The Dual Nature of GHZ9: Coexisting AGN and Star Formation Activity in a Remote X-ray Source at Z=10.145

Lorenzo Napolitano,Marco Castellano,Laura Pentericci,Cristian Vignali,Roberto Gilli,Adriano Fontana,Paola Santini,Tommaso Treu,Antonello Calabrò, Mario Llerena,Enrico Piconcelli, Luca Zappacosta,Sara Mascia, Pietro Bergamini, Tom J. L. C. Bakx,Mark Dickinson,Karl Glazebrook, Alaina Henry,Nicha Leethochawalit, Giovanni Mazzolari, Emiliano Merlin, Takahiro Morishita, Themiya Nanayakkara, Diego Paris,Simonetta Puccetti, Guido Roberts-Borsani, Sofia Rojas Ruiz,Eros Vanzella, Fabio Vito,Benedetta Vulcani,Xin Wang, Ilsang Yoon,Jorge A. Zavala

arxiv(2024)

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摘要
We present JWST/NIRSpec PRISM spectroscopic characterization of GHZ9 at z= 10.145 ± 0.010, currently the most distant source detected by the Chandra X-ray Observatory. The spectrum reveals several UV high-ionization lines, including CII, SiIV, [NIV], CIV, HeII, OIII], NIII], and CIII]. The prominent rest-frame equivalent widths (EW(CIV)≃65A, EW(HeII)≃18A, EW(CIII])≃48A) show the presence of a hard radiation field, while the analysis of line ratio diagnostics suggest this galaxy hosts both AGN and star-formation activity. GHZ9 is nitrogen-enriched (6–9.5 times solar), carbon-poor (0.2–0.65 times solar), metal-poor (Z = 0.01–0.1 Z_⊙), and compact (< 106 pc), similarly to GNz11, GHZ2, and recently discovered N-enhanced high redshift objects. We exploited the newly available JWST/NIRSpec and NIRCam dataset to perform an independent analysis of the Chandra data confirming that GHZ9 is the most likely JWST source associated to X-ray emission at 0.5-7 keV. Assuming a spectral index Γ = 2.3 (1.8), we estimate a black hole (BH) mass of 1.60 ± 0.31 (0.48 ± 0.09) × 10^8M_⊙, which is consistent either with Eddington-accretion onto heavy (≥ 10^6 M_⊙) BH seeds formed at z=18, or super-Eddington accretion onto a light seed of ∼ 10^2-10^4 M_⊙ at z = 25. The corresponding BH-to-stellar mass ratio M_BH/M_star= 0.33±0.22 (0.10±0.07), with a stringent limit >0.02, implies an accelerated growth of the BH mass with respect to the stellar mass. GHZ9 is the ideal target to constrain the early phases of AGN-galaxy coevolution with future multi-frequency observations.
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