An outflow powers the optical rise of the nearby, fast-evolving tidal disruption event AT2019qiz

Monthly Notices of the Royal Astronomical Society Oxford University Press (OUP) 499:1 (2020) 482-504

Authors:

M Nicholl, T Wevers, SR Oates, KD Alexander, G Leloudas, F Onori, A Jerkstrand, S Gomez, S Campana, I Arcavi, P Charalampopoulos, M Gromadzki, N Ihanec, PG Jonker, A Lawrence, I Mandel, S Schulze, P Short, J Burke, C McCully, D Hiramatsu, DA Howell, C Pellegrino, H Abbot, JP Anderson, E Berger, PK Blanchard, G Cannizzaro, T-W Chen, M Dennefeld, L Galbany, S González-Gaitán, G Hosseinzadeh, C Inserra, I Irani, P Kuin, T Müller-Bravo, J Pineda, NP Ross, R Roy, SJ Smartt, KW Smith, B Tucker, Ł Wyrzykowski, DR Young

Modelling burning thermonuclear plasma

Philosophical Transactions A: Mathematical, Physical and Engineering Sciences Royal Society 378:2184 (2020) 20200014

Authors:

Steven J Rose, Peter Hatfield, Robbie HH Scott

Abstract:

Considerable progress towards the achievement of thermonuclear burn using inertial confinement fusion has been achieved at the National Ignition Facility in the USA in the last few years. Other drivers, such as the Z-machine at Sandia, are also making progress towards this goal. A burning thermonuclear plasma would provide a unique and extreme plasma environment; in this paper we discuss (a) different theoretical challenges involved in modelling burning plasmas not currently considered, (b) the use of novel machine learning-based methods that might help large facilities reach ignition, and (c) the connections that a burning plasma might have to fundamental physics, including quantum electrodynamics studies, and the replication and exploration of conditions that last occurred in the first few minutes after the Big Bang.

The infrared-radio correlation of star-forming galaxies is strongly M$_{\star}$-dependent but nearly redshift-invariant since z$\sim$4

ArXiv 2010.0551 (2020)

Authors:

I Delvecchio, E Daddi, MT Sargent, MJ Jarvis, D Elbaz, S Jin, D Liu, IH Whittam, H Algera, R Carraro, C D'Eugenio, J Delhaize, BS Kalita, S Leslie, D Cs Molnar, M Novak, I Prandoni, V Smolcic, Y Ao, M Aravena, F Bournaud, JD Collier, SM Randriamampandry, Z Randriamanakoto, G Rodighiero, J Schober, SV White, G Zamorani

Discovery of optical outflows and inflows in the black hole candidate GRS 1716−249

Monthly Notices of the Royal Astronomical Society Oxford University Press (OUP) 498:1 (2020) 25-32

Authors:

VA Cúneo, T Muñoz-Darias, J Sánchez-Sierras, F Jiménez-Ibarra, M Armas Padilla, DAH Buckley, J Casares, P Charles, JM Corral-Santana, R Fender, JA Fernández-Ontiveros, D Mata Sánchez, G Panizo-Espinar, G Ponti, MAP Torres

Resolving the disc-halo degeneracy II: NGC 6946

Monthly Notices of the Royal Astronomical Society Oxford University Press 500:30 July 2020 (2020) 3579-3593

Authors:

S Aniyan, Anastasia Ponomareva, Kc Freeman, M Arnaboldi, Oe Gerhard, L Coccato, K Kuijken, M Merrifield

Abstract:

The mass-to-light ratio (M/L) is a key parameter in decomposing galactic rotation curves into contributions from the baryonic components and the dark halo of a galaxy. One direct observational method to determine the disc M/L is by calculating the surface mass density of the disc from the stellar vertical velocity dispersion and the scale height of the disc. Usually, the scale height is obtained from near-IR studies of edge-on galaxies and pertains to the older, kinematically hotter stars in the disc, while the vertical velocity dispersion of stars is measured in the optical band and refers to stars of all ages (up to ∼ 10 Gyr) and velocity dispersions. This mismatch between the scale height and the velocity dispersion can lead to underestimates of the disc surface density and a misleading conclusion of the sub-maximality of galaxy discs. In this paper we present the study of the stellar velocity dispersion of the disc galaxy NGC 6946 using integrated star light and individual planetary nebulae as dynamical tracers. We demonstrate the presence of two kinematically distinct populations of tracers which contribute to the total stellar velocity dispersion. Thus, we are able to use the dispersion and the scale height of the same dynamical population to derive the surface mass density of the disc over a radial extent. We find the disc of NGC 6946 to be closer to maximal with the baryonic component contributing most of the radial gravitational field in the inner parts of the galaxy (⁠Vmax(bar)=0.76(±0.14)Vmax⁠).