Weekly issue

Week 25, 2025

Jun 16–22, 2025

Week 25, 2025 includes 7 curated papers, centered on high-z, QSO, overmassive BH.

Digest

The authors measure the z=4–10 X-ray luminosity function at intermediate luminosities by combining UltraVISTA-selected COSMOS2020 galaxies with Chandra COSMOS imaging, using both blind detections and forced X-ray extraction (21 blind + 11 extracted). They find AGN space densities that exceed low‑z XLF extrapolations: consistent at z=4–5, but ~10× higher at z=5–7 and potentially up to ~220× at z=7–10. The sample indicates a dominantly obscured early AGN population with an obscured fraction of 0.982(+0.007/−0.008), and correcting for this further boosts the inferred densities. These results bridge bright-end quasar counts and JWST detections of faint AGN, implying a larger fraction of early galaxies hosted rapidly growing SMBHs than previously thought.

Key figures to inspect

  • Figure 1: Inspect the hard/full-band area curves to see the survey selection function—how sky coverage versus count rate (and the flux conversion assumptions) sets the accessible Lx range that underpins the z=4–10 XLF bins.
  • Figure 2: Compare false-probability histograms for blind versus extracted sources and the high‑z subset to understand contamination control, the effect of masking around blind detections, and where the adopted thresholds place the high‑z candidates.
  • Figure 3: Follow how the false fraction changes with the chosen probability threshold for the combined catalog; this justifies the final threshold that targets ~5% false positives among high‑z sources and sets the reliability of the extracted detections.
  • Figure 4: Examine rest‑frame 2–10 keV Lx versus redshift with both galaxy- and AGN-template photo‑z fits; note which points would drop out of the high‑z sample and how conservative vs optimistic selections map onto the moderate‑Lx regime used for the XLF.

Tags

  • obscured AGN
  • demographics
  • X-ray

2506.14870v1

JADES and BlackTHUNDER: rest-frame Balmer-line absorption and the local environment in a Little Red Dot at z = 5

Francesco D'Eugenio, Ignas Juodžbalis, Xihan Ji, Jan Scholtz, Roberto Maiolino, Stefano Carniani, Michele Perna, Giovanni Mazzolari, Hannah Übler, Santiago Arribas, Rachana Bhatawdekar, Andrew J. Bunker, Giovanni Cresci, Emma Curtis-Lake, Kevin Hainline, Kohei Inayoshi, Yuki Isobe, Benjamin D. Johnson, Gareth C. Jones, Tobias J. Looser, Erica J. Nelson, Eleonora Parlanti, Dávid Puskás, Pierluigi Rinaldi, Brant Robertson, Bruno Rodríguez Del Pino, Irene Shivaei, Fengwu Sun, Sandro Tacchella, Giacomo Venturi, Marta Volonteri, Christina C. Williams, Christopher N. A. Willmer, Chris Willott, Joris Witstok

Theme match 5/5

Digest

Reports a broad-line Little Red Dot at z=5.077 (JADES-GS+033223.41-275404.5/159717) with NIRSpec MSA+IFU, revealing multi-component Hα including two broad Gaussians. A virial black hole mass of log(MBH/M⊙)=7.65 and a narrow [O III] λ5007-based dynamical mass of log(Mdyn/M⊙)=9.1 imply a BH overmassive relative to its host. The source sits in a 7-kpc pool of ionized gas with three neighbors (a satellite, a possible satellite/gas cloud, and a tentatively detected spatially detached outflow). A deep rest-frame Hα absorber (deeper than the continuum; v=-13 km s−1, σ=120 km s−1) appears in G395H but not G395M, with tentative EW variability over two rest-frame months (2.6σ), underscoring resolution- and time-dependent incidence of absorbers in LRDs.

