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Discovery of a Broad-Line Active Galactic Nucleus at $z = 9.98$

Astrophysics of Galaxies · Submitted 20 Oct 2026 · 91 references

Pith's verdict: The highest-redshift broad-line AGN candidate is a real discovery if the marginal Hβ detection at the extended-wavelength limit holds up. The paper is honest about the fragility, but the result needs independent confirmation.

T0 · AI review

How this review was made: An AI referee (deepseek/deepseek-v4-flash) read the paper on October 22, 2026 and answered a fixed list of questions about it. T0 is the starting level every paper gets. The levels describe how deeply Pith has checked the paper, never the authors.

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arXiv ID2610.28735 (version 1)
Pith IDUEOG5VSM, Pith's permanent record of this paper and its review
CitationAkio K. Inoue, Anna de Graaff, Ivo Labbe, Jenny E. Greene, Jorryt Matthee, Ken Mawatari, Masafusa Onoue, Pascal A. Oesch, Pratika Dayal, Rohan P. Naidu, Suzuka Arai, Xi Kang, Xingyao Cai, Yoshinobu Fudamoto, Yuma Sugahara. "Discovery of a Broad-Line Active Galactic Nucleus at $z = 9.98$." arXiv:2610.28735 (2026). https://pith.science/paper/UEOG5VSM
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Referee report
The paper

The paper claims

MoM-BL-z10 is a broad-line active galactic nucleus at redshift 9.9837, the highest-redshift such object known, and its broad Hβ emission enables the first virial black hole mass estimate at z ≈ 10.

The reading

The paper reports the discovery of MoM-BL-z10, a broad-line active galactic nucleus (BL AGN) at a spectroscopic redshift of 9.9837, identified through a systematic search of public JWST/NIRSpec PRISM spectra. The detection of a broad component in the Hβ emission line (signal‑to‑noise ratio 3.87, full width at half‑maximum 3480 km/s) is statistically preferred over a narrow‑line‑only model, and supporting emission‑line ratios from [Ne III] and [O III] place the source firmly in the AGN region of standard excitation diagrams. If confirmed, this object becomes the highest‑redshift broad‑line AGN known, and it provides the first opportunity to estimate a virial supermassive‑black‑hole mass at z ≈ 10 (MBH ≈ 3.6 × 10⁷ M☉ under standard quasar corrections, or ≈ 2.1 × 10⁶ M☉ under an alternative Little‑Red‑Dot scenario). The inferred black‑hole mass at a cosmic age of only 470 Myr challenges models of early black‑hole growth, requiring either super‑Eddington accretion from stellar‑mass seeds or more massive seed black holes.

What carries the argument

The detection relies on the JWST/NIRSpec PRISM spectrum reduced by the DAWN JWST Archive (DJA) reduction, which recovers second‑ and third‑order spectra beyond the standard 5.3 μm pipeline cutoff, thereby covering Hβ at 5.35 μm for a z ≈ 10 source. The broad‑line identification is made by fitting a broken‑power‑law continuum, then comparing narrow‑only and narrow‑plus‑broad Gaussian models of the Hβ+[O III] complex convolved with the wavelength‑dependent NIRSpec line spread function, using the Bayesian Information Criterion (ΔBIC < −6) and a broad‑line S/N ≥ 3. The virial black‑hole mass is derived from the standard single‑epoch calibration (Kaspi et al. 2000) that uses the broad Hβ FWHM and the rest‑frame 5100 Å continuum luminosity.

Extended reading notes

Core claim

The paper claims that the source MoM-BL-z10 is a broad‑line AGN at z = 9.9837 ± 0.0009, making it the highest‑redshift broad‑line AGN identified to date. The central piece of evidence is a broad component in the Hβ emission line at 5.35 µm, detected at S/N = 3.87 with FWHM = 3480⁺²⁰⁴⁰₋₉₅₀ km s⁻¹, which is strongly preferred over a narrow‑line‑only model (ΔBIC = −15.55). Additional support comes from the detection of [Ne III] λ3870, from the positions of MoM-BL-z10 in the [Ne III]/[O II] versus [O III]/[O II] and [O III]/Hβ versus [Ne III]/[O II] diagnostic diagrams, which fall in the AGN region and are well separated from star‑forming galaxies, and from its compact NIRCam morphology. Using the broad Hβ width and the rest‑frame 5100 Å continuum luminosity, the authors derive a virial black‑hole mass of MBH = 3.6⁺⁵·⁸₋₁·⁷ × 10⁷ M☉ and an Eddington ratio λEdd = 0.11⁺⁰·¹⁰₋₋₀·₀₇. An alternative interpretation that adopts a bolometric correction appropriate for Little Red Dots and assumes Eddington‑limited accretion yields MBH,LRD = 2.1⁺⁰·⁶₋₀·₅ × 10⁶ M☉. Under either scenario, the existence of a multi‑million‑solar‑mass black hole when the Universe was only 470 Myr old poses a serious challenge to rapid black‑hole growth models.

