The curious case of the "Heartworm" Nebula

Astrophysical Journal IOP Publishing 934:1 (2022) 78

Authors:

WD Cotton, F Camilo, W Becker, JJ Condon, J Forbrich, Ian Heywood, B Hugo, S Legodi, T Mauch, P Predehl, P Slane, MA Thompson

Abstract:

The curious Galactic features near G357.2−0.2 were observed with the MeerKAT radio interferometer array in the UHF and L bands (0.56–1.68 GHz). There are two possibly related features: a newly identified faint heart-shaped partial shell (the "heart"), and a series of previously known but now much better imaged narrow, curved features (the "worm") interior to the heart. Polarized emission suggests that much of the emission is nonthermal and is embedded in a dense plasma. The filaments of the worm appear to be magnetic structures powered by embedded knots that are sites of particle acceleration. The morphology of the worm broadly resembles some known pulsar wind nebulae (PWNe) but there is no known pulsar or PWN which could be powering this structure. We also present eROSITA observations of the field; no part of the nebula is detected in X-rays, but the current limits do not preclude the existence of a pulsar/PWN of intermediate spin-down luminosity.

MIGHTEE: the nature of the radio-loud AGN population

ArXiv 2207.12379 (2022)

Authors:

IH Whittam, MJ Jarvis, CL Hale, M Prescott, LK Morabito, I Heywood, NJ Adams, J Afonso, Fangxia An, Y Ao, RA Bowler, JD Collier, RP Deane, J Delhaize, B Frank, M Glowacki, PW Hatfield, N Maddox, L Marchetti, AM Matthews, I Prandoni, S Randriamampandry, Z Randriamanakoto, DJB Smith, AR Taylor, NL Thomas, M Vaccari

A Late-time Radio Flare Following a Possible Transition in Accretion State in the Tidal Disruption Event AT 2019azh

The Astrophysical Journal American Astronomical Society 933:2 (2022) 176

Authors:

Itai Sfaradi, Assaf Horesh, Rob Fender, David A Green, David RA Williams, Joe Bright, Steve Schulze

Radio Galaxy Zoo: using semi-supervised learning to leverage large unlabelled data sets for radio galaxy classification under data set shift

Monthly Notices of the Royal Astronomical Society Oxford University Press (OUP) 514:2 (2022) 2599-2613

Authors:

Inigo V Slijepcevic, Anna MM Scaife, Mike Walmsley, Micah Bowles, O Ivy Wong, Stanislav S Shabala, Hongming Tang

Statistical properties of the population of the Galactic centre filaments – II. The spacing between filaments

Monthly Notices of the Royal Astronomical Society Oxford University Press 515:2 (2022) 3059-3093

Authors:

F Yusef-Zadeh, Rg Arendt, M Wardle, S Boldyrev, I Heywood, W Cotton, F Camilo

Abstract:

We carry out a population study of magnetized radio filaments in the Galactic centre using MeerKAT data by focusing on the spacing between the filaments that are grouped. The morphology of a sample of 43 groupings containing 174 magnetized radio filaments are presented. Many grouped filaments show harp-like, fragmented cometary tail-like, or loop-like structures in contrast to many straight filaments running mainly perpendicular to the Galactic plane. There are many striking examples of a single filament splitting into two prongs at a junction, suggestive of a flow of plasma along the filaments. Spatial variations in spectral index, brightness, bending, and sharpening along the filaments indicate that they are evolving on a 105-6-yr time-scale. The mean spacings between parallel filaments in a given grouping peaks at ∼16 arcsec. We argue by modeling that the filaments in a grouping all lie on the same plane and that the groupings are isotropically oriented in 3D space. One candidate for the origin of filamentation is interaction with an obstacle, which could be a compact radio source, before a filament splits and bends into multiple filaments. In this picture, the obstacle or sets the length scale of the separation between the filaments. Another possibility is synchrotron cooling instability occurring in cometary tails formed as a result of the interaction of cosmic ray driven Galactic centre outflow with obstacles such as stellar winds. In this picture, the mean spacing and the mean width of the filaments are expected to be a fraction of a parsec, consistent with observed spacing.