The ALMA REBELS Survey: cosmic dust temperature evolution out to z ∼ 7

被引:89
|
作者
Sommovigo, L. [1 ]
Ferrara, A. [1 ]
Pallottini, A. [1 ]
Dayal, P. [2 ]
Bouwens, R. J. [3 ]
Smit, R. [4 ]
da Cunha, E. [5 ,6 ]
De Looze, I [7 ,8 ]
Bowler, R. A. A. [9 ]
Hodge, J. [3 ]
Inami, H. [10 ]
Oesch, P. [11 ,12 ]
Endsley, R. [13 ]
Gonzalez, V [14 ,15 ]
Schouws, S. [3 ]
Stark, D. [13 ]
Stefanon, M. [3 ]
Aravena, M. [16 ]
Graziani, L. [17 ,18 ]
Riechers, D. [19 ]
Schneider, R. [17 ,20 ]
van der Werf, P. [3 ]
Algera, H. [10 ]
Barrufet, L. [11 ]
Fudamoto, Y. [11 ,21 ,22 ]
Hygate, A. P. S. [3 ]
Labbe, I [23 ]
Li, Y. [24 ,25 ]
Nanayakkara, T. [23 ]
Topping, M. [13 ]
机构
[1] Scuola Normale Super Pisa, Piazza Cavalieri 7, I-56126 Pisa, Italy
[2] Univ Groningen, Kapteyn Astron Inst, NL-9700 AV Groningen, Netherlands
[3] Leiden Univ, Leiden Observ, NL-2300 RA Leiden, Netherlands
[4] Liverpool John Moores Univ, Astrophys Res Inst, 146 Brownlow Hill, Liverpool L3 5RF, Merseyside, England
[5] Univ Western Australia, Int Ctr Radio Astron Res, 35 Stirling Hwy, Crawley, WA 266009, Australia
[6] ARC Ctr Excellence All Sky Astrophys 3 Dimens AST, Stromlo, Australia
[7] Univ Ghent, Sterrenkundig Observatorium, Krijgslaan 281-S9, B-9000 Ghent, Belgium
[8] UCL, Dept Phys & Astron, Gower St, London WC1E 6BT, England
[9] Univ Oxford, Astrophys, Denys Wilkinson Bldg,Keble Rd, Oxford OX1 3RH, England
[10] Hiroshima Univ, Hiroshima Astrophys Sci Ctr, 1-3-1 Kagamiyama, Higashihiroshima, Hiroshima 7398526, Japan
[11] Univ Geneva, Observ Geneve, CH-1290 Versoix, Switzerland
[12] Univ Copenhagen, Cosm Dawn Ctr DAWN, Niels Bohr Inst, Jagtvej 128, DK-2200 Copenhagen N, Denmark
[13] Univ Arizona, Steward Observ, 933N Cherry Ave, Tucson, AZ 85721 USA
[14] Univ Chile, Dept Astron, Casilla 36-D, Santiago 7591245, Chile
[15] Ctr Astrofis & Tecnol Afines CATA, Camino Observatorio 1515, Santiago 7591245, Chile
[16] Univ Diego Portales, Nucleo Astron, Av Ejercito 441, Santiago, Chile
[17] Sapienza Univ Roma, Dipartimento Fis, Piazzale Aldo Moro 5, I-00185 Rome, Italy
[18] INAF Osservatorio Astrofis Arcetri, Largo E Femi 5, I-50125 Florence, Italy
[19] Univ Cologne, Phys Inst 1, Zulpicher Str 77, D-50937 Cologne, Germany
[20] INAF Osservatorio Astron Roma, Via Frascati 33, I-00078 Monte Porzio Catone, Italy
[21] Waseda Univ, Res Inst Sci & Engn, Shinjuku Ku, 3-4-1 Okubo, Tokyo 1698555, Japan
[22] Natl Astron Observ Japan, 2-21-1 Osawa, Mitaka, Tokyo, Japan
[23] Swinburne Univ Technol, Ctr Astrophys & Supercomp, POB 218, Hawthorn, Vic 3112, Australia
[24] Penn State Univ, Dept Astron & Astrophys, 525 Davey Lab, University Pk, PA 16802 USA
[25] Penn State Univ, Inst Gravitat & Cosmos, University Pk, PA 16802 USA
基金
澳大利亚研究理事会; 瑞士国家科学基金会;
关键词
methods: analytical; methods: data analysis; dust; extinction; galaxies: high-redshift; infrared: ISM; ULTRA-DEEP FIELD; STAR-FORMING GALAXIES; SPECTRAL ENERGY-DISTRIBUTIONS; HUBBLE-SPACE-TELESCOPE; C II EMISSION; 158; MU-M; MASS-METALLICITY RELATION; DARK-MATTER HALOES; GREATER-THAN; INTERSTELLAR-MEDIUM;
D O I
10.1093/mnras/stac302
中图分类号
P1 [天文学];
学科分类号
0704 ;
摘要
ALMA observations have revealed the presence of dust in the first generations of galaxies in the Universe. However, the dust temperature T-d remains mostly unconstrained due to the few available FIR continuum data at redshift z > 5. This introduces large uncertainties in several properties of high-z galaxies, namely their dust masses, infrared luminosities, and obscured fraction of star formation. Using a new method based on simultaneous [CII] 158-mu m line and underlying dust continuum measurements, we derive T-d in the continuum and [CII] detected z approximate to 7 galaxies in the ALMA Large Project REBELS sample. We find 39 < T-d < 58 K, and dust masses in the narrow range M-d = (0.9-3.6) x 10(7) M-circle dot. These results allow us to extend for the first time the reported T-d(z) relation into the Epoch of Reionization. We produce a new physical model that explains the increasing T-d(z) trend with the decrease of gas depletion time, t(d)(ep) = M-g/SFR, induced by the higher cosmological accretion rate at early times; this hypothesis yields T-d proportional to (1 + z)(0.4). The model also explains the observed T-d scatter at a fixed redshift. We find that dust is warmer in obscured sources, as a larger obscuration results in more efficient dust heating. For UV-transparent (obscured) galaxies, T-d only depends on the gas column density (metallicity), T-d proportional to N-H(1/6) (T-d proportional to Z(-1/6)). REBELS galaxies are on average relatively transparent, with effective gas column densities around N-H similar or equal to (0.03-1) x 10(21) cm(-2). We predict that other high-z galaxies (e.g. MACS0416-Y1, A2744-YD4), with estimated T-d >> 60 K, are significantly obscured, low-metallicity systems. In fact, T-d is higher in metal-poor systems due to their smaller dust content, which for fixed L-IR results in warmer temperatures.
引用
收藏
页码:3122 / 3135
页数:14
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