The tidal evolution of satellite galaxies in cosmological simulations: insights from colibre
Authors:
- Feihong HeFHFeihong He
- Jiaxin HanJHJiaxin Han
- Joop SchayeJSJoop Schaye
- Wenting WangWWWenting Wang
- Sylvia PloeckingerSPSylvia Ploeckinger
- Evgenii ChaikinECEvgenii Chaikin
- Robert J McGibbonRMRobert J McGibbon
- Filip HuškoFHFilip Huško
- Matthieu SchallerMSMatthieu Schaller
- Alejandro Benítez-LlambayABAlejandro Benítez-Llambay
- Alexander J RichingsARAlexander J Richings
Open Access
- 24 July 2026
- journal article
- Published by Oxford University Press (OUP) in Monthly Notices of the Royal Astronomical Society
- Vol. 551 (1)
Abstract
We investigate the co-evolution of the stellar and dark matter mass of satellite galaxies using the colibre cosmological hydrodynamical simulations with subhaloes resolved by the history-based hbt-herons subhalo finder. We identify a universal tidal track connecting stellar mass-loss to subhalo mass-loss characterized by two distinct phases, which can be well described by the two-parameter model. The initial phase consists primarily of dark matter stripping, whereas stellar stripping becomes significant only after the subhalo total bound mass fraction drops below a critical value ($\sim 0.057$). We find a bimodal mass-loss rate distribution of subhaloes. In satellites with modest mass-loss rates, the stellar mass is largely frozen. By contrast, the galaxy quickly becomes unresolved, along with the dark matter component for the extreme mass-loss population, naturally explaining the lack of ‘orphan’ galaxies in previous hydrodynamical simulations. Our model also predicts the formation condition for dark-matter-deficient galaxies (DMDGs), whose abundance peaks at $m_{*}\sim 10^{9.5}\, \rm {M}_{\odot }$. The abundance of DMDGs can be very sensitive to numerical effects, with colibre resolving a much larger DMDG population than previous hydrodynamical simulations. We also estimate the influence of artificial disruption on the satellite stellar mass function, which can amount to 20 (50) per cent at $m_* \sim 10^{9} (10^{8}) \, \rm M_\odot$, given a baryonic mass resolution of $\sim 10^{6}\, \rm {M}_{\odot }$.
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Funding Information
- National Natural Science Foundation of China (12595312)
- National Key Research and Development Program of China (2023YFA1607800)
- National Key Research and Development Program of China (2023YFA1607801)
- China Manned Space Program (CMS-CSST-2025-A04)
- Office of Science and Technology, Shanghai Municipal Government (24DX1400100)
- Office of Science and Technology, Shanghai Municipal Government (ZJ2023-ZD-001)
- Fundamental Research Funds for the Central Universities (KG202502)
- Netherlands Organization for Scientific Research
- Nederlandse Organisatie voor Wetenschappelijk Onderzoek (184.034.002)
- Austrian Science Fund
- Science and Technology Facilities Council (ST/X004651/1)
- Italian Ministry for Universities
- Fondo di Ateneo quota competitiva (2024-ATEQC-0050)
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