Molecular line emission in NGC 4945, imaged with ALMA

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[1] [1,2,Henkel, C.
[2] Mühle, S.
[3] 5,Bendo, G.
[4] 4,7,Józsa, G.I.G.
[5] 1,Gong, Y.
[6] Viti, S.
[7] Aalto, S.
[8] Combes, F.
[9] García-Burillo, S.
[10] Hunt, L.K.
[11] Mangum, J.
[12] 16,Martín, S.
[13] Muller, S.
[14] Ott, J.
[15] Van Der Werf, P.
[16] Malawi, A.A.
[17] Ismail, H.
[18] Alkhuja, E.
[19] Asiri, H.M.
[20] Aladro, R.
[21] 4,Alves, F.
[22] Ao, Y.
[23] Baan, W.A.
[24] Costagliola, F.
[25] Fuller, G.
[26] Greene, J.
[27] Impellizzeri, C.M.V.
[28] Kamali, F.
[29] 23,Klessen, R.S.
[30] Mauersberger, R.
[31] 1,3,Tang, X.D.
[32] Tristram, K.
[33] Wang, M.
[34] Zhang, J.S.
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| 1600年 / EDP Sciences卷 / 615期
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NGC 4945 is one of the nearest (D ≈ 3.8 Mpc; 100 ≈ 19 pc) starburst galaxies. To investigate the structure, dynamics, and composition of the dense nuclear gas of this galaxy, ALMA band 3 (λ ≈ 3−4 mm) observations were carried out with ≈200 resolution. Three HCN and two HC+ isotopologues, CS, C3H2, SiO, HCO, and CH3C2H were measured. Spectral line imaging demonstrates the presence of a rotating nuclear disk of projected size 1000 × 200 reaching out to a galactocentric radius of r ≈ 100 pc with position angle PA = 45◦ ± 2◦, inclination i = 75◦ ± 2◦ and an unresolved bright central core of size∼200. The continuum source, representing mostly free-free radiation from star forming regions, is more compact than the nuclear disk by a linear factor of two but shows the same position angle and is centered 000 . 39 ± 000 . 14 northeast of the nuclear accretion disk defined by H2O maser emission. Near the systemic velocity but outside the nuclear disk, both HCN J = 1 → 0 and CS J = 2 → 1 delineate molecular arms of length>∼1500 (>∼285 pc) on opposite sides of the dynamical center. These are connected by a (deprojected) ≈ 0.6 kpc sized molecular bridge, likely a dense gaseous bar seen almost ends-on, shifting gas from the front and back side into the nuclear disk. Modeling this nuclear disk located farther inside (r∼100 pc) with tilted rings provides a good fit by inferring a coplanar outflow reaching a characteristic deprojected velocity of ≈50 km s−1. All our molecular lines, with the notable exception of CH3C2H, show significant absorption near the systemic velocity (≈571 km s−1), within the range ≈500-660 km s−1. Apparently, only molecular transitions with low critical H2 density (ncrit∼ 104 cm−3) do not show absorption. The velocity field of the nuclear disk, derived from CH3C2H, provides evidence for rigid rotation in the inner few arcseconds and a dynamical mass of Mtot = (2.1 ± 0.2) × 108 M inside a galactocentric radius of 200 . 45 (≈45 pc), with a significantly flattened rotation curve farther out. Velocity integrated line intensity maps with most pronounced absorption show molecular peak positions up to ≈100 . 5 (≈30 pc) southwest of the continuum peak, presumably due to absorption, which appears to be most severe slightly northeast of the nuclear maser disk. A nitrogen isotope ratio of14N/15N ≈ 200-450 is estimated. This range of values is much higher then previously reported on a tentative basis. Therefore, because15N is less abundant than expected, the question for strong15N enrichment by massive star ejecta in starbursts still remains to be settled. © ESO 2018
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