TDCOSMO XXIX: JWST/NIRSpec IFU Spatially Resolved Kinematics of Three Time-delay Lenses

(2026)

Authors:

Shawn Knabel, Pritom Mozumdar, Anowar J Shajib, Tommaso Treu, Devon M Williams, Michele Cappellari, David Law, Simon Birrer, Takahiro Morishita, William Sheu, Massimo Stiavelli

Stellar discs and intermediate-mass black holes in galactic nuclei – I. Fragmenting the disc in an isotropic stellar potential

Monthly Notices of the Royal Astronomical Society Oxford University Press (OUP) (2026) stag1637

Authors:

Taras Panamarev, Xiang Zou, Bence Kocsis

Abstract:

Abstract The origin of the complex orbital structure of young massive stars at the Galactic centre remains an open question. If these stars formed in a single episode from a gaseous accretion disc, they may initially have constituted a single, coherently rotating stellar disc. We investigate whether perturbations from an unseen intermediate-mass black hole (IMBH) could fragment and/or disrupt such a disc into the multiple orbital components observed today. First, we derive a theoretical criterion for when and where the IMBH’s torque overcomes the disc’s self-torque and tears it apart. We then test this picture with direct N-body simulations of a stellar disc interacting with an inclined IMBH around a central supermassive black hole. We find that the outcome depends strongly on the IMBH’s orbit and mass. A prograde IMBH rapidly aligns with the stellar disc, while a massive retrograde IMBH (m• ≃ 0.67 Md) anti-aligns relative to the radially overlapping stars and efficiently fragments the original disc into three components in angular-momentum space: an inner disc, a misaligned overlapping region, and an unperturbed outer disc. The IMBH also excites eccentricities in the overlapping region, driving stars away from initially circular orbits. These features emerge for an IMBH mass of 2000 ⊙ and a disc mass of 3000 ⊙ within 10–20 Myr, a timescale comparable to the age of the young Galactic centre stellar population, and provide a plausible explanation for the observed multiple orbital planes, warped geometry, and broad eccentricity distribution.

TDCOSMO XXVIII. The Hubble constant from the quadruply lensed quasar J1537$-$3010 with precise time delays

(2026)

Authors:

A Galan, AG Schweinfurth, SH Suyu, DP Johnson, A Chawla, D Sluse, GV Kharchilava, E Buckley-Geer, H Lin, S Knabel, W Sheu, S Ertl, T Anguita, S Birrer, F Courbin, F Dux, M Millon, V Motta, S Schuldt, T Treu, DM Williams, M Cappellari, KC Wong, D Eckert

TDCOSMO. XXVII. JWST-based Lens Models and H$_0$ Measurement of WFI2033, HE0435, and PG1115

(2026)

Authors:

DM Williams, T Treu, DP Johnson, P Mozumdar, S Knabel, S Birrer, CD Fassnacht, A Galan, AJ Shajib, KC Wong, M Cappellari, F Courbin, T Morishita, V Motta, D Sluse, M Stiavelli

BEACON: JWST NIRCam Pure-parallel Imaging Survey. IV. A Systematic Search for Galaxy Overdensities and Evidence for Gas Accretion Mode Transition

The Astrophysical Journal 1007:2 (2026)

Authors:

Ryo Albert Sutanto, Takahiro Morishita, Tadayuki Kodama, Abdurro’uf, Larry D Bradley, Andrew J Bunker, Nima Chartab, Nuo Chen, Matthew J Hayes, George Helou, Novan Saputra Haryana, Nicha Leethochawalit, Zhaoran Liu, Charlotte A Mason, Marc Rafelski, Michael J Rutkowski, Massimo Stiavelli, Kosuke Takahashi, Harry I Teplitz, Michele Trenti, Tommaso Treu, Benedetta Vulcani, Yechi Zhang

Abstract:

We systematically search for galaxy overdensities using 20 independent fields with a minimum of six filters (F090W, F115W, F150W, F277W, F356W, and F444W) from BEACON, the JWST Cycle 2 NIRCam pure-parallel imaging survey. We apply an adaptive kernel-density estimation method that incorporates the full photometric redshift probability distribution function of each galaxy to map galaxy overdensities, and identify 207 significant (>4σ) overdensities at 1.5 < z < 5. We measure the quenched galaxy fraction, the average specific star formation rate (sSFR), the total dark matter mass, and the local galaxy density of each system. By investigating the correlation among these observables, we find that galaxy quenching proceeds in two paths. (i) Overdensities within more massive halos exhibit higher quenched fractions and lower averaged sSFRs. This trend weakens at z ≳ 2, consistent with cold gas streams penetrating shock-heated massive halos and sustaining star formation activity at early times. (ii) We also find a dependence of the same parameters on local densities at z < 2, where the quenched fraction increases and the sSFR decreases toward higher densities. The environmental trend in sSFR weakens at z ∼ 2–3 and shows tentative evidence for a reversal at z > 3, potentially due to a larger cold gas supply in earlier times. Our study reveals a complex interplay between individual galaxies and large-scale environmental properties, marking the onset of environmental effects on galaxy quenching in massive halos at cosmic noon.