# Murchison Widefield Array and XMM-Newton observations of the Galactic   supernova remnant G5.9+3.1

**Authors:** D. Oni\'c (1), M. D. Filipovi\'c (2), I. Boji\v{c}i\'c (2), N., Hurley-Walker (3), B. Arbutina (1), T. G. Pannuti (4), C. Maitra (5), D., Uro\v{s}evi\'c (1, 17), F. Haberl (5), N. Maxted (2, 6), G. F. Wong (2, and 6), G. Rowell (7), M. E. Bell (8), J. R. Callingham (9), K. S., Dwarakanath (10), B.-Q. For (11), P. J. Hancock (3), L. Hindson (12), M., Johnston-Hollitt (3), A. D. Kapi\'nska (11), E. Lenc (13), B. McKinley (14),, J. Morgan (3), A. R. Offringa (9), L. E. Porter (4), P. Procopio (15), L., Staveley-Smith (11), R. B. Wayth (3), C. Wu (11), Q. Zheng (16) ((1), Department of Astronomy, Faculty of Mathematics, University of Belgrade,, Studentski trg 16, 11000 Belgrade, Serbia, (2) Western Sydney University,, Locked Bag 1797, Penrith South DC, NSW, Australia, (3) International Centre, for Radio Astronomy Research, Curtin University, GPO Box U1987, Perth WA, 6845, Australia, (4) Space Science Center, Department of Earth, Space, Sciences, Morehead State University, 235 Martindale Drive, Morehead, KY, 40351, USA, (5) Max-Planck-Institut f\"ur extraterrestrische Physik,, Giessenbachstra{\ss}e, 85748 Garching, Germany, (6) School of Physics, The, University of New South Wales, Sydney 2052, Australia, (7) School of Physical, Sciences, The University of Adelaide, Adelaide 5005, Australia, (8), University of Technology Sydney, 15 Broadway, Ultimo, NSW 2007, Australia,, (9) Netherlands Institute for Radio Astronomy (ASTRON), PO Bus 2, 7990AA, Dwingeloo, The Netherlands, (10) Raman Research Institute, Bangalore 560080,, India, (11) International Centre for Radio Astronomy Research (ICRAR), M468,, University of Western Australia, Crawley, WA 6009, Australia, (12) Centre for, Astrophysics Research, School of Physics, Astronomy, Mathematics,, University of Hertfordshire, College Lane, Hatfield AL10 9AB, UK, (13) CSIRO, Astronomy, Space Science, Marsfield, NSW 1710, Australia, (14) Research, School of Astronomy, Astrophysics, Australian National University,, Canberra, ACT 2611, Australia, (15) School of Physics, The University of, Melbourne, Parkville, VIC 3010, Australia, (16) Shanghai Astronomical, Observatory, 80 Nandan Rd, Xuhui Qu, Shanghai Shi, China, 200000, (17) Isaac, Newton Institute of Chile, Yugoslavia Branch)

arXiv: 1904.06541 · 2019-05-22

## TL;DR

This study combines radio and X-ray observations to analyze the properties of the supernova remnant G5.9+3.1, revealing its spectral characteristics, morphology, and potential compact remnant, contributing new multi-wavelength data to its understanding.

## Contribution

First combined radio and X-ray analysis of G5.9+3.1, providing detailed spectral, morphological, and plasma properties of this poorly studied supernova remnant.

## Key findings

- Radio spectral index estimated at 0.42±0.03.
- First detection of X-ray emission from G5.9+3.1.
- Estimated swept-up mass of ~46 solar masses.

## Abstract

In this paper we discuss the radio continuum and X-ray properties of the so-far poorly studied Galactic supernova remnant (SNR) G5.9+3.1. We present the radio spectral energy distribution (SED) of the Galactic SNR G5.9+3.1 obtained with the Murchison Widefield Array (MWA). Combining these new observations with the surveys at other radio continuum frequencies, we discuss the integrated radio continuum spectrum of this particular remnant. We have also analyzed an archival XMM-Newton observation, which represents the first detection of X-ray emission from this remnant. The SNR SED is very well explained by a simple power-law relation. The synchrotron radio spectral index of G5.9+3.1, is estimated to be 0.42$\pm$0.03 and the integrated flux density at 1GHz to be around 2.7Jy. Furthermore, we propose that the identified point radio source, located centrally inside the SNR shell, is most probably a compact remnant of the supernova explosion. The shell-like X-ray morphology of G5.9+3.1 as revealed by XMM-Newton broadly matches the spatial distribution of the radio emission, where the radio-bright eastern and western rims are also readily detected in the X-ray while the radio-weak northern and southern rims are weak or absent in the X-ray. Extracted MOS1+MOS2+PN spectra from the whole SNR as well as the north, east, and west rims of the SNR are fit successfully with an optically thin thermal plasma model in collisional ionization equilibrium with a column density N_H~0.80x$10^{22}$ cm$^{-2}$ and fitted temperatures spanning the range kT~0.14-0.23keV for all of the regions. The derived electron number densities n_e for the whole SNR and the rims are also roughly comparable (ranging from ~$0.20f^{-1/2}$ cm$^{-3}$ to ~$0.40f^{-1/2}$ cm$^{-3}$, where f is the volume filling factor). We also estimate the swept-up mass of the X-ray emitting plasma associated with G5.9+3.1 to be ~$46f^{-1/2}M_{\odot}$.

## Full text

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## Figures

9 figures with captions in the complete paper: https://tomesphere.com/paper/1904.06541/full.md

## References

60 references — full list in the complete paper: https://tomesphere.com/paper/1904.06541/full.md

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Source: https://tomesphere.com/paper/1904.06541