The most usual tracer of molecular gas is line emission from CO. However, the reliability of that tracer has long been questioned in environments different from the Milky Way. We study the relationship between H2 and CO abundances using a fully dynamical model of magnetized turbulence coupled to a chemical network simplified to follow only the dominant pathways for H2 and CO formation and destruction, and including photodissociation using a six-ray approximation. We find that the abundance of H2 is primarily determined by the amount of time available for its formation, which is proportional to the product of the density and the metallicity, but insensitive to photodissociation. Photodissociation only becomes important at extinctions under a few tenths of a visual magnitude, in agreement with both observational and prior theoretical work. On the other hand, CO forms quickly, within a dynamical time, but its abundance depends primarily on photodissociation, with only a weak secondary dependence on H2 abundance. As a result, there is a sharp cutoff in CO abundance at mean visual extinctions A_V < 3. At lower values of A_V we find that the ratio of H2 column density to CO emissivity X_CO is proportional to A_V^(-3.5). This explains the discrepancy observed in low metallicity systems between cloud masses derived from CO observations and other techniques such as infrared emission. Our work predicts that CO-bright clouds in low metallicity systems should be systematically larger or denser than Milky Way clouds, or both. Our results further explain the narrow range of observed molecular cloud column densities as a threshold effect, without requiring the assumption of virial equilibrium.
Anisotropy in the carbon monoxide (CO) line emission across the Milky Way's disk
Department of Astronomy, University of Massachusetts, Amherst(马萨诸塞大学阿默斯特分校天文学系);Laboratoire AIM, Paris-Saclay, CEA/IRFU/SAp - CNRS - Université Paris Diderot(巴黎-萨克雷天文信息实验室 (CEA/CNRS/巴黎第七大学));Universität Heidelberg, Zentrum für Astronomie, Institut für Theoretische Astrophysik(海德堡大学天体物理中心理论天体物理研究所);Universität Heidelberg, Interdiszipliäres Zentrum für Wissenschaftliches Rechnen(海德堡大学跨学科科学计算中心);Harvard-Smithsonian Center for Astrophysics(哈佛-史密森尼天体物理中心);Radcliffe Institute for Advanced Studies at Harvard University(哈佛大学拉德克利夫高等研究院);Dipartimento di Fisica, Università di Roma Tor Vergata(罗马托尔维加塔大学物理系);SUPA, School of Physics and Astronomy, University of St Andrews(圣安德鲁斯大学物理与天文学学院 (SUPA));École Polytechnique Fédérale de Lausanne, Observatoire de Sauverny(洛桑联邦理工学院索弗尼天文台)
Collisional excitation of far-infrared line emissions from warm interstellar carbon monoxide (CO)
受Herschel/PACS最近观测的启发,以及CO碰撞激发的新速率系数的可用性(Yang et al. 2010),使用数值和分析方法重新审视了温暖天体物理CO的激发。对于等温介质的情况,已经获得了气体温度(100至5000 K)和H2密度(1 E +3至1 E +9 cm-3)的宽范围的结果,并以旋转图的形式呈现,其中每个磁子状态的柱密度的对数log(N[J]/g[J])被绘制为每个状态的能量E[J]的函数。对于Herschel/PACS可达到的波长范围内的旋转跃迁,当n(H2)> 1 E +8 cm-3时,这样的图几乎是线性的。当log 10(n[H2])= 6.8至8时,它们表现出显著的负曲率,而当log 10(n[H2])< 4.8时,曲率在整个PACS可访问范围内一致为正。因此,观测一个正弯曲的CO转动图并不一定需要多个温度分量的存在。事实上,对于Herschel/PACS观察到的一些源,CO旋转图显示出适度的正曲率,可以用单个等温分量来解释。通常,所需的物理参数是1 E +4至1 E +5 cm-3范围内的H2密度和接近CO可以存活的最大温度T。其他来源展示更多的曲率旋转图比可以占一个单一的温度分量。对于气体温度呈幂律分布的介质,dN/dT与T的b次方成正比,H2密度为1 E +3 ~ 1 E +9 cm-3,幂律指数b在1 ~ 5范围内,这种介质可以解释CO旋转图,…
The ALMA carbon monoxide supernova (ACOS) survey II. Turbulent giant molecular clouds at the positions of core-collapse supernovae
Adam Mickiewicz University(亚当·密茨凯维奇大学);Instituto de Astrofísica de Canarias(加那利天体物理研究所);Universidad de La Laguna (ULL)(拉帕卢纳大学);Stockholm University(斯德哥尔摩大学);Foundation for Research and Technology-Hellas(希腊研究与技术基金会);National and Kapodistrian University of Athens(雅典国立卡波季斯特里安大学);University of Costa Rica(哥斯达黎加大学);Institute of Space Sciences (ICE, CSIC)(空间科学研究所);Institut d’Estudis Espacials de Catalunya (IEEC)(加泰罗尼亚空间研究学院);University of Copenhagen(哥本哈根大学)
The motivation to study experimentally CO ice under mimicked interstellar conditions is supported by the large CO gas abundances and ubiquitous presence of CO in icy grain mantles. Upon irradiation in its pure ice form, this highly stable species presents a limited ion and photon-induced chemistry, and an efficient non-thermal desorption. Using infrared spectroscopy, single laser interference, and quadrupole mass spectrometry during CO ice deposition, the CO ice density was estimated as a function of deposition temperature. Only minor variations in the density were found. The proposed methodol…
The inclusion of molecular physics is an important piece that tends to be missing from the puzzle when modeling the spectra of supernovae (SNe). Molecules have both a direct impact on the spectra, particularly in the infrared, and an indirect one as a result of their influence on certain physical conditions, such as temperature. In this paper, we aim to investigate molecular formation and non-local thermodynamic equilibrium (NLTE) cooling, with a particular focus on CO, the most commonly detected molecule in supernovae. We also aim to determine the dependency of supernova chemistry on physical…
Magnetic fields are expected to play an important role in accretion processes for circumstellar disks. Measuring the magnetic field morphology is difficult, especially since polarimetric (sub)millimeter continuum observations may not trace fields in most disks. The Goldreich-Kylafis (GK) effect suggests that line polarization is perpendicular or parallel to the magnetic field direction. We attempt to observe CO(2-1), $^{13}$CO(2-1), and C$^{18}$O(2-1) line polarization toward HD 142527 and IM Lup, which are large, bright protoplanetary disks. We use spatial averaging and spectral integration t…
We present near-infrared and optical observations of the Type Ic Supernova (SN) 2020oi in the galaxy M100 and the broad-lined Type Ic SN2020bvc in UGC 9379, using Gemini, LCO, SOAR, and other ground-based telescopes. The near-IR spectrum of SN2020oi at day 63 since the explosion shows strong CO emissions and a rising K-band continuum, which is the first unambiguous dust detection from a Type Ic SN. Non-LTE CO modeling shows that CO is still optically thick, and that the lower limit to the CO mass is 0.001 Msun. The dust temperature is 810 K, and the dust mass is ~10^(-5) Msun. We explore the p…
Discovery of a Perseus-like cloud in the early Universe: HI-to-H2 transition, carbon monoxide and small dust grains at zabs=2.53 towards the quasar J0000+0048