Observations of Pressure Anisotropy Effects within Semi-Collisional Magnetized-Plasma Bubbles

(2020)

Authors:

ER Tubman, AS Joglekar, AFA Bott, M Borghesi, B Coleman, G Cooper, CN Danson, P Durey, JM Foster, P Graham, G Gregori, ET Gumbrell, MP Hill T Hodge, S Kar, RJ Kingham, M Read, CP Ridgers, J Skidmore, C Spindloe, AGR Thomas, P Treadwell, S Wilson, L Willingale, NC Woolsey

Probability distribution of astrophysical gravitational-wave background fluctuations

Physical Review D American Physical Society (APS) 102:8 (2020) 083501

Authors:

Yonadav Barry Ginat, Vincent Desjacques, Robert Reischke, Hagai B Perets

Detecting Kozai–Lidov Imprints on the Gravitational Waves of Intermediate-mass Black Holes in Galactic Nuclei

The Astrophysical Journal American Astronomical Society 901:2 (2020) 125-125

Authors:

Barnabás Deme, Bao-Minh Hoang, Smadar Naoz, Bence Kocsis

Turbulence-level dependence of cosmic ray parallel diffusion

Monthly Notices of the Royal Astronomical Society Oxford University Press (OUP) 498:4 (2020) 5051-5064

Authors:

P Reichherzer, J Becker Tjus, EG Zweibel, L Merten, MJ Pueschel

Jeans modelling of the Milky Way’s nuclear stellar disc

Monthly Notices of the Royal Astronomical Society Oxford University Press (OUP) (2020)

Authors:

Mattia C Sormani, John Magorrian, Francisco Nogueras-Lara, Nadine Neumayer, Ralph Schönrich, Ralf S Klessen, Alessandra Mastrobuono-Battisti

Abstract:

<jats:title>Abstract</jats:title> <jats:p>The nuclear stellar disc (NSD) is a flattened stellar structure that dominates the gravitational potential of the Milky Way at Galactocentric radii 30 ≲ R ≲ 300 pc. In this paper, we construct axisymmetric Jeans dynamical models of the NSD based on previous photometric studies and we fit them to line-of-sight kinematic data of APOGEE and SiO maser stars. We find that (i) the NSD mass is lower but consistent with the mass independently determined from photometry by Launhardt et al. (2002). Our fiducial model has a mass contained within spherical radius r = 100 pc of $M(r&amp;lt;100\, {\rm pc}) = 3.9 \pm 1 \times 10^8 \, \rm M_\odot$ and a total mass of $M_{\rm NSD} = 6.9 \pm 2 \times 10^8 \, \rm M_\odot$. (ii) The NSD might be the first example of a vertically biased disc, i.e. with ratio between the vertical and radial velocity dispersion σz/σR &amp;gt; 1. Observations and theoretical models of the star-forming molecular gas in the central molecular zone suggest that large vertical oscillations may be already imprinted at stellar birth. However, the finding σz/σR &amp;gt; 1 depends on a drop in the velocity dispersion in the innermost few tens of parsecs, on our assumption that the NSD is axisymmetric, and that the available (extinction corrected) stellar samples broadly trace the underlying light and mass distributions, all of which need to be established by future observations and/or modelling. (iii) We provide the most accurate rotation curve to date for the innermost 500 pc of our Galaxy.</jats:p>