 kpc. The results presented in this paper are based on the J = 2–1 transition and encompass 364 sources showing both C 18 O and C 17 O detections. The previously suggested 18 O/ 17 O gradient is confirmed. For the 41 sources detected with both facilities, good agreement is obtained. A correlation of the 18 O/ 17 O ratios with heliocentric distance is not found, indicating that beam dilution and linear beam sizes are not relevant. For the subsample of IRAM 30 m high-mass star-forming regions with accurate parallax distances, an unweighted fit gives 18 O/ 17 O = (0.12 ± 0.02) R GC + (2.38 ± 0.13) with a correlation coefficient of R = 0.67. While the slope is consistent with our J = 1–0 measurement, the ratios are systematically lower. This should be caused by larger optical depths of C 18 O 2–1 lines with respect to the corresponding 1–0 transitions, which is supported by RADEX calculations and the fact that C 18 O/C 17 O is positively correlated with 13 CO/C 18 O. When we consider that optical depth effects with C 18 O J = 2–1 typically reach an optical depth of ∼0.5, the corrected 18 O/ 17 O ratios from the J = 1–0 and J = 2–1 lines are consistent. A good numerical fit to the data is provided by the MWG-12 model, which includes both rotating stars and novae.
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