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$M_*/L$ gradients driven by IMF variation: Large impact on dynamical stellar mass estimates

Authors :
Ravi K. Sheth
J. L. Fischer
Kyu-Hyun Chae
Francesco Shankar
Mariangela Bernardi
H. Domínguez-Sánchez
Marc Huertas-Company
Galaxies, Etoiles, Physique, Instrumentation (GEPI)
Institut national des sciences de l'Univers (INSU - CNRS)-Observatoire de Paris
PSL Research University (PSL)-PSL Research University (PSL)-Centre National de la Recherche Scientifique (CNRS)
Galaxies, Etoiles, Physique, Instrumentation ( GEPI )
Institut national des sciences de l'Univers ( INSU - CNRS ) -Observatoire de Paris-Université Paris Diderot - Paris 7 ( UPD7 ) -Centre National de la Recherche Scientifique ( CNRS )
Université Paris sciences et lettres (PSL)-Université Paris sciences et lettres (PSL)-Université Paris Diderot - Paris 7 (UPD7)-Centre National de la Recherche Scientifique (CNRS)
Source :
Mon.Not.Roy.Astron.Soc., Mon.Not.Roy.Astron.Soc., 2018, 477 (2), pp.2560-2571. ⟨10.1093/mnras/sty781⟩, Mon.Not.Roy.Astron.Soc., 2018, 477, pp.2560. 〈10.1093/mnras/sty781〉, Monthly Notices of the Royal Astronomical Society, Monthly Notices of the Royal Astronomical Society, Oxford University Press (OUP): Policy P-Oxford Open Option A, 2018, 477 (2), pp.2560-2571. ⟨10.1093/mnras/sty781⟩
Publication Year :
2018
Publisher :
HAL CCSD, 2018.

Abstract

Within a galaxy the stellar mass-to-light ratio $\Upsilon_*$ is not constant. Spatially resolved kinematics of nearby early-type galaxies suggest that allowing for a variable initial mass function (IMF) returns significantly larger $\Upsilon_*$ gradients than if the IMF is held fixed. If $\Upsilon_*$ is greater in the central regions, then ignoring the IMF-driven gradient can overestimate $M_*^{\rm dyn}$ by as much as a factor of two for the most massive galaxies, though stellar population estimates $M_*^{\rm SP}$ are also affected. Large $\Upsilon_*$-gradients have four main consequences: First, $M_*^{\rm dyn}$ cannot be estimated independently of stellar population synthesis models. Second, if there is a lower limit to $\Upsilon_*$ and gradients are unknown, then requiring $M_*^{\rm dyn}=M_*^{\rm SP}$ constrains them. Third, if gradients are stronger in more massive galaxies, then $M_*^{\rm dyn}$ and $M_*^{\rm SP}$ can be brought into agreement, not by shifting $M_*^{\rm SP}$ upwards by invoking constant bottom-heavy IMFs, as advocated by a number of recent studies, but by revising $M_*^{\rm dyn}$ estimates in the literature downwards. Fourth, accounting for $\Upsilon_*$ gradients changes the high-mass slope of the stellar mass function $\phi(M_*^{\rm dyn})$, and reduces the associated stellar mass density. These conclusions potentially impact estimates of the need for feedback and adiabatic contraction, so our results highlight the importance of measuring $\Upsilon_*$ gradients in larger samples.<br />Comment: 13 pages, 7 figures, MNRAS in press

Details

Language :
English
ISSN :
00358711 and 13652966
Database :
OpenAIRE
Journal :
Mon.Not.Roy.Astron.Soc., Mon.Not.Roy.Astron.Soc., 2018, 477 (2), pp.2560-2571. ⟨10.1093/mnras/sty781⟩, Mon.Not.Roy.Astron.Soc., 2018, 477, pp.2560. 〈10.1093/mnras/sty781〉, Monthly Notices of the Royal Astronomical Society, Monthly Notices of the Royal Astronomical Society, Oxford University Press (OUP): Policy P-Oxford Open Option A, 2018, 477 (2), pp.2560-2571. ⟨10.1093/mnras/sty781⟩
Accession number :
edsair.doi.dedup.....0b8779d1d29ef871a4903128d233df2a
Full Text :
https://doi.org/10.1093/mnras/sty781⟩