On 31 August 2026, a University of Tokyo / Kavli IPMU team led by graduate student Takumi Tanaka, with John Silverman and dozens of COSMOS collaborators, reported four dual Little Red Dot (LRD) systems in JWST’s COSMOS-Web field — compact, extremely red objects thought to host rapidly growing black holes when the universe was only about a billion years old. The paper, Hidden in Pixels. I., went live in Publications of the Astronomical Society of Japan (DOI 10.1093/pasj/psag092); the Kavli IPMU release pegs the lookback at ~12.5–12.8 billion years.

Two of the four pairs have COSMOS-3D slitless spectroscopy: matching single lines (assumed Hα) put them at z = 5.822 and z = 5.464, with projected separations 1.64 kpc and 7.36 kpc. Across the sample, the LRD angular auto-correlation shows roughly a 20–30× excess on sub-arcsecond (kilo-parsec) scales versus an extrapolation of the power-law clustering of JWST-found AGNs measured on 10″–100″ scales. These are precursor dual LRDs / merger candidates — not confirmed black-hole mergers already completed, and not all four pairs are spectroscopically locked.

Why it matters

Every big galaxy today has a supermassive black hole. Nobody fully knows how those holes got huge so fast in the first billion years. JWST’s Little Red Dots are one of the leading clues: tiny, red, often showing broad Balmer lines, abundant enough that their number density sits well above a simple extrapolation from luminous quasars.

Mergers are a standard growth channel on paper — gas inflows, dual active nuclei, later gravitational waves — but until this work, nobody had a clean sample of two LRDs sitting on top of each other. Conventional LRD searches used aperture color plus compactness cuts that can glue a close pair into one “dot” or throw the system out. Tanaka’s group flipped the method: color every pixel, relax compactness, and hunt for red cores that are actually twins.

For a stranger, the stake is visual and simple. Four pairs of infant-universe black-hole engines, some already confirmed at the same redshift, sitting thousands of light-years apart — a collision course you can point at on a JWST cutout. If the pairs really merge later, future space gravitational-wave observatories such as LISA could hear the echoes.

Key numbers

MetricValueNotes
Dual LRD candidate pairs4COSMOS-Web; pixel-by-pixel color selection
Lookback age (IPMU release)~12.5–12.8 billion yearsEarly-universe window
Spectroscopic redshifts (2 pairs)z = 5.822, z = 5.464Matching single lines; assumed Hα
Projected separations (those 2)1.64 kpc, 7.36 kpcPhysical, not comoving
Angular separations (all 4)0.2″–1.2″Few thousand to tens of thousands of ly
Clustering excess on kpc scales~20–30×vs extrapolated JWST AGN ACF (10″–100″)
Parent cleaned LRD sampleN = 829Pixel method; ~2× Akins et al. aperture sample
Chance of 4 pairs ≤1.2″ at random~7×10⁻⁵ (~3.8σ)Monte Carlo in COSMOS-Web-like field
Journal / datePASJ, 31 Aug 2026DOI 10.1093/pasj/psag092
LeadTakumi S. Tanaka (UTokyo / Kavli IPMU)Silverman et al.

Pair separations run from a few thousand to a few tens of thousands of light-years — far smaller than the Milky Way’s ~100,000-light-year disk. That is close, in galaxy terms.

How they found them

COSMOS-Web covers 0.54 deg² with NIRCam (and a MIRI subset). Instead of one color per aperture, the team built S/N and (m_F277W − m_F444W) maps, kept contiguous patches of ≥10 pixels with per-pixel S/N > 1 and color > 1.5, then cleaned artifacts with DINOv2 + UMAP + DBSCAN and visual inspection. Four systems survived where both neighbors independently meet LRD color criteria inside a 3″ cutout.

Image modeling with galight favored compact PSF-like components. Brown-dwarf templates fit worse than LRD SED models. Two systems — CW-B2-4383 and CW-A4-16093 — fall inside COSMOS-3D F444W grism coverage. Each shows a line at the same observed wavelength in both components. Alternative line IDs (C IV, Mg II, Hβ, Paschen) clash with photometry or missing [O III]; Hα at z = 5.822 and 5.464 fits. Brighter components show broad-line evidence (FWHM ~1800–2100 km s⁻¹ in double-Gaussian fits); fainter components are noisier — a broad line may simply be undetected.

Velocity offsets between the spectroscopically confirmed members are tiny (Δv ≈ 13 and 47 km s⁻¹), well below estimated escape speeds from ~10¹¹–10¹¹·⁵ M_⊙ halos at these separations. Fly-bys are unlikely; the pairs sit deep inside a shared halo’s virial radius.

Black-hole mass estimates still disagree by method: single-epoch broad Hα gives roughly 10⁷ M_⊙; BH-envelope blackbody fits assuming near-Eddington radiation give closer to 10⁵·³–10⁶·³ M_⊙. Either way, the paper argues early mergers in the 10⁵–10⁷ M_⊙ range are on the table.

What this is not

  • Not confirmed mergers. The authors call the sample “likely to represent precursors of mergers between LRDs.”
  • Not four spectroscopically confirmed pairs. Two have matching-line support; two remain photometric (system z_photo ~6.4).
  • Not proof every LRD is a black hole in the same way. The field still debates envelopes, stellar contributions, and selection. The paper’s working frame is rapidly accreting early SMBHs.
  • Not Roman Space Telescope news. Different mission, different story already on this site.

What to watch

  1. Deeper NIRSpec IFU on all four systems — especially the two photometric pairs and the off-centered extended fluff around CW-B5-15958.
  2. The same pixel method on more JWST treasury fields. CEERS, JADES, and PRIMER-UDS turned up no duals yet; their combined area is still several times smaller than COSMOS-Web, so the null is not a contradiction.
  3. A proper dual fraction with completeness corrections (raw four / 829 ≈ 0.5% is only a starting sketch).
  4. Whether kilo-parsec LRD clustering stays special once large WFSS programs build matched galaxy and AGN control samples — and whether LISA-era forecasts can use dual-LRD rates as a prior on early SMBH merger rates.

Four red twins in the infant universe, two already locked at the same redshift, clustering far above chance: that is the progress signal. The mergers themselves are still in the future — of the cosmos, and of the observing queue.

Sources