On the Kinematic Nature of Apparent Disks at High Redshifts: Local Counterparts are Not Dominated by Ordered Rotation but by Tangentially Anisotropic Random Motion

The Astrophysical Journal Letters American Astronomical Society 973:1 (2024) L29

Authors:

Bitao Wang, Yingjie Peng, Michele Cappellari, Hua Gao, Houjun Mo

Abstract:

It is not straightforward to physically interpret the apparent morphology of galaxies. Recent observations by the James Webb Space Telescope (JWST) revealed a dominant galaxy population at high redshifts (z > 2) that were visually classified as disks for their flattened shapes and/or exponential light profiles. The extensively accepted interpretation is that they are dynamically cold disks supported by bulk rotation. However, it is long known that flattened shapes and exponential profiles are not exclusive for rotating disk structure. To break degeneracy and assess the rotational support of typical high-z galaxies in the JWST samples, those with active star formation and stellar masses lg(M⋆/M⊙)∼9 , we study the kinematics of their equal-mass counterparts at z = 0. While these local star-forming low-mass galaxies are photometrically similar to real dynamically cold disks, they are not supported by ordered rotation but primarily by random motion, and their flattened shapes result largely from tangential orbital anisotropy. Given the empirical and theoretical evidence that young galaxies are dynamically hotter at higher redshifts, our results suggest that the high-z JWST galaxies may not be cold disks but are dynamically warm/hot galaxies with flattened shapes driven by anisotropy. While both have low rotational support, local low-mass galaxies possess oblate shapes, contrasting the prolate shapes (i.e., cigar like) of low-mass systems at high redshifts. Such shape transition (prolate ⇒ oblate) indicates an associated change in orbital anisotropy (radial ⇒ tangential), with roots likely in the assembly of their host dark matter halos.

Spatially Resolved Kinematics of SLACS Lens Galaxies. I: Data and Kinematic Classification

(2024)

Authors:

Shawn Knabel, Tommaso Treu, Michele Cappellari, Anowar J Shajib, Chih-Fan Chen, Simon Birrer, Vardha N Bennert

The ALMA-CRISTAL survey

Astronomy & Astrophysics EDP Sciences 689 (2024) a145

Authors:

M Solimano, J González-López, M Aravena, R Herrera-Camus, I De Looze, NM Förster Schreiber, J Spilker, K Tadaki, RJ Assef, L Barcos-Muñoz, RL Davies, T Díaz-Santos, A Ferrara, DB Fisher, L Guaita, R Ikeda, EJ Johnston, D Lutz, I Mitsuhashi, C Moya-Sierralta, M Relaño, T Naab, AC Posses, K Telikova, H Übler, S van der Giessen, S Veilleux, V Villanueva

HARMONI at ELT: towards final designs and AIT strategies for SCAOS sub-system in NGSS

Proceedings of SPIE--the International Society for Optical Engineering SPIE, the international society for optics and photonics 13097 (2024) 1309755-1309755-19

Authors:

J-F Sauvage, Z Challita, E Renault, W Bon, A Bozier, K Dohlen, A Bonnefoi, B Foulon, C Bond, M Noirel, B Aqua, J Floriot, D Le Mignant, A Costille, T Fusco, B Neichel, N Thatte, F Clarke, P-Y Madec, J Paufique

MOSAIC GLAO performance and system architecture: AO for the entire ELT focal plane

Proceedings of SPIE Society of Photo-optical Instrumentation Engineers 13097 (2024) 4Z-5

Authors:

Nazim Ali Bharmal, Timothy Morris, Gavin Dalton

Abstract:

MOSAIC is a wide-field spectrograph, combining multiple-object spectroscopy and integral field units, to cover the ELT focal plane with a field-of-view of 7.8 arcmin from the blue to the near-infrared, 390 to 1800nm. In the current Phase B design, AO is GLAO supported by four LGS in a fixed asterism and with multiple NGS. Although the GLAO correction is modest compared to other ELT instrumentation, the use of the integrated M4/M5 correction elements and the existing LGS allows for an efficient design which is outlined. MOSAIC GLAO will use the ELT PFS guide-probes to compensate for high- frequency tip/tilt errors, greatly relaxing the requirements on the instrumental NGS sensors. The Phase A architecture used the same pick-off mirrors as the IFU instruments to feed the NGS-WFS from anywhere in the focal plane, which was mandatory for the proposed MOAO design. The reduced performance requirements at Phase B allows us to take advantage, instead, of the four 2 arcmin diameter field-of-view through the LGS cutouts, arranged in a square pattern at an off-axis distance of 3.75 arcmin. In each LGS cutout, a wide-field-imager is implemented–alongside one LGS WFS–to acquire multiple NGS that supports both slow tip/tilt measurements, isolating instrument-Nasmyth flexure, solving for the astrometric distortion expected from errors in the ELT optical path, and supporting the alignment of MOS apertures with the field. The latter is a key requirement for MOSAIC, leading to 40mas accuracy in MOS aperture positioning and 40mas rotation displacement at the edge of the scientific field.