2012
DOI: 10.1093/mnrasl/sls014
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Systematic variation of the stellar initial mass function with velocity dispersion in early-type galaxies

Abstract: An essential component of galaxy formation theory is the stellar initial mass function (IMF), that describes the parent distribution of stellar mass in star forming regions. We present observational evidence in a sample of early-type galaxies (ETGs) of a tight correlation between central velocity dispersion and the strength of several absorption features sensitive to the presence of low-mass stars. Our sample comprises ∼ 40, 000 ETGs from the SPIDER survey (z < ∼ 0.1). The data -extracted from the Sloan Digita… Show more

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Cited by 212 publications
(221 citation statements)
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References 47 publications
(53 reference statements)
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“…We set the lower and upper mass-cutoff of the IMF to 0.1 and 100 M⊙, respectively. It is worth noting that the very lowmass (< 0.6 M⊙) tapered "bimodal" IMF has been found to be consistent with the line-strengths and mass-to-light (M/L) ratios of massive ETGs (e.g., Ferreras et al 2013;La Barbera et al 2013;Spiniello et al 2014). On the contrary, the single power-law "unimodal" IMF leads to extremely high M/L values that are not supported by independent gravitational lensing and dynamical estimates (e.g., Treu et al 2000;Spiniello et al 2012).…”
Section: Imfsupporting
confidence: 57%
“…We set the lower and upper mass-cutoff of the IMF to 0.1 and 100 M⊙, respectively. It is worth noting that the very lowmass (< 0.6 M⊙) tapered "bimodal" IMF has been found to be consistent with the line-strengths and mass-to-light (M/L) ratios of massive ETGs (e.g., Ferreras et al 2013;La Barbera et al 2013;Spiniello et al 2014). On the contrary, the single power-law "unimodal" IMF leads to extremely high M/L values that are not supported by independent gravitational lensing and dynamical estimates (e.g., Treu et al 2000;Spiniello et al 2012).…”
Section: Imfsupporting
confidence: 57%
“…These authors ran a 100 Mpc h −1 cosmological simulation with the N-body/SPH code gadget, with an effective resolution of 3.75 kpc h −1 . The simulations, which included physical prescriptions for momentum-driven winds and chemical enrichment, have previously shown good agreement with the galaxy mass-metallicity relation (Finlator & Davé, 2008), observed IGM enrichment (Oppenheimer & Davé, 2006, 2009, and the cosmological evolution of the UV-luminosity function. Davé et al (2010) identified SMGs as the most heavily star-forming galaxies in their simulations, and chose all SMGs above a given SFR threshold such that their abundance matched the observed number counts of SMGs.…”
Section: Cosmological Hydrodynamic Simulationsmentioning
confidence: 56%
“…For example, observations of gravity sensitive stellar absorption lines (such as FeH, the so called "Wing-Ford" band; Ca II and Na I) aimed at distinguishing K and M dwarfs from K and M giants have found the IMF to be bottom heavy in z ∼ 0 early type galaxies (van Dokkum & Conroy, 2010Conroy & van Dokkum, 2012a,b;Spiniello et al, 2012;Ferreras et al, 2013 Herschel-SPIRE Galaxy (Casey+12) Submillimeter Galaxy (Swinbank+04, Banerji+11, Chapman+prep)…”
Section: Stellar Imfmentioning
confidence: 99%
“…There are indications that the light of stars in massive early type galaxies is consistent with populations formed with a bottom-heavy IMF, as given by the analysis of their spectral features (van Dokkum & Conroy 2010Ferreras et al 2013;La Barbera et al 2013;; in other works, the mass-to-light ratio of massive early type galaxies is constrained by using dynamical tools (Cappellari et al 2012;Dutton et al 2012;Tortora et al 2013) or strong gravitational lensing Treu et al 2010). However, these methods present a degeneracy in the sense that a higher ratio of less massive stars implies either a bottom heavy IMF or a top heavy IMF, since massive stars end their lives in short time-scales and contribute to the total emitted light only during star formation events and shortly after.…”
Section: Discussionmentioning
confidence: 96%