Key figures to inspect

  • Hα profile decomposition from the G395H spectrum: inspect the two broad Gaussian components plus the deep rest-frame absorber exceeding the continuum to verify the non-stellar origin and measure v=-13 km s−1, σ=120 km s−1 and EW.
  • Side-by-side G395H vs G395M spectra around Hα: confirm that the absorber is prominent at high resolution yet absent at medium resolution, illustrating how spectral resolution biases absorber incidence.
  • NIRSpec/IFU [O III] λ5007 flux, velocity, and dispersion maps: trace the 7-kpc ionized gas pool, assess rotation/dispersion, and check the spatially detached outflow candidate for position–velocity offsets.
  • Environment/neighbor map over NIRCam imaging with IFU/MSA footprints: locate the satellite galaxy and possible satellite/gas cloud, measure projected separations, and verify redshift/kinematic association.
  • BH–host comparison plot: place log(MBH)=7.65 against log(Mdyn)=9.1 relative to local scaling relations to visualize the BH-overmassive nature of this LRD.

Tags

  • LRD
  • overmassive BH
  • outflows
  • variability
  • spectroscopy

2506.17641v1

Dark Bondi Accretion Aided by Baryons and the Origin of JWST Little Red Dots

Wei-Xiang Feng, Hai-Bo Yu, Yi-Ming Zhong

Theme match 4/5

Digest

Proposes an SIDM-driven seeding pathway for JWST little red dots in which gravothermal core collapse, sped up by central baryons, makes a tiny seed that grows first via baryonic Eddington accretion and then rapidly through dark Bondi inflow of SIDM. Demonstrates that black holes can reach ~10^7 Msun within ~500 Myr after the formation of ~10^9 Msun halos at z≈4–11, with most of the final mass supplied by dark matter rather than gas. Fluid simulations with and without a Plummer-fit baryonic potential show that baryons substantially shorten the collapse timescale and establish conditions for efficient dark-sector Bondi growth. The framework naturally explains the overmassive BH-to-stellar ratios in LRDs and links them to SIDM cross sections consistent with galaxy-scale structure data.

Key figures to inspect

  • Figure 1: Compare the central-density evolution with (green/magenta) and without (blue) a compact Plummer baryonic potential to see how baryons accelerate gravothermal collapse; note the solid/dashed curves to gauge the dependence on the assumed self-interaction cross section.
  • Figure 2: Read off when the blue (dark Bondi) curve overtakes the orange (baryonic Eddington) contribution and how the red total track depends on the initial seed (solid vs dashed); this pinpoints the transition to DM-dominated growth in the LRD regime.
  • Figure 3: Use the density, Knudsen number, and SMFP-boundary markers to trace how the baryonic potential shifts the short–mean-free-path region and boosts central densities that feed Bondi inflow; the dash-dotted curve shows where stars/gas sit relative to the SIDM core.
  • Figure 4: Contrast with Fig. 3 to see how changing the SIDM cross section alters the SMFP core size, Knudsen evolution, and inner density slope, i.e., the sensitivity of dark Bondi fueling to particle physics parameters.

Tags

  • LRD
  • overmassive BH
  • BH seeds

2506.18112v1

Peering into the heart of darkness with VLBA : Radio Quiet AGN in the JWST North Ecliptic Pole Time-Domain Field

Payaswini Saikia, Ramon Wrzosek, Joseph Gelfand, Walter Brisken, William Cotton, S. P. Willner, Hansung B. Gim, Rogier A. Windhorst, Vicente Estrada-Carpenter, Ivan Yu. Katkov, Ingyin Zaw, Michael Rosenthal, Hanaan Shafi, Kenneth Kellermann, James Condon, Anton M. Koekemoer, Christopher J. Conselice, Rafael Ortiz, Christopher N. A. Willmer, Brenda Frye, Norman A. Grogin, Heidi B. Hammel, Seth H. Cohen, Rolf A. Jansen, Jake Summers, Jordan C. J. D'Silva, Simon P. Driver, Nor Pirzkal, Haojing Yan, Min S. Yun

Theme match 3/5

Digest

A 4.8 GHz VLBA snapshot survey of the JWST NEP Time-Domain Field targeted 106 VLA-selected radio sources and detected 12 compact emitters at 3.3 μJy rms and 4 mas resolution. The detections show pc-scale (<40 pc) structure with high VLBA/VLA flux ratios and Tb >10^5 K, and flatter spectra (α > −0.5) correlate with higher compactness—consistent with synchrotron from AGN coronae or low-power jets. Star formation contributes <50% of the VLBA flux in most cases, with several cores essentially AGN-driven; eight have JWST/NIRCam counterparts in predominantly early-type, bulge-dominated hosts, and WISE colors separate compact AGN/intermediate disks from extended SF galaxies. Comparing SCUBA-2 850 μm SFRs to new JWST-based estimates reveals discrepancies, underscoring JWST’s leverage to disentangle black-hole–driven radio cores from host-galaxy star formation.