Load-bearing premise

The broad Hβ component is detected at S/N = 3.87, which is just above the 3σ selection threshold, and the detection requires a non-standard data reduction that recovers spectra beyond the official 5.3 μm pipeline cutoff; if that extended reduction introduces systematic errors or if the signal is a noise fluctuation, the broad-line claim collapses.

Editorial extensions

If this is right

  • MoM-BL-z10 becomes the first broad‑line AGN at z ≈ 10, extending by almost one full redshift unit the reach of virial black‑hole mass estimates, which previously stopped at z ≈ 9.3.
  • The inferred black‑hole mass of either ∼ 3 × 10⁷ M☉ or ∼ 2 × 10⁶ M☉ at 470 Myr after the Big Bang provides a new observational benchmark that tightens the constraints on seed black‑hole mass and accretion history.
  • If the object is confirmed as a Little Red Dot (LRD), it would strengthen the connection between the LRD population and accreting supermassive black holes at the highest redshifts.
  • The Hβ emission lies near the long‑wavelength limit of the extended NIRSpec coverage, suggesting that similar spectroscopic searches at z ≳ 10 may require alternative tracers such as high‑ionization emission lines or X‑ray observations.

Reading between the lines

Editorial extensions of the paper, not claims the author makes directly.

  • The paper’s reliance on a single broad line at modest S/N (3.87) and on a non‑standard data‑reduction step means that independent confirmation (e.g., through a deeper NIRSpec spectrum or a MIRI detection of broad Hα) is essential before the object can be considered a securely established broad‑line AGN at z = 10.
  • If the alternative LRD‑calibrated mass (∼ 2 × 10⁶ M☉) is closer to the truth, the tension with early‑growth models eases considerably, but the object would still require super‑Eddington accretion from a stellar‑mass seed or a heavy seed of ∼ 10⁴–10⁵ M☉.
  • The broad‑line search that uncovered MoM-BL-z10 is part of a larger systematic survey (X. Cai et al. in preparation); the full sample, with its well‑characterised selection function, will allow a first estimate of the space density of faint broad‑line AGNs at z > 6 and may reveal more such objects near the spectroscopic limit.
  • The tentative MIRI F770W detection and the red rest‑frame optical continuum suggest that this object may also be a candidate for the Little Red Dot population at z ≈ 10, linking the early‑AGN and LRD phenomena in a redshift regime where very few examples have been studied spectroscopically.
Original abstract

The James Webb Space Telescope (JWST) has uncovered a previously unexplored population of faint active galactic nuclei (AGNs) in the early Universe. We present MoM-BL-z10 at $z=9.9837\pm0.0009$, identified through a systematic search for broad-line AGNs at $z\geq6$ using public JWST/NIRSpec PRISM spectra from the DAWN JWST Archive. The PRISM spectrum exhibits a broad component in H$\beta$ at 5.35 microns. A narrow+broad Gaussian fit yields a broad H$\beta$ detection at S/N = 3.87, with FWHM = $3480^{+2040}_{-950}$ km s$^{-1}$ and $L_{{\rm H}\beta,{\rm broad}}=1.25^{+0.33}_{-0.31}\times10^{42}$ erg s$^{-1}$. The detection of [Ne III] $\lambda3870$ and the high [Ne III]/[O II] and [O III]/H$\beta$ ratios further support the AGN interpretation. Its rest-frame UV and optical continuum slopes, compact NIRCam morphology, and a tentative MIRI F770W detection suggest similarities to Little Red Dots (LRDs). The broad H$\beta$ detection enables the first virial SMBH mass estimate at $z\sim10$. We derive $M_{\rm BH}=3.6^{+5.8}_{-1.7}\times10^7 M_\odot$ and $\lambda_{\rm Edd}=0.11^{+0.10}_{-0.07}$ using the standard single-epoch virial calibration and quasar bolometric correction. We also consider an alternative scenario adopting the LRD-specific bolometric correction and assuming $\lambda_{\rm Edd}=1$, which yields $M_{\rm BH}=2.1^{+0.6}_{-0.5}\times10^6 M_\odot$. Under either scenario, the inferred SMBH mass at a cosmic age of only 470 Myr highlights the challenge of rapid BH growth in the early Universe, suggesting super-Eddington accretion from a stellar-mass seed or a more massive seed. As the highest-redshift broad-line AGN identified to date, MoM-BL-z10 provides a new observational benchmark for understanding the early growth of supermassive black holes.

