TY - JOUR
T1 - FEASTS
T2 - Radial Distribution of H i Surface Densities Down to 0.01 M⊙pc−2 of 35 Nearby Galaxies
AU - Wang, Jing
AU - Yang, Dong
AU - Lin, Xuchen
AU - Huang, Qifeng
AU - Qu, Zhijie
AU - Chen, Hsiao Wen
AU - Guo, Hong
AU - Ho, Luis C.
AU - Jiang, Peng
AU - Liang, Zezhong
AU - Péroux, Céline
AU - Staveley-Smith, Lister
AU - Weng, Simon
N1 - Publisher Copyright:
© 2025. The Author(s). Published by the American Astronomical Society.
PY - 2025/2/10
Y1 - 2025/2/10
N2 - We present the H i surface density (ΣH i) radial distributions based on total-power H i images obtained by FAST in the FEASTS program, for 35 galaxies with inclinations lower than 72°. We derive the H i radius R001, which is the radius for the 0.01 M⊙ pc−2 (~1018.1 cm−2) isodensity level, 100 times deeper than the 1 M⊙ pc−2 level previously commonly used to measure R1. The profile shapes show a large diversity at a given radius in units of kpc, group virial radius, and R1, but they align more tightly with the radius normalized by R001. The universal H i profile has a scatter of ~0.2 dex and a scale length of ~0.11R001 in the outer region. We derive a new R001-MH i relation, which has a scatter of 0.03 dex and a similar slope of ~0.5 to the previously known R1-MH i relation. Excluding strongly tidal-interacting galaxies, the ratio R001/R1 (anti)correlates strongly and significantly with the H i-to-stellar mass ratio and specific star formation rate, but not with the stellar mass, MH i, dark matter mass, or star formation rate. The strongly tidal-interacting galaxies tend to show deviations from these trends and have the most flattened profiles. These results imply that, in the absence of major tidal interactions, physical processes must cooperate so that ΣH i distributes in a self-similar way in the outer region down to the 0.01 M⊙ pc−2 level.
AB - We present the H i surface density (ΣH i) radial distributions based on total-power H i images obtained by FAST in the FEASTS program, for 35 galaxies with inclinations lower than 72°. We derive the H i radius R001, which is the radius for the 0.01 M⊙ pc−2 (~1018.1 cm−2) isodensity level, 100 times deeper than the 1 M⊙ pc−2 level previously commonly used to measure R1. The profile shapes show a large diversity at a given radius in units of kpc, group virial radius, and R1, but they align more tightly with the radius normalized by R001. The universal H i profile has a scatter of ~0.2 dex and a scale length of ~0.11R001 in the outer region. We derive a new R001-MH i relation, which has a scatter of 0.03 dex and a similar slope of ~0.5 to the previously known R1-MH i relation. Excluding strongly tidal-interacting galaxies, the ratio R001/R1 (anti)correlates strongly and significantly with the H i-to-stellar mass ratio and specific star formation rate, but not with the stellar mass, MH i, dark matter mass, or star formation rate. The strongly tidal-interacting galaxies tend to show deviations from these trends and have the most flattened profiles. These results imply that, in the absence of major tidal interactions, physical processes must cooperate so that ΣH i distributes in a self-similar way in the outer region down to the 0.01 M⊙ pc−2 level.
KW - Inefficient star-formation
KW - Lyman limit systems
KW - Neutral hydrogen
KW - Atomic gas
KW - Circumgalactic medium
KW - Accretion
KW - I.
KW - Simulations
KW - Physics
KW - Discs
UR - http://www.scopus.com/inward/record.url?scp=85219110105&partnerID=8YFLogxK
U2 - 10.3847/1538-4357/ada95a
DO - 10.3847/1538-4357/ada95a
M3 - Article
AN - SCOPUS:85219110105
SN - 0004-637X
VL - 980
JO - Astrophysical Journal
JF - Astrophysical Journal
IS - 1
M1 - 25
ER -