MeerKAT-16 H i observation of the dIrr galaxy WLM

Author:

Ianjamasimanana Roger12ORCID,Namumba Brenda1,Ramaila Athanaseus J T2,Saburova Anna S34ORCID,Józsa Gyula I G125,Myburgh Talon12,Thorat Kshitij6,Carignan Claude7,Maina Eric1,de Blok W J G879,Andati Lexy A L1,Hugo Benjamin V12,Kleiner Dane10ORCID,Kamphuis Peter11,Serra Paolo10,Smirnov Oleg M12,Maccagni Filippo M10,Makhathini Sphesihle1,Molnár Dániel Cs10ORCID,Perkins Simon2,Ramatsoku Mpati110,White Sarah V1ORCID

Affiliation:

1. Department of Physics and Electronics, Rhodes University, PO Box 94, Makhanda 6140, South Africa

2. South African Radio Astronomy Observatory, 2 Fir Street, Black River Park, Observatory, Cape Town 7925, South Africa

3. Sternberg Astronomical Institute, Moscow M.V. Lomonosov State University, Universitetskij pr., 13, Moscow 119234, Russia

4. Institute of Astronomy, Russian Academy of Sciences, Pyatnitskaya St, 48, Moscow 119017, Russia

5. Argelander-Institut für Astronomie, Auf dem Hügel 71, D-53121 Bonn, Germany

6. Department of Physics, University of Pretoria, Hatfield, Pretoria 0028, South Africa

7. Department of Astronomy, University of Cape Town, Private Bag X3, Rondebosch 7701, South Africa

8. Netherlands Institute for Radio Astronomy (ASTRON), Postbus 2, NL-7990 AA Dwingeloo, the Netherlands

9. Kapteyn Astronomical Institute, University of Groningen, Postbus 800, NL-9700 AV Groningen, the Netherlands

10. INAF-Osservatorio Astronomico di Cagliari, Via della Scienza 5, I-09047 Selargius (CA), Italy

11. Faculty of Physics and Astronomy, Astronomical Institute, Ruhr-Universität Bochum, D-44780 Bochum, Germany

Abstract

ABSTRACT We present observations and models of the kinematics and the distribution of the neutral hydrogen (H i) in the isolated dwarf irregular galaxy, Wolf-Lundmark-Melotte (WLM). We observed WLM with the Green Bank Telescope (GBT) and as part of the MeerKAT Early Science Programme, where 16 dishes were available. The H i disc of WLM extends out to a major axis diameter of 30 arcmin (8.5 kpc), and a minor axis diameter of 20 arcmin (5.6 kpc) as measured by the GBT. We use the MeerKAT data to model WLM using the tirific software suite, allowing us to fit different tilted-ring models and select the one that best matches the observation. Our final best-fitting model is a flat disc with a vertical thickness, a constant inclination and dispersion, and a radially varying surface brightness with harmonic distortions. To simulate bar-like motions, we include second-order harmonic distortions in velocity in the tangential and vertical directions. We present a model with only circular motions included and a model with non-circular motions. The latter describes the data better. Overall, the models reproduce the global distribution and the kinematics of the gas, except for some faint emission at the 2σ level. We model the mass distribution of WLM with pseudo-isothermal (ISO) and Navarro–Frenk–White (NFW) dark matter halo models. The NFW and the ISO models fit the derived rotation curves within the formal errors, but with the ISO model giving better reduced chi-square values. The mass distribution in WLM is dominated by dark matter at all radii.

Funder

H2020 European Research Council

Publisher

Oxford University Press (OUP)

Subject

Space and Planetary Science,Astronomy and Astrophysics

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1. What causes the formation of discs and end of bursty star formation?;Monthly Notices of the Royal Astronomical Society;2023-06-24

2. MIGHTEE-H i: possible interactions with the galaxy NGC 895;Monthly Notices of the Royal Astronomical Society;2023-03-23

3. Probing galaxy evolution through Hi 21-cm emission and absorption: current status and prospects with square kilometre array;Journal of Astrophysics and Astronomy;2022-12-19

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