The compiled record

The paper's own sentences, arranged, kept beside the review and separate from it. Each label is drawn from a closed vocabulary; the number beside it is the probability the classifier gave that label. Numbers in the tables are the authors', checked by code. No sentence in this record was written by a model.

Compiled by classifier-1.13.0 via TypeSafe API, question bank abstract-p1-20260923, 2026-10-22: 1 request, 8,900 input tokens.

What the abstract itself states, as probabilities: claims first 0.81 · states limitation 0.79 · human participants 0.01 · controlled comparison 0.04 · randomized assignment 0.01 · states quantitative result 0.99 · compares with prior results 0.74 · mentions code or data availability 0.04.

The abstract, sentence by sentence

arXiv listing abstract v1. Results and the main claim are underlined; .

The James Webb Space Telescope (JWST) has uncovered a previously unexplored population of faint active galactic nuclei (AGNs) in the early Universe. We present MoM-BL-z10 at $z=9.9837\pm0.0009$, identified through a systematic search for broad-line AGNs at $z\geq6$ using public JWST/NIRSpec PRISM spectra from the DAWN JWST Archive. The PRISM spectrum exhibits a broad component in H$\beta$ at 5.35 microns. A narrow+broad Gaussian fit yields a broad H$\beta$ detection at S/N = 3.87, with FWHM = $3480^{+2040}_{-950}$ km s$^{-1}$ and $L_{{\rm H}\beta,{\rm broad}}=1.25^{+0.33}_{-0.31}\times10^{42}$ erg s$^{-1}$. The detection of [Ne III] $\lambda3870$ and the high [Ne III]/[O II] and [O III]/H$\beta$ ratios further support the AGN interpretation. Its rest-frame UV and optical continuum slopes, compact NIRCam morphology, and a tentative MIRI F770W detection suggest similarities to Little Red Dots (LRDs). The broad H$\beta$ detection enables the first virial SMBH mass estimate at $z\sim10$. We derive $M_{\rm BH}=3.6^{+5.8}_{-1.7}\times10^7 M_\odot$ and $\lambda_{\rm Edd}=0.11^{+0.10}_{-0.07}$ using the standard single-epoch virial calibration and quasar bolometric correction. We also consider an alternative scenario adopting the LRD-specific bolometric correction and assuming $\lambda_{\rm Edd}=1$, which yields $M_{\rm BH}=2.1^{+0.6}_{-0.5}\times10^6 M_\odot$. Under either scenario, the inferred SMBH mass at a cosmic age of only 470 Myr highlights the challenge of rapid BH growth in the early Universe, suggesting super-Eddington accretion from a stellar-mass seed or a more massive seed. As the highest-redshift broad-line AGN identified to date, MoM-BL-z10 provides a new observational benchmark for understanding the early growth of supermassive black holes.

background contribution method result interpretation main claim

What the classifier reports for each sentence. The number is the probability it gave the label.
#sentencerolethe authors' own workstates the main conclusionstrength
s0 The James Webb Space Telescope (JWST) has uncovered a previously unexplored population of faint active galactic nuclei (AGNs) in the early Universe. background 0.96 0.21 0.06 asserted 1.00
s1 We present MoM-BL-z10 at $z=9.9837\pm0.0009$, identified through a systematic search for broad-line AGNs at $z\geq6$ using public JWST/NIRSpec PRISM spectra from the DAWN JWST Archive. contribution 0.92 0.96 0.29 asserted 1.00
s2 The PRISM spectrum exhibits a broad component in H$\beta$ at 5.35 microns. result 0.98 0.85 0.03 asserted 1.00
s3 A narrow+broad Gaussian fit yields a broad H$\beta$ detection at S/N = 3.87, with FWHM = $3480^{+2040}_{-950}$ km s$^{-1}$ and $L_{{\rm H}\beta,{\rm broad}}=1.25^{+0.33}_{-0.31}\times10^{42}$ erg s$^{-1}$. result 1.00 0.96 0.06 asserted 1.00
s4 The detection of [Ne III] $\lambda3870$ and the high [Ne III]/[O II] and [O III]/H$\beta$ ratios further support the AGN interpretation. interpretation 0.51 0.87 0.04 asserted 0.77
s5 Its rest-frame UV and optical continuum slopes, compact NIRCam morphology, and a tentative MIRI F770W detection suggest similarities to Little Red Dots (LRDs). interpretation 0.69 0.87 0.04 hedged possibility 0.99
s6 The broad H$\beta$ detection enables the first virial SMBH mass estimate at $z\sim10$. contribution 0.49 0.77 0.18 asserted 0.98
s7 We derive $M_{\rm BH}=3.6^{+5.8}_{-1.7}\times10^7 M_\odot$ and $\lambda_{\rm Edd}=0.11^{+0.10}_{-0.07}$ using the standard single-epoch virial calibration and quasar bolometric correction. result 1.00 0.97 0.13 asserted 1.00
s8 We also consider an alternative scenario adopting the LRD-specific bolometric correction and assuming $\lambda_{\rm Edd}=1$, which yields $M_{\rm BH}=2.1^{+0.6}_{-0.5}\times10^6 M_\odot$. result 0.90 0.93 0.05 hedged possibility 0.57
s9 Under either scenario, the inferred SMBH mass at a cosmic age of only 470 Myr highlights the challenge of rapid BH growth in the early Universe, suggesting super-Eddington accretion from a stellar-mass seed or a more massive seed. interpretation 1.00 0.81 0.54 hedged possibility 0.88
s10 As the highest-redshift broad-line AGN identified to date, MoM-BL-z10 provides a new observational benchmark for understanding the early growth of supermassive black holes. interpretation 0.61 0.88 0.62 asserted 1.00

