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arXiv 1908.01487astro-ph.GA
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星际C $_2$和CN的$A$ --PDMATHAAB(0,0)带的首次探测

First detection of $A$--$X$ (0,0) bands of interstellar C$_2$ and CN

Satoshi Hamano, Hideyo Kawakita, Naoto Kobayashi, Keiichi Takenaka, Yuji Ikeda, Noriyuki Matsunaga, Sohei Kondo, Hiroaki Sameshima, Kei Fukue, Chikako Yasui, Mi… 展开作者

Satoshi Hamano, Hideyo Kawakita, Naoto Kobayashi, Keiichi Takenaka, Yuji Ikeda, Noriyuki Matsunaga, Sohei Kondo, Hiroaki Sameshima, Kei Fukue, Chikako Yasui, Misaki Mizumoto, Shogo Otsubo, Ayaka Watase, Tomohiro Yoshikawa, Hitomi Kobayashi

摘要:

我们报告了在星际介质中首次探测到C-$_2$-$A^1Π_u$- $X^1Σ_g^+$(0,0)和CN-$A^2Π_u$ - $X^2Σ^+$(0,0)吸收带。使用天鹅座OB 2 No. 1的近红外(0.91- 1.35 $μ$ m)高分辨率($R=20,000$和68,000)光谱进行检测,12是用安装在1.3米荒木望远镜上的WINERED摄谱仪收集的。同时检测到C $_2$和CN的$A$-$X$(1,0)带。这些近红外波段具有更大的振子强度,与光学中的C $_2$和CN的$A$-$X$(2,0)波段相比。在C $_2$(0,0)带的谱中,用$R=68,000$可以分辨视线中的三个速度分量,并且可以探测到高旋转能级($J''\sim20$)的谱线。通过分析C-$_2$的旋转分布,我们可以高精度地估计云的动力学温度和气体密度。此外,我们在星际介质中第一次勉强检测到$^{12}$ C $^{13}$ C的弱线。假设$^{12}$ C $_2$和$^{12}$ C $^{13}$ C的转动分布和相应跃迁的振子强度相同,则碳同位素比值估计为$^{12}\text{C}/^{13}\text{C}=50$ -100,这与本星际介质中的比值一致。我们还计算了C-$_2$(0,0)和(1,0)带的振子强度比。不幸的是,我们的结果不能区分理论和实验结果,因为不确定性。为了对振子强度比施加更强的约束,两个波段都需要高分辨率数据来分辨速度分量。

英文摘要:

We report the first detection of C$_2$ $A^1Π_u$--$X^1Σ_g^+$ (0,0) and CN $A^2Π_u$--$X^2Σ^+$ (0,0) absorption bands in the interstellar medium. The detection was made using the near-infrared (0.91--1.35 $μ$m) high-resolution ($R=20,000$ and 68,000) spectra of Cygnus OB2 No.\,12 collected with the WINERED spectrograph mounted on the 1.3 m Araki telescope. The $A$--$X$ (1,0) bands of C$_2$ and CN were detected simultaneously. These near-infrared bands have larger oscillator strengths, compared with the $A$--$X$ (2,0) bands of C$_2$ and CN in the optical. In the spectrum of the C$_2$ (0,0) band with $R=68,000$, three velocity components in the line of sight could be resolved and the lines were detected up to high rotational levels ($J''\sim20$). By analyzing the rotational distribution of C$_2$, we could estimate the kinetic temperature and gas density of the clouds with high accuracy. Furthermore, we marginally detected weak lines of $^{12}$C$^{13}$C for the first time in the interstellar medium. Assuming that the rotational distribution and the oscillator strengths of the relevant transitions of $^{12}$C$_2$ and $^{12}$C$^{13}$C are the same, the carbon isotope ratio was estimated to be $^{12}\text{C}/^{13}\text{C}=50$--100, which is consistent with the ratio in the local interstellar medium. We also calculated the oscillator strength ratio of the C$_2$ (0,0) and (1,0) bands from the observed band strengths. Unfortunately, our result could not discern theoretical and experimental results because of the uncertainties. High-resolution data to resolve the velocity components will be necessary for both bands in order to put stronger constraints on the oscillator strength ratios.

机构、总结、中文摘要均由AI分析而来,可能存在错误,请以论文正文为准。

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