paper

Quenching timescales of galaxies in the EAGLE simulations

arXiv:1810.07335 · doi:10.1093/mnras/stz1410

Abstract

We use the \eagle\ simulations to study the connection between the quenching timescale, , and the physical mechanisms that transform star-forming galaxies into passive galaxies. By quantifying in two complementary ways - as the time over which (i) galaxies traverse the green valley on the colour-mass diagram, or (ii) leave the main sequence of star formation and subsequently arrive on the passive cloud in specific star formation rate (SSFR)-mass space - we find that the distribution of high-mass centrals, low-mass centrals and satellites are divergent. In the low stellar mass regime where , centrals exhibit systematically longer quenching timescales than satellites (~Gyr compared to ~Gyr). Satellites with low stellar mass relative to their halo mass cause this disparity, with ram pressure stripping quenching these galaxies rapidly. Low mass centrals are quenched as a result of stellar feedback, associated with long ~Gyr. At intermediate stellar masses where , are the longest for both centrals and satellites, particularly for galaxies with higher gas fractions. At , galaxy merger counts and black hole activity increase steeply for all galaxies. Quenching timescales for centrals and satellites decrease with stellar mass in this regime to ~Gyr. In anticipation of new intermediate redshift observational galaxy surveys, we analyse the passive and star-forming fractions of galaxies across redshift, and find that the peak at intermediate stellar masses is responsible for a peak (inflection point) in the fraction of green valley central (satellite) galaxies at .

Final version accepted to MNRAS. 18 pages, 16 figures