What kind of paper the classifier reports this is: empirical study 1.00 · evidence from analysis of existing data 0.88.

What was examined, and what was not

sources read
  • arXiv listing abstract v1
not examined
  • full text
  • figures and tables
  • references and citing sentences
  • relations to other papers
levels run
  • P abstract
not run
  • S sections
  • T body sentences
  • C citations
  • R cross-paper relations

Every quoted sentence on this record is the authors'. Every label is from Pith's closed vocabulary, with the probability shown beside it. Every number in the measurements table is the authors', checked by code. Record as JSON

Figures
Figure 1. JWST spectroscopy and imaging of MoM-BL-z10. The top row shows 2 × 2 arcsec2 cutout images in 7 NIRCam broadbands from F090W to F444W. The rightmost panel shows a pseudo-color image (blue: F090W+F115W+F150W; green: F200W+F277W; red: F356W+F444W). The middle panels show the 2D and 1D NIRSpec/PRISM spectra. In the 2D spectrum, positive and negative signals are shown in blue and white, respectively. The blue shaded region in the 1D spectrum indicates 1σ uncertainties. The positions of Lyα and Hβ+[O III] are marked. The right-hand panels show the Hγ+[O iii] λ4364 and the Hβ+[O iii]…
Figure 2. Rest-frame UV-to-near-infrared SED of MoM-BL-z10, combining NIRCam and MIRI photometry with a scaled PRISM spectrum (see text). For visualization, the PRISM spectrum is resampled onto a logarithmic wavelength grid with a fixed velocity step of ∆v = 1160 km s−1 . Black circles show the NIRCam photometry, and grey arrows indicate the 3σ upper limits for undetected bands. Open orange squares show synthetic PRISM photometry, obtained by convolving the scaled PRISM spectrum with the NIRCam filter transmission curves. The filled diamond shows the tentative MIRI F770W detection. The open…
Figure 3. The [O ii]-FLR (left) and OHNO (right) diagnostics. The yellow star shows MoM-BL-z10, where we infer the [O iii] λ5008 from the [O iii] λ4960 flux by assuming a fiducial flux ratio of 2.98, and only the narrow Hβ component is used. The error bars reflect the propagated 1σ measurement uncertainties of the emission-line fluxes. An additional 0.20-dex uncertainty is added in quadrature to log([Ne III]/[O II]) to account for possible blending with Hη, Hζ, and He I λ3889 (e.g., R. Tripodi et al. 2025). Blue points show the SDSS AGN sample selected from BPT and [Ne v] λ3426 emission in…
Figure 4. Black hole mass–bolometric luminosity distribu￾tion at z ≳ 8. The yellow star shows MoM-BL-z10 with the black hole mass estimated using the Hβ-based calibra￾tion of S. Kaspi et al. (2000) and the standard bolomet￾ric correction for quasars (Lbol = 9.26L5100; G. T. Richards et al. 2006). The white star shows the alternative LRD case for the same object, adopting the bolometric correction of Lbol,LRD = 5L5100 (J. E. Greene et al. 2026) and assuming an Eddington-limited accretion (λEdd = 1). In the LRD-based MBH estimate, only the uncertainty of continuum luminosity is considered in…
Figure 5. Illustrative black hole growth tracks of MoM-BL-z10 as a function of redshift assuming continuous accretion at fixed Eddington ratios with 10% radiative efficiency. The yellow star shows the fiducial virial SMBH mass of MoM-BL-z10, while the white star shows the LRD-based SMBH mass estimate assuming Eddington-limited accretion. The yellow stripe shows the backward extrapolation of the fiducial BH mass, assuming the observed Eddington ratio of λEdd = 0.1. The orange and blue stripes show the expected growth curves from a heavy (104−5 M⊙) and a light (10–100 M⊙) seed BH, respectively,…

Figures reproduced from arXiv:2610.28735 by the authors.

References

Discussion

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