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The possible hierarchical scales of observed clumps in high-redshift disc galaxies

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Behrendt,  M.
Optical and Interpretative Astronomy, MPI for Extraterrestrial Physics, Max Planck Society;

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Schartmann,  M.
Optical and Interpretative Astronomy, MPI for Extraterrestrial Physics, Max Planck Society;

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Burkert,  A.
Optical and Interpretative Astronomy, MPI for Extraterrestrial Physics, Max Planck Society;

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Citation

Behrendt, M., Schartmann, M., & Burkert, A. (2019). The possible hierarchical scales of observed clumps in high-redshift disc galaxies. Monthly Notices of the Royal Astronomical Society, 488(1), 306-323. doi:10.1093/mnras/stz1717.


Cite as: https://hdl.handle.net/21.11116/0000-0005-4028-6
Abstract
Giant clumps on ∼kpc scales and with masses of 108−109M are ubiquitous in observed high-redshift disc galaxies. Recent simulations and observations with high spatial resolution indicate the existence of substructure within these clumps. We perform high-resolution simulations of a massive galaxy to study the substructure formation within the framework of gravitational disc instability. We focus on an isolated and pure gas disc with an isothermal equation of state with T = 104 K that allows capturing the effects of self-gravity and hydrodynamics robustly. The main mass of the galaxy resides in rotationally supported clumps which grow by merging to a maximum clump mass of 108M with diameter ∼120 pc for the dense gas. They group to clump clusters (CCs) within relatively short times (⁠≪50Myr⁠), which are present over the whole simulation time. We identify several mass and size scales on which the clusters appear as single objects at the corresponding observational resolution between ∼108 and 109M⁠. Most of the clusters emerge as dense groups and for larger beams they are more likely to be open structures represented by a single object. In the high-resolution runs higher densities can be reached, and the initial structures can collapse further and fragment to many clumps smaller than the initial Toomre length. In our low-resolution runs, the clumps directly form on larger scales 0.3–1 kpc with 108−109M⁠. Here, the artificial pressure floor which is typically used to prevent spurious fragmentation strongly influences the initial formation of clumps and their properties at very low densities.