Bursting at the seams: the star-forming main sequence and its scatter at z=3-9 using NIRCam photometry from JADES

Monthly Notices of the Royal Astronomical Society Oxford University Press (OUP) (2025) staf1950

Authors:

C Simmonds, S Tacchella, W McClymont E Curtis-Lake, F D’Eugenio, K Hainline, BD Johnson, A Kravtsov, D Puskás, B Robertson, A Stoffers, C Willott, WM Baker, VA Belokurov, R Bhatawdekar, AJ Bunker, S Carniani, J Chevallard, M Curti, Q Duan, JM Helton, Z Ji, TJ Looser, R Maiolino, MV Maseda, I Shivaei, CC Williams

Abstract:

Abstract We present a comprehensive study of the star-forming main sequence (SFMS) and its scatter at redshifts 3 ≤ z ≤ 9, using NIRCam photometry from the JADES survey in the GOODS-S and GOODS-N fields. Our analysis is based on a sample of galaxies that is stellar mass complete down to log (M⋆/M⊙) ≈ 8.1. The redshift evolution of the SFMS at an averaging timescale of 10 Myr follows a relation, quantified by the specific star-formation rates (sSFR10), of sSFR∝(1 + z)μ with $\mu = 2.30^{+0.03}_{-0.01}$, in good agreement with theoretical predictions and the specific mass accretion rate of dark matter halos. We find that the SFMS normalisation varies in a complex way with the SFR averaging timescale, reflecting the combined effects of bursty star formation and rising star formation histories (SFHs). We quantify the scatter of the SFMS, revealing that it decreases with longer SFR averaging timescales, from σint ≈ 0.4 − 0.5dex at 10 Myr to σint ≈ 0.2dex at 100 Myr, indicating that shorter-term fluctuations dominate the scatter, although long-term variations in star formation activity are also present. Our findings suggest that bursty SFHs are more pronounced at lower stellar masses. Furthermore, we explore the implications of our results for the observed over-abundance of UV-bright galaxies at z > 10, concluding that additional mechanisms, such as top-heavy initial mass functions, increased star-formation efficiencies, or increased burstiness in star formation are needed to explain these observations. Finally, we emphasize the importance of accurate stellar mass completeness limits when fitting the SFMS, especially for galaxies with bursty SFHs.

Excitation of Molecular Hydrogen in Seyferts: NGC 5506 and NGC 3081

The Astrophysical Journal American Astronomical Society 993:2 (2025) 217

Authors:

Daniel E Delaney, Erin KS Hicks, Lulu Zhang, Chris Packham, Ric Davies, Miguel Pereira Santaella, Enrica Bellocchi, Nancy A Levenson, Steph Campbell, David J Rosario, Houda Haidar, Cristina Ramos Almeida, Anelise Audibert, Claudio Ricci, Laura Hermosa Muñoz, Francoise Combes, Almudena Alonso-Herrero, Santiago García-Burillo, Federico Esposito, Ismael García-Bernete, Taro Shimizu, Martin Ward, Omaira Gonzalez Martin, Alvaro Labiano, Dimitra Rigopoulou

Abstract:

We utilize James Webb Space Telescope (JWST) Mid Infrared Instrument (MIRI) integral field unit observations to investigate the behavior and excitation of H2 in the nearby Seyfert galaxies NGC 3081 and NGC 5506, both part of the Galactic Activity, Torus, and Outflow Survey (or GATOS). We compare population levels of the S(1) to S(8) rotational H2 emission lines visible to JWST/MIRI spectroscopy to models assuming local thermodynamic equilibrium (LTE), in order to estimate the column density and thermal scaling of the molecular gas. For the nuclear regions, we incorporate Very Large Telescope Spectrograph for INtegral Field Observations in the Near Infrared (or VLT/SINFONI) K-band observations to estimate population levels for available rovibrational H2 emission lines, and compare the resultant population curves to non-LTE radiative transfer models and shock modeling. We report a differing set of prominent active galactic nuclei (AGN)-driven excitation mechanisms between the two galaxies. For NGC 3081, we find that a non-LTE radiative transfer environment is adequate to explain observations of the nuclear region, indicating that the primary mode in which the AGN transfers excitation energy is likely irradiation. We estimate the extent of AGN photoionization along the ionization bicone to be ≈330 pc. In contrast, for NGC 5506, we find a shock scenario to be a more plausible excitation mechanism, a conclusion bolstered by an observed spatial correlation between higher-energy rotational H2 and [Fe II]5.34μm emission. In addition, we identify potential nuclear H2 outflows resulting from an interaction between the ionization bicone and the rotational disk. By isolating the outflowing component of the H2 emission, we estimate the warm molecular mass outflow rate to be 0.07 M⊙ yr−1.

Creating halos with autoregressive multistage networks

Physical Review D American Physical Society (APS) 112:10 (2025) 103503

Authors:

Shivam Pandey, Chirag Modi, Benjamin D Wandelt, Deaglan J Bartlett, Adrian E Bayer, Greg L Bryan, Matthew Ho, Guilhem Lavaux, T Lucas Makinen, Francisco Villaescusa-Navarro

The GECKOS Survey: revealing the formation history of a barred galaxy via structural decomposition and resolved spectroscopy

(2025)

Authors:

A Fraser-McKelvie, DA Gadotti, F Fragkoudi, C de Sá-Freitas, M Martig, M Bureau, T Davis, R Elliott, E Emsellem, D Fisher, MR Hayden, J van de Sande, AB Watts

Warped Disk Galaxies. II. From the Cosmic Web to the Galactic Warp

The Astrophysical Journal American Astronomical Society 993:2 (2025) 205

Authors:

Woong-Bae G Zee, S Lyla Jung, Sanjaya Paudel, Suk-Jin Yoon

Abstract:

Galactic warps are common in disk galaxies. While often attributed to galaxy–galaxy tides, a nonspherical dark matter halo has also been proposed as a driver of disk warping. We investigate links among warp morphology, satellite distribution, and large-scale structure using the Sloan Digital Sky Survey catalog of warped disks compiled by W.-B. G. Zee et al. Warps are classified into 244 S- and 127 U-types, hosting 1373 and 740 satellites, respectively, and are compared to an unwarped control matched in stellar mass, redshift, and local density. As an indirect, population-level proxy for the host halo’s shape and orientation, we analyze the stacked spatial distribution of satellites. Warped hosts show a significant anisotropy: an excess at 45° < ϕ < 90° (measured from the host major axis), peaking at P(ϕ) ≃ 0.003, versus nearly isotropic controls. Satellites of S-type warps preferentially align with the nearest cosmic filament, whereas those of U-type warps are more often perpendicular. The incidence of warps increases toward filaments (rfila < 4 Mpc h−1), while the number of satellites around warped hosts remains approximately constant with filament distance, indicating a direct influence of the large-scale environment. We discuss possible links between galactic warps and the cosmic web, including anisotropic tidal fields and differences in evolutionary stage.