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WorksPhysics and Astronomy

The clumpy fraction of galaxies at z=1−9z=1-9 with JADES: evidence for a mass-dependent transition in clump origin

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Abstract · v1

We measure the fraction of clumpy galaxies (fclumpyf_{\rm clumpy}) over the redshift range z=1−9z=1-9 and stellar masses log⁡10(M⋆/M⊙)≥8\log_{10}(M_\star/{\rm M_\odot}) \geq 8 using JWST/NIRCam imaging from JADES. We define clumps as compact off-centre surface-brightness peaks with characteristic sizes of a few hundred parsecs, and develop a dendrogram-based clump-finding method with astrodendro to identify them directly in rest-frame UV, blue, and optical images. Clump-detection completeness is quantified through injection-recovery simulations, which we use to define (M⋆M_\star, zz)-dependent 50 per cent completeness-limited fclumpyf_{\rm clumpy}, alongside a probability-weighted completeness-corrected statistic for comparison. For the full sample, the blue and optical fclumpyf_{\rm clumpy} reach ≈55\approx55 per cent at z≈1−2z\approx1-2 and decline to ≲5\lesssim5 per cent by z≈8−9z\approx8-9, while the UV fraction remains higher at ≈12\approx12 per cent. At z≈1−2z\approx1-2, fclumpyf_{\rm clumpy} increases strongly with stellar mass, from ≈35\approx35 per cent in the lowest-mass bin to ≈85\approx85 per cent at log⁡10(M⋆/M⊙)≥10\log_{10}(M_\star/{\rm M_\odot})\geq10. Most clumpy galaxies host only one or two robustly detected off-centre clumps, while higher-multiplicity systems occur preferentially in massive, strongly star-forming galaxies at low to intermediate redshift. Comparison with major merger rates suggests that mergers could account for a substantial fraction of low-mass (log⁡10(M⋆/M⊙)<8.5\log_{10}(M_\star/{\rm M_\odot})<8.5), high-redshift clumpy galaxies, while the observed fractions in more massive systems (log⁡10(M⋆/M⊙)>9\log_{10}(M_\star/{\rm M_\odot})>9) require an additional in situ clump-formation channel. Our results are consistent with a transition from merger-dominated clumpy morphologies at early times and low stellar masses to an increasing contribution from in situ clump-formation channels, such as disc instabilities, in more massive systems.

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