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The dark side of early galaxies: geko\texttt{geko} uncovers dark-matter fractions at z46z\sim4-6

Published 16 Oct 2025 in astro-ph.GA | (2510.14779v1)

Abstract: JWST/NIRCam slitless spectroscopy enables dynamical mass measurements for typical star-forming galaxies only a billion years after the Big Bang. We model the Hα\alpha morpho-kinematics of 163 galaxies at redshift z4z\approx4-6 from FRESCO and CONGRESS (with JADES imaging), using the geko\texttt{geko} code, and infer rotational velocities and dispersions within rer_{\rm e}. Our sample spans logM7\log M_{\star}\approx7-10 and logMdyn9\log M_{\rm dyn}\approx9-11. Gas masses are estimated via scaling relations, yielding baryonic masses and dark-matter (DM) fractions $f_{\rm DM}(r<r_{\rm e})$ within the Hα\alpha half-light radius. We find high median fractions of fgas=0.77\langle f_{\rm gas}\rangle=0.77 and fDM=0.73\langle f_{\rm DM}\rangle=0.73, where fgasf_{\rm gas} is measured with respect to the baryonic mass and fDMf_{\rm DM} with respect to the DM+baryonic mass. About two-thirds of systems are DM-dominated within re0.51r_{\rm e}\sim0.5-1 kpc. Both fgasf_{\rm gas} and fDMf_{\rm DM} decrease with stellar mass, consistent with simulations. The stellar Tully-Fisher relation shows a tentative offset to higher vcircv_{\rm circ} at fixed MM_{\star} and substantial intrinsic scatter, suggesting that the relation is only beginning to emerge at z5z\sim5. We measure a negative correlation between fDMf_{\rm DM} and baryonic surface density Σbar\Sigma_{\rm bar}, weaker but broadly consistent with trends at cosmic noon and at z0z\sim0. Qualitatively comparing with modified NFW profiles coupled to an empirical stellar-to-halo mass relation suggests that the lowest fDMf_{\rm DM} (0.4\lesssim0.4) require cored inner DM profiles, while the highest fractions favour cuspier profiles, potentially reflecting adiabatic contraction. Overall, the elevated fgasf_{\rm gas} and fDMf_{\rm DM} at z4z\gtrsim4 are compatible with progenitors of baryon-dominated systems at z2z\sim2 and naturally anticipate overmassive black holes at fixed MM_{\star}.

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