Weekly issue

Week 11, 2026

Mar 9–15, 2026

Week 11, 2026 includes 3 curated papers, centered on LRD, QSO, v-shaped SED.

2603.13736v1

Blackbody Quasar and Radio Source (BBQSORS): A Candidate of Transitional Little Red Dots with a $T\sim10^4\ K$ Blackbody Spectrum

Yuxing Zhong, Xiaoyang Chen, Kohei Ichikawa, Youwen Kong, Kentaro Aoki, Satoshi Yamada, Tohru Nagao, Daisaburo Kido, Toshihiro Kawaguchi, Yoshiki Matsuoka, Toru Misawa, Shoichiro Mizukoshi, Masafusa Onoue, Ayumi Takahashi, Yoshiki Toba

Theme match 5/5

Digest

Subaru/PFS follow-up of a radio-loud, X-ray–detected UNVEIL source at z=1.715 (BBQSORS) reveals a broad Mg II line (FWHM ≳ 4000 km s−1) with narrow absorbers and a strongly curved, Λ-shaped UV continuum across 1500–3500 Å. The continuum is incompatible with simple dust reddening and is well matched by a T≈10^4 K blackbody; UV–MIR photometry is consistently fit by three blackbodies at ≈9700, 1500, and 80 K. A marginal GALEX NUV detection suggests a V-shaped SED break near 1400 Å—bluer than the 3000–4000 Å breaks seen in canonical LRDs—implying a hotter, thinning envelope around the SMBH. Together with the emerging X-ray and radio emission, the data point to a transitional LRD-to-quasar phase as the cocoon fragments and the nucleus becomes exposed.

Key figures to inspect

  • Figure 1: Use the HSC+Spitzer cutouts with VLASS 3 GHz contours to confirm the radio core’s association with BBQSORS and look for a close companion/merger; in the PFS spectrum panels, inspect the Λ-shaped continuum and quantify the Mg II width, the narrow absorber that dips to the continuum, and accompanying Al III ab…
  • Figure 2: Check the EPIC/pn 0.4–7.2 keV (rest 1–20 keV) detection and the ≈3.4σ significance; compare the best-fit spectral model and residuals to assess whether emerging hard X-rays are consistent with a dispersing envelope rather than heavy, Compton-thick obscuration.
  • Figure 3: Examine the UV–MIR SED decomposition—blackbodies at ≈9700 K (envelope), ≈1500 K (torus), and ≈80 K (host dust)—and locate the V-shaped break near 1400 Å; contrast with the plotted LRD-like ≈5000 K component to see how a hotter envelope shifts the turnover.
  • Figure 4: Compare BBQSORS to blue and dust-reddened quasar templates after de-reddening the PFS spectrum; note the persistent blue-end mismatch (<~2200 Å) arguing against dust-only explanations, and use the PFS vs SDSS/DESI overlay to gauge spectral-shape stability across epochs/instruments.

Tags

  • LRD
  • v-shaped SED
  • spectroscopy
  • radio
  • variability

2603.10162v1

The X-ray weakness of Little Red Dots and JWST-selected AGN: comparison with local AGN in different accretion regimes

A. Tortosa, C. Ricci, P. Du, G. Venturi, L. C. Ho, R. Li, J. -M. Wang, M. Berton

Theme match 5/5

Digest

Compares z≳4 little red dots and JWST-selected broad-line AGN to local SEAMBHs, NLS1s, and type I AGN using L2–10 keV, broad Hα, λEdd, Lbol, and κbol,X. Finds an anti-correlation between L2–10 keV/LHα and λEdd in the local high-λEdd subsample (slim-disc–like), while most high‑z objects fall below the SEAMBH locus, implying more extreme accretion, intrinsically weak/cool coronae, or heavy obscuration. SEAMBHs show Hα‑based Lbol underestimates SED‑based values, and SEAMBHs/LRDs/JWST-AGN share a high‑κbol,X regime indicating a relative X‑ray deficit. Caveat: many high‑z X‑ray points are upper limits and may miss heavy or Compton‑thick absorption, with sensitivity and steep spectra further suppressing detections.

Key figures to inspect

  • L2–10 keV/LHα vs λEdd plane comparing SEAMBHs (baseline) with LRDs and JWST BL AGN—check how far high‑z sources sit below the SEAMBH locus and the strength/slope of the anti‑correlation for high‑λEdd objects.
  • L2–10 keV vs LHα relation with censored points (upper limits) for high‑z sources—quantify the offset from standard local trends and how survival-analysis treatment changes the inference.
  • κbol,X distributions (or κbol,X vs λEdd) across SEAMBHs, LRDs, and JWST BL AGN—verify the common high‑κbol,X regime that signals X‑ray deficit relative to bolometric output.
  • SED‑based Lbol versus Hα‑based Lbol for SEAMBHs (with dust correction flagged)—measure the systematic underestimation when using Hα and its impact on placing high‑z analogs.
  • Sample overview panel (SEAMBHs, NLS1s, BASS/SDSS type I, LRDs/JWST BL AGN)—inspect λEdd and redshift distributions to assess comparability and selection-driven biases.

Tags

  • LRD
  • broad-line AGN
  • variability

2603.11747v1

Merger-driven buildup of the $M_{\rm BH}$ - $M_*$ relation bridging high-$z$ overmassive black holes with the local relation

Takumi S. Tanaka, John D. Silverman, Kazuhiro Shimasaku, Knud Jahnke, Junyao Li, Makoto Ando

Theme match 4/5

Digest

Monte Carlo merger-only experiments evolve the MBH–M* plane from z≈6 to 0 using observed high‑z scatter and redshift‑dependent merger rates. The models reproduce the local dispersion (~0.3 dex) even when initialized with σ=0.8–1.0 dex at z≈6, and they show that the decline of scatter is highly sensitive to the mass‑ratio distribution and overall merger frequency, with frequent minor mergers also accelerating convergence. This provides a non‑causal “averaging” bridge between JWST reports of overmassive SMBHs and the local relation. The authors highlight that measuring the M*‑dependence of σ and securing σ at z≈3–4 will be decisive tests.

Key figures to inspect

  • Evolution of σ(z) for different merger‑rate prescriptions and mass‑ratio cuts; verify that tracks starting at σ=0.8/1.0 converge to ~0.3 by z≈0 and how minor‑merger–dominated histories differ from major‑only cases.
  • MBH–M* distributions at z≈6, z≈3–4, and z≈0 (scatter contours/residuals); inspect how the high‑σ initial population tightens and whether an overmassive tail persists at intermediate redshift.
  • Predicted σ versus M* (mass‑dependent scatter) at z≈3–4; identify the mass bins where deviations are largest to target with upcoming surveys.
  • Cumulative number of mergers per galaxy versus redshift, split into major and minor; assess the central‑limit averaging behavior and quantify the relative contribution of minor mergers.
  • Sensitivity test comparing alternative galaxy‑replenishment strategies or merger‑rate parameterizations; check robustness of σ(z) convergence against these choices.

Tags

  • overmassive BH
  • BH seeds
  • simulation