HST/ACS Morphology of Lyman Alpha Emitters at Redshift 5.7 in the COSMOS Field
Y. Taniguchi, T. Murayama, N. Z. Scoville, S. S. Sasaki, T. Nagao, Y., Shioya, T. Saito, Y. Ideue, A. Nakajima, K. Matsuoka, D. B. Sanders, B., Mobasher, H. Aussel, P. Capak, M. Salvato, A. Koekemoer, C. Carilli, A., Cimatti, R. S. Ellis, B. Garilli, M. Giavalisco, O. Ilbert

TL;DR
This study analyzes the morphology of Lyman alpha emitters at redshift 5.7 using HST/ACS data, revealing their sizes, structures, and light profiles, and comparing UV continuum and Lyα emission properties.
Contribution
It provides detailed morphological analysis of LAEs at z~5.7 with high-resolution imaging, highlighting their sizes, structures, and light profiles, which was not extensively studied before at this redshift.
Findings
Nearly half of LAEs are spatially extended beyond 0.15 arcsec.
Most LAEs have disk-like or irregular light profiles with a Sersic index around 0.7.
Larger UV continuum sizes correlate with larger Lyα emission regions.
Abstract
We present detailed morphological properties of Lyman alpha emitters (LAEs) at z~ 5.7 in the COSMOS field, based on {\it Hubble Space Telescope} Advanced Camera for Surveys (ACS) data. The ACS imaging in the F814W filter covered 85 LAEs of the 119 LAEs identified in the full two square degree field, and 47 LAEs of them are detected in the ACS images. Nearly half of them are spatially extended with a size larger than 0.15 arcsec (~0.88 kpc at z=5.7) up to 0.4 arcsec (~2.5 kpc at z=5.7). The others are nearly unresolved compact objects. Two LAEs show double-component structures, indicating interaction or merging of building components to form more massive galaxies. By stacking the ACS images of all the detected sources, we obtain a Sersic parameter of n~0.7 with a half-light radius of 0.13 arcsec (0.76 kpc), suggesting that the majority of ACS detected LAEs have not spheroidal-like but…
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Taxonomy
TopicsCCD and CMOS Imaging Sensors · Galaxies: Formation, Evolution, Phenomena · Astronomy and Astrophysical Research