Key figures to inspect

  • Figure 1: Use the point vs. Gaussian peak comparison to gauge source compactness; note PC 64 is resolved and PC 67 marginally so—key for distinguishing true pc-scale cores from slightly extended structures.
  • Figure 2: Inspect each 4.8 GHz VLBA panel for mas-scale morphology and elongation; confirm which sources are point-like versus resolved and relate this to the inferred emission mechanism (coronal vs. jet).
  • Figure 3: Cross-check the eight VLBA detections with JWST/NIRCam cutouts to see bulge-dominated hosts and the precise VLBA–NIR positional alignment within the VLA beam, informing counterpart reliability and host type.
  • Figure 4: Examine Legacy Survey RGB cutouts for PC 24, PC 41, and PC 64 to verify optical morphology and environment, complementing the NIR classifications and compactness seen with VLBA.

Tags

  • variability
  • radio
  • broad-line AGN

2506.14896v1

Overmassive Black holes live in compact galaxies in the early Universe

Yuxuan Wu, Tao Wang, Daizhong Liu, Qinghua Tan, Luis C. Ho, Zhiyu Zhang, Yong Shi, Ke Xu, Kotaro Kohno, Ran Wang, Takuma Izumi, Zhaozhou Li

Theme match 3/5

Digest

Uniform ALMA [CII] 158 μm size measurements for a curated sample of 22 z≈6 quasars show their hosts are systematically compact, with a median Re≈1.58 kpc versus 2.26 kpc for main-sequence SFGs measured in the same line. The hosts also have elevated MBH/M* and, for the most compact systems, reduced cold-gas content and sizes akin to massive quiescent galaxies at z≈4–5. Simple evolution over a gas-depletion timescale moves them toward the local MBH–M* relation as stellar mass builds. The compact, gas-poor subset likely marks the late stage of rapid BH growth and are prime progenitors of the first quiescent galaxies.

Key figures to inspect

  • Figure 1 (MBH–M*): Check how far individual quasars sit above constant MBH/M* tracks and identify objects with M* upper limits (grey arrows), confirming the prevalence of overmassive BHs in the sample.
  • Figure 2 (compactness comparisons): In the Re–M* plane, quantify the offset below the ALPINE SFG size relation; in the Σ*–MBH/M* panel, note the overlap with local galaxies hosting overmassive BHs and the position relative to the feedback-ineffective threshold line.
  • Figure 3 (evolution over tdep): Left panel arrows show predicted motion in MBH/M* after one depletion timescale—inspect which sources exhibit galaxy- versus BH-dominated growth and the overall drift toward the local relation. Right panel contrasts starburstiness and sizes with quiescent galaxies at z≈4–5; verify that…
  • Figure 4 (schematic pathway): Follow the proposed route from compact, overmassive-BH hosts to quiescence and compare the marked region for Little Red Dots to assess whether similarly compact, overmassive systems would track the same evolutionary path.

Tags

  • luminous quasar
  • overmassive BH
  • demographics

2506.13852v1

Overmassive black holes in the early Universe can be explained by gas-rich, dark matter-dominated galaxies

William McClymont, Sandro Tacchella, Xihan Ji, Rahul Kannan, Roberto Maiolino, Charlotte Simmonds, Aaron Smith, Ewald Puchwein, Enrico Garaldi, Mark Vogelsberger, Francesco D'Eugenio, Laura Keating, Xuejian Shen, Bartolomeo Trefoloni, Oliver Zier

Theme match 3/5

Digest

Using THESAN-ZOOM zoom-ins, the authors assign black-hole masses by assuming the M_BH–M_dyn relation is fundamental and then compare to JWST-selected AGN and JADES host properties at z>3. This simple prescription reproduces the observed distribution of “overmassive” black holes relative to local M_BH–M_* relations, with M_BH/M_* declining from ~0.1 at M_*≈10^6 Msun to ~0.01 at M_*≈10^10.5 Msun. The trend naturally follows the high dark-matter and gas fractions of low-mass galaxies—f_DM and f_gas decrease with M_* and show little evolution to z≈3—yielding small M_*/M_dyn and thus large apparent BH offsets; Prospector-inferred f_gas for 48,022 JADES galaxies (3<z<9) agrees with the simulations. A caveat is that BH growth and feedback are not modeled live, so full BH–galaxy co-evolution is not captured.

