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Planck early results. XIX. All-sky temperature and dust optical depth from Planck and IRAS. Constraints on the "dark gas" in our Galaxy

P.A.R. Ade N. Aghanim M. Arnaud M. Ashdown J. Aumont C. Baccigalupi A. Balbi A. J. Banday R. B. Barreiro J.G. Bartlett 1 E. Battaner K. Benabed A. Benoit 2 J. -P. Bernard M. Bersanelli R. Bhatia J. J. Bock A. Bonaldi J. R. Bond J. Borrill F. R. Bouchet F. Boulanger M. Bucher 3 C. Burigana P. Cabella J.-F. Cardoso 3 A. Catalano 3 L. Cayón A. Challinor A. Chamballu L. -Y Chiang C. Chiang P. R. Christensen D. L. Clements S. Colombi F. Couchot 4 A. Coulais B. P. Crill F. Cuttaia T. Dame L. Danese R. D. Davies R. J. Davis P. de Bernardis G. de Gasperis A. de Rosa G. de Zotti J. Delabrouille 5 J. -M. Delouis F. -X. Désert C. Dickinson K. Dobashi U. Doerl S. Donzelli O. Doré M. Douspis X. Dupac G. Efstathiou T. A. Enßlin H. K. Eriksen F. Finelli O. Forni P. Fosalba M. Frailis E. Franceschi Y. Fukui S. Galeotta K. Ganga 3 M. Giard G. Giardino Y. Giraud-Héraud 1 J. González-Nuevo K. M. Górski S. Gratton A. Gregorio I. A. Grenier A. Gruppuso F. K. Hansen D. Harrison G. Helou S. Henrot-Versillé 4 D. Herranz S.R. Hildebrandt 6 E. Hivon M. Hobson W. A. Holmes W. Hovest R. J. Hoyland K. M. Huffenberger A. H. Jaffe W. C. Jones M. Juvela A. Kawamura E. Keihänen R. Keskitalo T. S. Kisner R. Kneissl L. Knox H. Kurki-Suonio Guilaine Lagache J. -M. Lamarre A. Lasenby R. J. Laureijs C. R. Lawrence S. Leach R. Leonardi C. Leroy P. B. Lilje M. Linden-V\ornle M. López-Caniego P. M. Lubin J.F. Macías-Pérez 6 C. J. Mactavish B. Maffei D. Maino N. Mandolesi R. Mann M. Maris P. Martin E. Martínez-González S. Masi S. Matarrese F. Matthai P. Mazzotta P. Mcgehee P. R. Meinhold A. Melchiorri L. Mendes A. Mennella M. -A. Miville-Deschênes A. Moneti L. Montier G. Morgante D. Mortlock D. Munshi A. Murphy P. Naselsky P. Natoli C. B. Netterfield H. U. N\orgaard-Nielsen F. Noviello D. Novikov I. Novikov I. J. O'Dwyer T. Onishi S. Osborne F. Pajot R. Paladini D. Paradis F. Pasian G. Patanchon 3 O. Perdereau 4 L. Perotto 6 F. Perrotta F. Piacentini M. Piat 3 Stéphane Plaszczynski 4 E. Pointecouteau G. Polenta N. Ponthieu T. Poutanen G. Prézeau S. Prunet J. -L. Puget W. T. Reach M. Reinecke C. Renault 6 S. Ricciardi T. Riller I. Ristorcelli G. Rocha C. Rosset 3 M. Rowan-Robinson J. A. Rubiño-Martín B. Rusholme M. Sandri D. Santos 6 G. Savini D. Scott M. D. Seiffert P. Shellard G.F. Smoot 3 Jean-Luc Starck F. Stivoli V. Stolyarov Radek Stompor 5 R. Sudiwala J. -F. Sygnet J. A. Tauber L. Terenzi L. Toffolatti M. Tomasi J. -P. Torre M. Tristram 4 J. Tuovinen G. Umana L. Valenziano P. Vielva F. Villa N. Vittorio L. A. Wade B. D. Wandelt A. Wilkinson D. Yvon A. Zacchei A. Zonca
1 APC - Cosmologie
APC (UMR_7164) - AstroParticule et Cosmologie
2 HELFA - Hélium : du fondamental aux applications
NEEL - Institut Néel
3 APC (UMR_7164) - AstroParticule et Cosmologie
4 LAL - Laboratoire de l'Accélérateur Linéaire
5 APC-Gravitation - APC - Gravitation
APC (UMR_7164) - AstroParticule et Cosmologie, AEI - Max-Planck-Institut für Gravitationsphysik ( Albert-Einstein-Institut )
6 LPSC - Laboratoire de Physique Subatomique et de Cosmologie
Abstract : We construct an all-sky map of the apparent temperature and optical depth of thermal dust emission using the Planck-HFI and IRAS data. The optical depth maps are correlated to tracers of the atomic and molecular gas. The correlation is linear in the lowest column density regions at high galactic latitudes. At high NH, the correlation is consistent with that of the lowest NH. In the intermediate NH range, we observe departure from linearity, with the dust optical depth in excess to the correlation. We attribute this excess emission to thermal emission by dust associated with a Dark-Gas phase, undetected in the available HI and CO measurements. We show the 2D spatial distribution of the Dark-Gas in the solar neighborhood and show that it extends around known molecular regions traced by CO. The average dust emissivity in the HI phase in the solar neighborhood follows roughly a power law distribution with beta = 1.8 all the way down to 3 mm, although the SED flattens slightly in the millimetre. The threshold for the existence of the Dark-Gas is found at NH = (8.0\pm 0.58) 10^{20} Hcm-2. Assuming the same dust emissivity at high frequencies for the dust in the atomic and molecular phases leads to an average XCO = (2.54\pm0.13) 10^{20} H2cm-2/(K km s-1). The mass of Dark-Gas is found to be 28% of the atomic gas and 118% of the CO emitting gas in the solar neighborhood. A possible origin for the Dark-Gas is the existence of a dark molecular phase, where H2 survives photodissociation but CO does not. The observed transition for the onset of this phase in the solar neighborhood (AV = 0.4 mag) appears consistent with recent theoretical predictions. We also discuss the possibility that up to half of the Dark-Gas could be in atomic form, due to optical depth effects in the HI measurements.
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http://hal.in2p3.fr/in2p3-00644355
Contributor : Sabine Starita <>
Submitted on : Thursday, November 24, 2011 - 11:40:09 AM
Last modification on : Wednesday, January 6, 2021 - 9:14:04 AM

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OBSPM | CEA | UNIV-PARIS7 | IN2P3 | LAL | APC | CNRS | LPSC | NEEL | UGA | USPC | IRFU-APC | DSM-IRFU | CEA-DRF | UNIV-PARIS | GEPI | UP-SCIENCES | PSL

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P.A.R. Ade, N. Aghanim, M. Arnaud, M. Ashdown, J. Aumont, et al.. Planck early results. XIX. All-sky temperature and dust optical depth from Planck and IRAS. Constraints on the "dark gas" in our Galaxy. Astronomy and Astrophysics - A&A, EDP Sciences, 2011, 536, pp.A19. ⟨10.1051/0004-6361/201116479⟩. ⟨in2p3-00644355⟩

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