Molecular gas kinematics within the central 250 pc of the Milky Way
Date Issued
2016
Author(s)
Henshaw, J. D.
•
Longmore, S. N.
•
Kruijssen, J. M. D.
•
Davies, B.
•
Bally, J.
•
Barnes, A.
•
Battersby, C.
•
Burton, M.
•
Cunningham, M. R.
•
Dale, J. E.
•
Ginsburg, A.
•
Immer, K.
•
Jones, P. A.
•
Kendrew, S.
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Mills, E. A. C.
•
•
Moore, T. J. T.
•
Ott, J.
•
Pillai, T.
•
Rathborne, J.
•
Schilke, P.
•
Schmiedeke, A.
•
•
Walker, D.
•
Walsh, A.
•
Zhang, Q.
Abstract
Using spectral line observations of HNCO, N2H+, and HNC, we investigate the kinematics of dense gas in the central ∼250 pc of the Galaxy. We present SCOUSE (Semi-automated multi-COmponent Universal Spectral-line fitting Engine), a line-fitting algorithm designed to analyse large volumes of spectral line data efficiently and systematically. Unlike techniques which do not account for complex line profiles, SCOUSE accurately describes the {l, b, vLSR} distribution of Central Molecular Zone (CMZ) gas, which is asymmetric about Sgr A* in both position and velocity. Velocity dispersions range from 2.6 km s-1 < σ < 53.1 km s-1. A median dispersion of 9.8 km s-1, translates to a Mach number, M_3D≥28. The gas is distributed throughout several `streams', with projected lengths ∼100-250 pc. We link the streams to individual clouds and sub-regions, including Sgr C, the 20 and 50 km s-1 clouds, the dust ridge, and Sgr B2. Shell-like emission features can be explained by the projection of independent molecular clouds in Sgr C and the newly identified conical profile of Sgr B2 in {l, b, vLSR} space. These features have previously invoked supernova-driven shells and cloud-cloud collisions as explanations. We instead caution against structure identification in velocity-integrated emission maps. Three geometries describing the 3D structure of the CMZ are investigated: (I) two spiral arms; (II) a closed elliptical orbit; (III) an open stream. While two spiral arms and an open stream qualitatively reproduce the gas distribution, the most recent parametrization of the closed elliptical orbit does not. Finally, we discuss how proper motion measurements of masers can distinguish between these geometries, and suggest that this effort should be focused on the 20 km s-1 and 50 km s-1 clouds and Sgr C.
Volume
457
Issue
3
Start page
2675
Issn Identifier
0035-8711
Ads BibCode
2016MNRAS.457.2675H
Rights
open.access
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