Key figures to inspect

  • Figure 1 (M_BH vs M_* assuming M_BH–M_dyn): Inspect the median track where M_BH/M_* falls from ~0.1 to ~0.01, the constant-ratio lines, and the overlay of JWST broad-line AGN and z>6 QSOs; note how the simulated distribution reproduces the observed overmassive regime and how the TNG50 overlay trends toward the local e…
  • Figure 2 (left; dark-matter fraction vs M_*): Check how f_DM decreases with stellar mass with only weak redshift dependence; compare to de Graaff et al. points and TNG50 trends to see how high f_DM at low M_* drives small M_*/M_dyn and thus large apparent M_BH/M_*.
  • Figure 2 (right; gas fraction vs M_*): Verify the declining f_gas with mass and the close agreement with JADES (Prospector-derived) medians; note the higher de Graaff values, the xGASS low-z reference, and the near-zero-f_gas outliers attributed to burst–quench ISM ejection; observe the minimal redshift evolution once…

Tags

  • overmassive BH
  • simulation
  • broad-line AGN

2506.13945v1

Euclid: The potential of slitless infrared spectroscopy: A z=5.4 quasar and new ultracool dwarfs

E. Bañados, V. Le Brun, S. Belladitta, I. Momcheva, D. Stern, J. Wolf, M. Ezziati, D. J. Mortlock, A. Humphrey, R. L. Smart, S. L. Casewell, A. Pérez-Garrido, B. Goldman, E. L. Martín, A. Mohandasan, C. Reylé, C. Dominguez-Tagle, Y. Copin, E. Lusso, Y. Matsuoka, K. McCarthy, F. Ricci, H. -W. Rix, H. J. A. Rottgering, J. -T. Schindler, J. R. Weaver, A. Allaoui, T. Bedrine, M. Castellano, P. -Y. Chabaud, G. Daste, F. Dufresne, J. Gracia-Carpio, M. Kümmel, M. Moresco, M. Scodeggio, C. Surace, D. Vibert, A. Balestra, A. Bonnefoi, A. Caillat, F. Cogato, A. Costille, S. Dusini, S. Ferriol, E. Franceschi, W. Gillard, K. Jahnke, D. Le Mignant, S. Ligori, E. Medinaceli, G. Morgante, F. Passalacqua, K. Paterson, S. Pires, C. Sirignano, I. T. Andika, H. Atek, D. Barrado, S. Bisogni, C. J. Conselice, R. Decarli, H. Dole, T. Dupuy, A. Feltre, S. Fotopoulou, B. Gillis, X. Lopez Lopez, M. Onoue, G. Rodighiero, N. Sedighi, F. Shankar, M. Siudek, L. Spinoglio, D. Vergani, G. Vietri, F. Walter, G. Zamorani, M. R. Zapatero Osorio, J. -Y. Zhang, M. Bethermin, N. Aghanim, B. Altieri, A. Amara, S. Andreon, C. Baccigalupi, M. Baldi, S. Bardelli, A. Basset, P. Battaglia, A. Biviano, A. Bonchi, D. Bonino, E. Branchini, M. Brescia, J. Brinchmann, S. Camera, V. Capobianco, C. Carbone, J. Carretero, S. Casas, G. Castignani, S. Cavuoti, A. Cimatti, C. Colodro-Conde, G. Congedo, L. Conversi, F. Courbin, H. M. Courtois, M. Cropper, J. -G. Cuby, A. Da Silva, H. Degaudenzi, G. De Lucia, A. M. Di Giorgio, C. Dolding, F. Dubath, C. A. J. Duncan, X. Dupac, A. Ealet, M. Farina, F. Faustini, N. Fourmanoit, M. Frailis, S. Galeotta, K. George, C. Giocoli, B. R. Granett, A. Grazian, F. Grupp, L. Guzzo, S. V. H. Haugan, J. Hoar, H. Hoekstra, W. Holmes, I. Hook, F. Hormuth, A. Hornstrup, P. Hudelot, M. Jhabvala, B. Joachimi, E. Keihänen, S. Kermiche, B. Kubik, K. Kuijken, M. Kunz, H. Kurki-Suonio, P. B. Lilje, V. Lindholm, I. Lloro, G. Mainetti, D. Maino, E. Maiorano, O. Mansutti, O. Marggraf, K. Markovic, M. Martinelli, N. Martinet, F. Marulli, R. Massey, S. Mei, Y. Mellier, M. Meneghetti, E. Merlin, G. Meylan, A. Mora, L. Moscardini, C. Neissner, S. -M. Niemi, J. W. Nightingale, C. Padilla, S. Paltani, F. Pasian, K. Pedersen, W. J. Percival, V. Pettorino, G. Polenta, M. Poncet, L. A. Popa, L. Pozzetti, F. Raison, R. Rebolo, A. Renzi, J. Rhodes, G. Riccio, E. Romelli, M. Roncarelli, E. Rossetti, R. Saglia, Z. Sakr, D. Sapone, B. Sartoris, J. A. Schewtschenko, M. Schirmer, P. Schneider, T. Schrabback, A. Secroun, E. Sefusatti, G. Seidel, M. Seiffert, S. Serrano, G. Sirri, L. Stanco, J. Steinwagner, P. Tallada-Crespí, A. N. Taylor, H. I. Teplitz, I. Tereno, S. Toft, R. Toledo-Moreo, F. Torradeflot, I. Tutusaus, L. Valenziano, J. Valiviita, T. Vassallo, G. Verdoes Kleijn, A. Veropalumbo, Y. Wang, J. Weller, F. M. Zerbi, E. Zucca, M. Bolzonella, C. Burigana, R. Cabanac, L. Gabarra, V. Scottez, M. Viel, H. Dannerbauer, D. Scott

