The role of thermal and non-thermal processes in the ISM of the Magellanic Clouds

Author:

Hassani H12ORCID,Tabatabaei F2,Hughes A34ORCID,Chastenet J56,McLeod A F78ORCID,Schinnerer E9,Nasiri S1

Affiliation:

1. Shahid Beheshti University, Faculty of Physics, Department of Astronomy and Astrophysics, 19839 Tehran, Iran

2. School of Astronomy, Institute for Research in Fundamental Sciences (IPM), PO Box 19395-5531, Tehran, Iran

3. CNRS, IRAP, 9 Av. du Colonel Roche, BP 44346, F-31028 Toulouse cedex 4, France

4. Université de Toulouse, UPS-OMP, IRAP, F-31028 Toulouse cedex 4, France

5. Center for Astrophysics and Space Sciences, Department of Physics, University of California, San Diego, 9500 Gilman Drive, La Jolla, CA 92093, USA

6. Sterrenkundig Observatorium, Ghent University, Kri-jgslaan 281-S9, B-9000 Gent, Belgium

7. Department of Astronomy, University of California Berkeley, Berkeley, CA 94720, USA

8. Centre for Extragalactic Astronomy, Department of Physics, Durham University, South Road, Durham DH1 3LE, UK

9. Max-Planck-Institut für Astronomie, Königstuhl 17, D-69117 Heidelberg, Germany

Abstract

ABSTRACT Radio continuum emission is a dust-unbiased tracer of both thermal and non-thermal processes in the interstellar medium. We present new maps of the free–free and synchrotron emission in the Magellanic Clouds (MCs) at 0.166, 1.4, and 4.8 GHz with no prior assumption about the radio non-thermal spectrum. The maps were constructed using a de-reddened H α map as a template for the thermal radio emission, which we subtract from maps of the total radio continuum emission. To de-redden the H α emission, it is important to know the fraction of dust surface density that attenuates the H α emission along the line of sight, fd. This fraction is obtained by comparing the dust opacity obtained through the infrared emission spectrum and the Balmer decrement method. In star-forming regions, the median fd is about 0.1, which is lower than that in diffuse regions by a factor of three. We obtain a global thermal radio fraction, fth, of 30 per cent (35 per cent) in the LMC (SMC) at 1.4 GHz. Furthermore, we present maps of the equipartition magnetic field strength with average values of $\simeq \, 10.1\, \mu$G in the LMC and $\simeq \, 5.5\, \mu$G in the SMC. The magnetic field is proportional to the star-formation rate to the power of 0.24 and 0.20 for the LMC and SMC, respectively. This study shows that non-thermal processes control the interstellar medium in the MCs.

Funder

Institute for Research in Fundamental Sciences

Publisher

Oxford University Press (OUP)

Subject

Space and Planetary Science,Astronomy and Astrophysics

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