TY - JOUR
T1 - Constraining the low-mass slope of the star formation sequence at 0.5 < z < 2.5
AU - Whitaker, Katherine E.
AU - Franx, Marijn
AU - Leja, Joel
AU - Van Dokkum, Pieter G.
AU - Henry, Alaina
AU - Skelton, Rosalind E.
AU - Fumagalli, Mattia
AU - Momcheva, Ivelina G.
AU - Brammer, Gabriel B.
AU - Labbé, Ivo
AU - Nelson, Erica J.
AU - Rigby, Jane R.
N1 - Publisher Copyright:
© 2014. The American Astronomical Society. All rights reserved.
PY - 2014/11/10
Y1 - 2014/11/10
N2 - We constrain the slope of the star formation rate (SFR; log Ψ) to stellar mass (log M ∗) relation down to log (M ∗/M⊙) = 8.4 (log (M ∗/M⊙) = 9.2) at z = 0.5 (z = 2.5) with a mass-complete sample of 39,106 star-forming galaxies selected from the 3D-HST photometric catalogs, using deep photometry in the CANDELS fields. For the first time, we find that the slope is dependent on stellar mass, such that it is steeper at low masses (log Ψlog M ∗) than at high masses (log Ψ(0.3-0.6)log M ∗). These steeper low-mass slopes are found for three different star formation indicators: the combination of the ultraviolet (UV) and infrared (IR), calibrated from a stacking analysis of Spitzer/MIPS 24 μm imaging; β-corrected UV SFRs; and Hα SFRs. The normalization of the sequence evolves differently in distinct mass regimes as well: for galaxies less massive than log (M ∗/M⊙) < 10 the specific SFR (Ψ/M ∗) is observed to be roughly self-similar with Ψ/M ∗∝(1 + z)1.9, whereas more massive galaxies show a stronger evolution with Ψ/M ∗∝(1 + z)2.2-3.5 for log (M ∗/M⊙) = 10.2-11.2. The fact that we find a steep slope of the star formation sequence for the lower mass galaxies will help reconcile theoretical galaxy formation models with the observations.
AB - We constrain the slope of the star formation rate (SFR; log Ψ) to stellar mass (log M ∗) relation down to log (M ∗/M⊙) = 8.4 (log (M ∗/M⊙) = 9.2) at z = 0.5 (z = 2.5) with a mass-complete sample of 39,106 star-forming galaxies selected from the 3D-HST photometric catalogs, using deep photometry in the CANDELS fields. For the first time, we find that the slope is dependent on stellar mass, such that it is steeper at low masses (log Ψlog M ∗) than at high masses (log Ψ(0.3-0.6)log M ∗). These steeper low-mass slopes are found for three different star formation indicators: the combination of the ultraviolet (UV) and infrared (IR), calibrated from a stacking analysis of Spitzer/MIPS 24 μm imaging; β-corrected UV SFRs; and Hα SFRs. The normalization of the sequence evolves differently in distinct mass regimes as well: for galaxies less massive than log (M ∗/M⊙) < 10 the specific SFR (Ψ/M ∗) is observed to be roughly self-similar with Ψ/M ∗∝(1 + z)1.9, whereas more massive galaxies show a stronger evolution with Ψ/M ∗∝(1 + z)2.2-3.5 for log (M ∗/M⊙) = 10.2-11.2. The fact that we find a steep slope of the star formation sequence for the lower mass galaxies will help reconcile theoretical galaxy formation models with the observations.
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U2 - 10.1088/0004-637X/795/2/104
DO - 10.1088/0004-637X/795/2/104
M3 - Article
AN - SCOPUS:84908456476
SN - 0004-637X
VL - 795
JO - Astrophysical Journal
JF - Astrophysical Journal
IS - 2
M1 - 104
ER -