The peculiar mass-loss history of SN 2014C as revealed through AMI radio observations

(2016)

Authors:

GE Anderson, A Horesh, KP Mooley, AP Rushton, RP Fender, TD Staley, MK Argo, RJ Beswick, PJ Hancock, MA Perez-Torres, YC Perrott, RM Plotkin, ML Pretorius, C Rumsey, DJ Titterington

The peculiar mass-loss history of SN 2014C as revealed through AMI radio observations

Monthly Notices of the Royal Astronomical Society Oxford University Press 466:3 (2016) 3648-3662

Authors:

GE Anderson, A Horesh, Kunal P Mooley, Anthony P Rushton, Robert P Fender, Timothy D Staley, MK Argo, RJ Beswick, PJ Hancock, MA Pérez-Torres, YC Perrott, RM Plotkin, ML Pretorius, C Rumsey, DJ Titterington

Abstract:

We present a radio light curve of supernova (SN) 2014C taken with the Arcminute Microkelvin Imager (AMI) Large Array at 15.7 GHz. Optical observations presented by Milisavljevic et al. demonstrated that SN 2014C metamorphosed from a stripped-envelope Type Ib SN into a strongly interacting Type IIn SN within 1 yr. The AMI light curve clearly shows two distinct radio peaks, the second being a factor of 4 times more luminous than the first peak. This double bump morphology indicates two distinct phases of mass-loss from the progenitor star with the transition between density regimes occurring at 100-200 d. This reinforces the interpretation that SN 2014C exploded in a low-density region before encountering a dense hydrogen-rich shell of circumstellar material that was likely ejected by the progenitor prior to the explosion. The AMI flux measurements of the first light-curve bump are the only reported observations taken within ~50 to ~125 d post-explosion, before the blast-wave encountered the hydrogen shell. Simplistic synchrotron self-absorption and free-free absorption modelling suggest that some physical properties of SN 2014C are consistent with the properties of other Type Ibc and IIn SNe. However, our single frequency data does not allow us to distinguish between these two models, which implies that they are likely too simplistic to describe the complex environment surrounding this event. Lastly, we present the precise radio location of SN 2014C obtained with the electronic Multi-Element Remotely Linked Interferometer Network, which will be useful for future very long baseline interferometry observations of the SN.

Disc–jet quenching of the galactic black hole Swift J1753.5−0127

Monthly Notices of the Royal Astronomical Society Oxford University Press (OUP) 463:1 (2016) 628-634

Authors:

AP Rushton, AW Shaw, RP Fender, D Altamirano, P Gandhi, P Uttley, PA Charles, M Kolehmainen, GE Anderson, C Rumsey, DJ Titterington

Rapid Radio Flaring during an Anomalous Outburst of SS Cyg

(2016)

Authors:

KP Mooley, JCA Miller-Jones, RP Fender, GR Sivakoff, C Rumsey, Y Perrott, D Titterington, K Grainge, TD Russell, SH Carey, J Hickish, N Razavi-Ghods, A Scaife, P Scott, EO Waagen

Simultaneous radio and X-ray observations of PSR B0611+22

Monthly Notices of the Royal Astronomical Society Oxford University Press 462:3 (2016) 2518-2526

Authors:

K Rajwade, A Seymour, DR Lorimer, Aris Karastergiou, M Serylak, MA McLaughlin, J-M Griessmeier

Abstract:

We report results from simultaneous radio and X-ray observations of PSR B0611+22 which is known to exhibit bursting in its single-pulse emission. The pulse phase of the bursts vary with radio frequency. The bursts are correlated in 327/150 MHz data sets while they are anti-correlated, with bursts at one frequency associated with normal emission at the other, in 820/150 MHz data sets. Also, the flux density of this pulsar is lower than expected at 327 MHz assuming a power law. We attribute this unusual behaviour to the pulsar itself rather than absorption by external astrophysical sources. Using this data set over an extensive frequency range, we show that the bursting phenomenon in this pulsar exhibits temporal variance over a span of few hours. We also show that the bursting is quasi-periodic over the observed band. The anti-correlation in the phase offset of the burst mode at different frequencies suggests that the mechanisms responsible for phase offset and flux enhancement have different dependencies on the frequency. We did not detect the pulsar with XMM-Newton and place a 99 per cent confidence upper limit on the X-ray efficiency of 10-5.