Searching for the Signatures of Jet‐ISM Interactions in X‐ray Binaries

AIP Conference Proceedings AIP Publishing 1010:1 (2008) 50-56

Authors:

James Miller-Jones, Dave Russell, Catherine Brocksopp, Jennifer Sokoloski, Ben Stappers, Tom Muxlow, Reba M Bandyopadhyay, Stefanie Wachter, Dawn Gelino, Christopher R Gelino

Watching the Formation and Evolution of Compact Jets from Accreting Black Holes

AIP Conference Proceedings AIP Publishing 1010:1 (2008) 13-17

Authors:

John A Tomsick, Simone Migliari, Sera Markoff, Emrah Kalemci, Charles D Bailyn, Michelle M Buxton, Stephane Corbel, Rob Fender, Philip Kaaret, Reba M Bandyopadhyay, Stefanie Wachter, Dawn Gelino, Christopher R Gelino

A semi-empirical simulation of the extragalactic radio continuum sky for next generation radio telescopes

ArXiv 0805.3413 (2008)

Authors:

RJ Wilman, L Miller, MJ Jarvis, T Mauch, F Levrier, FB Abdalla, S Rawlings, H-R Kloeckner, D Obreschkow, D Olteanu, S Young

Abstract:

We have developed a semi-empirical simulation of the extragalactic radio continuum sky suitable for aiding the design of next generation radio interferometers such as the Square Kilometre Array (SKA). The emphasis is on modelling the large-scale cosmological distribution of radio sources rather than the internal details of individual galaxies. Here we provide a description of the simulation to accompany the online release of a catalogue of 320 million simulated radio sources. The simulation covers 20x20 deg^2 - a plausible upper limit to the instantaneous field of view attainable with future (e.g. SKA) aperture array technologies - out to redshift z=20, and down to flux density limits of 10 nJy at 151, 610 MHz, 1.4, 4.86 and 18 GHz. Five distinct source types are included: radio-quiet AGN, radio-loud AGN of the FRI and FRII structural classes, and star-forming galaxies, the latter split into populations of quiescent and starbursting galaxies. In our semi-empirical approach, the simulated sources are drawn from observed (or extrapolated) luminosity functions and grafted onto an underlying dark matter density field with biases which reflect their measured large-scale clustering. A numerical Press-Schechter-style filtering of the density field is used to identify and populate clusters of galaxies. Radio source structures are built from point source and elliptical sub-components, and for FRI and FRII sources an orientation-based unification and beaming model is used to partition flux between the core and extended lobes and hotspots. The simulation output can be post-processed to achieve more complete agreement with observational data in the years ahead, with the aim of using these 'idealised skies' in telescope simulators to optimise the design of the SKA itself (abridged).

The needle in the haystack: where to look for more isolated cooling neutron stars

Astronomy & Astrophysics EDP Sciences 482:2 (2008) 617-629

Authors:

B Posselt, SB Popov, F Haberl, J Trümper, R Turolla, R Neuhäuser

Multi-frequency integrated profiles of pulsars

ArXiv 0804.3838 (2008)

Authors:

Simon Johnston, Aris Karastergiou, Dipanjan Mitra, Yashwant Gupta

Abstract:

We have observed a total of 67 pulsars at five frequencies ranging from 243 to 3100 MHz. Observations at the lower frequencies were made at the Giant Metre Wave Telescope in India and those at higher frequencies at the Parkes Telescope in Australia. We present profiles from 34 of the sample with the best signal to noise ratio and the least scattering. The general `rules' of pulsar profiles are seen in the data; profiles get narrower, the polarization fraction declines and outer components become more prominent as the frequency increases. Many counterexamples to these rules are also observed, and pulsars with complex profiles are especially prone to rule breaking. We hypothesise that the location of pulsar emission within the magnetosphere evolves with time as the the pulsar spins down. In highly energetic pulsars, the emission comes from a confined range of high altitudes, in the middle range of spin down energies the emission occurs over a wide range of altitudes whereas in pulsars with low spin-down energies it is confined to low down in the magnetosphere.