A study on the multicolour evolution of Red Sequence galaxy populations: insights from hydrodynamical simulations and semi-analytical models
A. D. Romeo (PMO Nanjing), Xi Kang (PMO Nanjing), E. Contini (PMO, Nanjing), J. Sommer-Larsen (NBI Copenhagen), R. Fassbender (INAF-OA Roma), N., R. Napolitano (INAF-OAC Napoli), V. Antonuccio-Delogu (INAF-OA Catania), I., Gavignaud (UNAB)

TL;DR
This study uses hydrodynamical simulations and semi-analytical models to analyze galaxy populations in clusters and groups from UV to NIR wavelengths, revealing how red/blue fractions and luminosity ratios evolve since redshift 2.
Contribution
It introduces a comprehensive comparison of galaxy population evolution using both simulations and models, highlighting the impact of selection criteria on observed properties.
Findings
The Butcher-Oemler effect is wavelength-dependent, with a steeper increase in blue fraction in optical colours.
Red Sequence luminosity fraction shows mild evolution when measured by stellar mass, aligning with high-redshift cluster observations.
Environmental differences affect galaxy properties, with groups and outskirts showing higher star-forming fractions at low redshift.
Abstract
By means of our own cosmological-hydrodynamical simulation and semi-analytical model we studied galaxy population properties in clusters and groups, spanning over 10 different bands from UV to NIR, and their evolution since redshift z=2. We compare our results in terms of galaxy red/blue fractions and luminous-to-faint ratio (LFR) on the Red Sequence (RS) with recent observational data reaching beyond z=1.5. Different selection criteria were tested in order to retrieve galaxies belonging to the RS: either by their quiescence degree measured from their specific SFR ("Dead Sequence"), or by their position in a colour-colour plane which is also a function of sSFR. In both cases, the colour cut and the limiting magnitude threshold were let evolving with redshift, in order to follow the natural shift of the characteristic luminosity in the LF. We find that the Butcher-Oemler effect is…
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