Theme match 2/5

Digest

Euclid NISP slitless spectra demonstrate blind, space-based identification of both high‑z quasars and their chief photometric contaminants, ultracool dwarfs. The team reports a bright z=5.404 quasar, EUCL J181530.01+652054.0, flagged by strong broad CIII] and MgII in RGE (1206–1892 nm) with CIV/CIII] also in BGE (926–1366 nm) and confirmed by LBT optical data. It is a high‑excitation BAL quasar detected by LOFAR at 144 MHz (L144≈4×10^25 W/Hz), with Lbol≈3×10^12 Lsun and MBH≈3.4×10^9 Msun—an unexpectedly luminous find within only ~20 deg2. Cross-correlation of NISP spectra likewise yields new ultracool dwarfs (e.g., T3 EUCL J002516.31+491618.5; M6 EUCL J174429.80+672728.1), underscoring RGE’s ability to uncover bright quasars at z~5.5 and z>7 where photometric selection struggles.

Key figures to inspect

  • Figure 1: Use the line–redshift map to see where ≥2 strong lines fall in the NISP bandpasses—highlighting the z~5.5 and z>7 windows for reliable blind redshifts and the space-based advantage over telluric gaps.
  • Figure 2: Inspect quasar vs M/L/T-dwarf colors and the marked objects (EUCL J181530.01+652054.0, EUCL J002516.31+491618.5, EUCL J174429.80+672728.1) to appreciate why photometry alone is degenerate and why spectroscopy is decisive.
  • Figure 3: Check the T3 dwarf EUCL J002516.31+491618.5 postage stamps and RGE spectrum; the template match shows how cross-correlation cleanly identifies ultracool dwarfs in slitless data.
  • Figure 4: Compare the M6 dwarf EUCL J174429.80+672728.1 NISP spectrum with the LBT/MODS optical confirmation and note the LOFAR upper limit—validating the Euclid spectral classification pipeline.

Tags

  • luminous quasar
  • demographics
  • spectroscopy