Discovery of Very Minor Merger-Induced Star-forming Clumps at z=3.33 with JWST
Abstract
High-redshift galaxies often contain ''clumps:'' compact, ∼kpc-scale regions of intense star formation. These substructures make up significant fractions of the masses and star-formation rates of their host galaxies and are expected to affect the morphologies of their hosts, such as by building up bulges. Studying clumps can therefore inform theoretical models of galaxy evolution. Two main mechanisms have been proposed for their formation: gas fragmentation from disk instabilities and compression of gas during gravitational interactions with other galaxies. In the latter, only mergers with mass ratios greater than 1:10 have been considered. Here, we report James Webb Space Telescope spectroscopy and imaging of JADES 1034862, a galaxy at zspec = 3.33, which hosts a clump that formed during an interaction with a companion with a stellar mass that is ≈28 times lower than the host. From fits to the spectral energy distributions of the clump and the companion, it is found that both of their star-formation histories rose sharply in the most recent 100-300 Myr, during which the clump formed ∼107.2 M⊙ in stars and currently makes up ≈10% of the total star-formation rate of its host. Given the higher frequency of mergers with low mass ratios (<1:10) to those with higher ratios, we infer that a substantial fraction of high-redshift clumps could have formed through weak gravitational interactions.
Related
- Ionised gas kinematics and star-forming clumps in extremely metal-poor galaxies
- What sets the star-formation rate in the Milky Way?. II. Comparing the star-forming clumps from simulations and observations
- GASTRO Library. II. Exploring Chemical Bimodalities in Disk Galaxies with GSE-like Mergers and Massive Star-forming Clumps
- Ionized Gas Kinematics and Star-forming Clumps in Extremely Metal-poor Galaxies
- Investigating the young stellar populations and hierarchies in nearby galaxies with the UVIT. II. Presenting the properties of ~25,000 UV-detected star-forming clumps
BibTeX
@misc{vega2026discovery,
title = {{Discovery of Very Minor Merger-Induced Star-forming Clumps at $z=3.33$ with JWST}},
author = {Alexander de la Vega and Bahram Mobasher},
howpublished = {arXiv},
year = {2026},
month = sep,
doi = {10.48550/arxiv.2609.05611},
eprint = {2609.05611},
archivePrefix = {arXiv},
url = {https://arxiv.org/abs/2609.05611},
note = {CC BY 4.0},
}
RIS
TY - UNPB
TI - Discovery of Very Minor Merger-Induced Star-forming Clumps at z=3.33 with JWST
AU - Alexander de la Vega
AU - Bahram Mobasher
PY - 2026
DA - 2026/09/04
PB - arXiv
DO - 10.48550/arxiv.2609.05611
UR - https://arxiv.org/abs/2609.05611
AB - High-redshift galaxies often contain ''clumps:'' compact, ∼kpc-scale regions of intense star formation. These substructures make up significant fractions of the masses and star-formation rates of their host galaxies and are expected to affect the morphologies of their hosts, such as by building up bulges. Studying clumps can therefore inform theoretical models of galaxy evolution. Two main mechanisms have been proposed for their formation: gas fragmentation from disk instabilities and compression of gas during gravitational interactions with other galaxies. In the latter, only mergers with mass ratios greater than 1:10 have been considered. Here, we report James Webb Space Telescope spectroscopy and imaging of JADES 1034862, a galaxy at z_spec = 3.33, which hosts a clump that formed during an interaction with a companion with a stellar mass that is ≈28 times lower than the host. From fits to the spectral energy distributions of the clump and the companion, it is found that both of their star-formation histories rose sharply in the most recent 100-300 Myr, during which the clump formed ∼10^7.2 M_⊙ in stars and currently makes up ≈10% of the total star-formation rate of its host. Given the higher frequency of mergers with low mass ratios (<1:10) to those with higher ratios, we infer that a substantial fraction of high-redshift clumps could have formed through weak gravitational interactions.
ER -