Molecular cloud photoevaporation and far-infrared line emission

被引:58
|
作者
Vallini, L. [1 ,2 ,3 ,4 ]
Ferrara, A. [5 ,6 ]
Pallottini, A. [5 ,7 ,8 ]
Gallerani, S. [5 ]
机构
[1] KTH Royal Inst Technol, NORDITA, Roslagstullsbacken 23, SE-10691 Stockholm, Sweden
[2] Stockholm Univ, Roslagstullsbacken 23, SE-10691 Stockholm, Sweden
[3] Dipartimento Fis & Astron, Viale Berti Pichat 6, I-40127 Bologna, Italy
[4] Osservatorio Astron Bologna, INAF, Via Ranzani 1, I-40127 Bologna, Italy
[5] Scuola Normale Super Pisa, Piazza Cavalieri 7, I-56126 Pisa, Italy
[6] Univ Tokyo, Todai Inst Adv Study, Kavli IPMU WPI, 5-1-5 Kashiwanoha, Kashiwa, Chiba 2778583, Japan
[7] Univ Cambridge, Kavli Inst Cosmol, Madingley Rd, Cambridge CB3 0HA, England
[8] Univ Cambridge, Cavendish Lab, 19 JJ Thomson Ave, Cambridge CB3 0HE, England
基金
美国国家科学基金会;
关键词
line: formation; ISM: clouds; galaxies: high-redshift; galaxies: ISM; infrared: ISM; HIGH-REDSHIFT GALAXIES; STAR-FORMATION RATE; PROBABILITY-DISTRIBUTION FUNCTIONS; TURBULENT MAGNETIZED CLOUDS; RAY DOMINATED REGIONS; PHOTODISSOCIATION REGIONS; FORMATION EFFICIENCY; INTERSTELLAR CLOUDS; ORION NEBULA; SUPERSONIC TURBULENCE;
D O I
10.1093/mnras/stx180
中图分类号
P1 [天文学];
学科分类号
0704 ;
摘要
With the aim of improving predictions on far-infrared (FIR) line emission from Giant Molecular Clouds (GMCs), we study the effects of photoevaporation (PE) produced by external farultraviolet (FUV) and ionizing (extreme-ultraviolet) radiation on GMC structure. We consider three different GMCs with mass in the range M-GMC = 10(3)-10(6)M(O). Our model includes (i) an observationally based inhomogeneous GMC density field, and (ii) its time evolution during the PE process. In the fiducial case (M-GMC approximate to 10(5)M(O)), the PE time (t(pe)) increases from 1 to 30 Myr for gasmetallicityZ = 0.05-1 Z(O)), respectively. Next, we compute the time-dependent luminosity of key FIR lines tracing the neutral and ionized gas layers of the GMCs, ([C II] at 158 mu m, [O III] at 88 mu m) as a function of G(0), and Z until complete PE at t(pe). We find that the specific [C II] luminosity is almost independent of the GMC model within the survival time of the cloud. Stronger FUV fluxes produce higher [C II] and [O III] luminosities, however, lasting for progressively shorter times. At Z = Z(O), the [CII] emission is maximized (LCII approximate to 10(4) L-O for the fiducial model) for t < 1Myr and logG(0) >= 3. Noticeably, and consistently with the recent detection by Inoue et al. of a galaxy at redshift z approximate to 7.2, for Z = 0.2Z(O), the [OIII] line might outshine [C II] emission by up to approximate to 1000 times. We conclude that the [OIII] line is a key diagnostic of low-metallicity interstellar medium, especially in galaxies with very young stellar populations.
引用
收藏
页码:1300 / 1312
页数:13
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