CLEAR: The Evolution of Spatially Resolved Star Formation in Galaxies between 0.5 ≲ z ≲ 1.7 Using Hα Emission Line Maps

• Published in: The Astrophysical journal 2022-09, Vol.937 (1), p.16
• Main Authors: Matharu, Jasleen, Papovich, Casey, Simons, Raymond C., Momcheva, Ivelina, Brammer, Gabriel, Ji, Zhiyuan, Backhaus, Bren E., Cleri, Nikko J., Estrada-Carpenter, Vicente, Finkelstein, Steven L., Finlator, Kristian, Giavalisco, Mauro, Jung, Intae, Muzzin, Adam, Nelson, Erica J., Pillepich, Annalisa, Trump, Jonathan R., Weiner, Benjamin
• Format: Article
• Language: English
• Subjects: Astrophysics; Emission analysis; Emission lines; Evolution; Field cameras; Galaxies; Galaxy distribution; Galaxy evolution; Galaxy stellar content; H alpha line; High-redshift galaxies; Hubble Space Telescope; Ionization; Red shift; Space telescopes; Spatial distribution; Spectroscopy; Star & galaxy formation; Star formation; Stars & galaxies; Stellar evolution; Stellar mass
• ISSN: 0004-637X; 1538-4357
• DOI: 10.3847/1538-4357/ac8471

Using spatially resolved H α emission line maps of star-forming galaxies, we study the spatial distribution of star formation over a wide range in redshift (0.5 ≲ z ≲ 1.7). Our z ∼ 0.5 measurements come from deep Hubble Space Telescope (HST) Wide Field Camera 3 G102 grism spectroscopy obtained as part of the CANDELS Ly α Emission at Reionization Experiment. For star-forming galaxies with log( M * / M ⊙ ) ≥ 8.96, the mean H α effective radius is 1.2 ± 0.1 times larger than that of the stellar continuum, implying inside-out growth via star formation. This measurement agrees within 1 σ with those measured at z ∼ 1 and z ∼ 1.7 from the 3D-HST and KMOS 3D surveys, respectively, implying no redshift evolution. However, we observe redshift evolution in the stellar mass surface density within 1 kpc (Σ 1kpc ). Star-forming galaxies at z ∼ 0.5 with a stellar mass of log( M * / M ⊙ ) = 9.5 have a ratio of Σ 1kpc in H α relative to their stellar continuum that is lower by (19 ± 2)% compared to z ∼ 1 galaxies. Σ 1kpc,H α /Σ 1kpc,Cont decreases toward higher stellar masses. The majority of the redshift evolution in Σ 1kpc,H α /Σ 1kpc,Cont versus stellar mass stems from the fact that log(Σ 1kpc,H α ) declines twice as much as log(Σ 1kpc,Cont ) from z ∼ 1 to 0.5 (at a fixed stellar mass of log( M * / M ⊙ ) = 9.5). By comparing our results to the TNG50 cosmological magneto-hydrodynamical simulation, we rule out dust as the driver of this evolution. Our results are consistent with inside-out quenching following in the wake of inside-out growth, the former of which drives the significant drop in Σ 1kpc,H α from z ∼ 1 to z ∼ 0.5.