How is cold, star-forming gas in galaxies affected by magnetic fields?
Numerical simulations provide a unique opportunity to improve our understanding of the role of magnetic fields in the interstellar medium of galaxies and in star formation. However, many existing galaxy-scale numerical simulations impose a Kennicutt-Schmidt (KS) star formation law by construction. I...
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| Main Authors: | , , , , , , , , , , , |
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| Format: | Article (Journal) |
| Language: | English |
| Published: |
2025 December 02
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| In: |
Monthly notices of the Royal Astronomical Society
Year: 2026, Volume: 545, Issue: 3, Pages: 1-17 |
| ISSN: | 1365-2966 |
| DOI: | 10.1093/mnras/staf2132 |
| Online Access: | Verlag, kostenfrei, Volltext: https://doi.org/10.1093/mnras/staf2132 Verlag, kostenfrei, Volltext: https://academic.oup.com/mnras/article/545/3/staf2132/8362715?login=true 
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| Author Notes: | Kamran R.J. Bogue, Rowan J. Smith, Robin G. Treß, Mordecai-Mark Mac Low, David J. Whitworth, Ralf S. Klessen, Noé Brucy, Philipp Girichidis, Simon C.O. Glover, Junia Göller, Juan D. Soler, and Alessio Traficante |
| Summary: | Numerical simulations provide a unique opportunity to improve our understanding of the role of magnetic fields in the interstellar medium of galaxies and in star formation. However, many existing galaxy-scale numerical simulations impose a Kennicutt-Schmidt (KS) star formation law by construction. In this paper, we present two arepo simulations of an isolated star-forming galaxy with and without magnetic fields, using sink particles to model star formation without imposing a KS relation. We examine global differences between the models and investigate the impacts on star formation. We include a time-dependent, non-equilibrium chemical network coupled to a thermal evolution scheme and supernova feedback. Our magnetic field amplifies via dynamo action from a small initial seed field. We find a more compact magnetohydrodynamic (MHD) disc (radius $\sim$5.1 kpc, compared to $\sim$7.4 kpc), with a diffuse atomic envelope above and below the plane that is not seen in the hydrodynamic (HD) case. The HD disc displays a smoother, more even radial distribution of gas and star formation, and more bubbly substructure. Our MHD simulation has a higher proportion of dense, gravitationally unbound gas than the HD case, but a lower star formation rate, an average between 125 and 150 Myr of $\sim 4.8\, \mathrm{{\rm M}_{\odot }}$ yr$^{-1}$ compared to $\sim 8.4\, \mathrm{{\rm M}_{\odot }}$ yr$^{-1}$. We see a clear shift in the KS relation to higher gas surface densities in the MHD case, more consistent with observations. The additional magnetic support against gravitational collapse seems to raise the threshold gas surface density required for star formation. |
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| Item Description: | Gesehen am 01.04.2026 |
| Physical Description: | Online Resource |
| ISSN: | 1365-2966 |
| DOI: | 10.1093/mnras/staf2132 |