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  • NAM2021
    • Contacts
  • Science
    • Science Programme
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    • Special Lunches/Discussion Sessions
    • Poster Session
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  • Social
    • Presidential Address
    • Herschel Concert
    • RAS Awards Ceremony
    • Virtual Stonehenge Tour
  • Media
  • Public Engagement
    • Public engagement opportunities
    • Public talk
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Wednesday

Schedule

id
date time
AM
09:42
Abstract
The low-mass end turnover -- New measurements of the low-mass z~6-7 galaxy stellar mass function
Wednesday

Abstract details

id
The low-mass end turnover -- New measurements of the low-mass z~6-7 galaxy stellar mass function
Date Submitted
2021-04-28 00:00:00
Lukas
Furtak
Institut d'Astrophysique de Paris (IAP)
Cosmic Star Formation – theory and observations, from the first galaxies to the Milky Way
Contributed
L. Furtak (IAP), H. Atek (IAP), M. D. Lehnert (IAP)
Early star-forming galaxies at redshifts z>6 in the epoch of cosmic reionization are at the frontier of observability with the current instrumentation and represent the progenitors of present-day galaxies. The galaxy stellar mass function (GSMF) at z~6-9 is therefore a robust and crucial tool to study the build-up of stellar mass in the Universe and provides the tightest constraints on cosmological simulations. The observation of a decline in galaxy number density towards very low masses, i.e. a turnover at the very low-mass end of the GSMF, is of particular interest to constrain the evolution of the underlying dark matter halos in numerical simulations: The drop in number density of galaxies at high-redshifts provides strong constraints on the characteristic halo mass scale at which stellar feedback (supernovae and winds from massive stars) can suppress star formation.
I will present our recent work on the low-mass end of the GSMF at z=6-7 and the tentative detection of a downward turnover on the low-mass end using the gravitational magnification of the Hubble Frontier Fields clusters. I will then discuss these results regarding strong lensing and SED-fitting uncertainties in order to assess what is believable in the resulting mass function when considering these uncertainties.

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