A Very Small Array search for the extended Sunyaev-Zel'dovich effect in the Corona Borealis supercluster

Monthly Notices of the Royal Astronomical Society Oxford University Press (OUP) 363:1 (2005) 79-92

Authors:

Ricardo Génova-Santos, José Alberto Rubiño-Martín, Rafael Rebolo, Kieran Cleary, Rod D Davies, Richard J Davis, Clive Dickinson, Nelson Falcón, Keith Grainge, Carlos M Gutiérrez, Michael P Hobson, Michael E Jones, Rüdiger Kneissl, Katy Lancaster, Carmen P Padilla-Torres, Richard DE Saunders, Paul F Scott, Angela C Taylor, Robert A Watson

Correlation between radio luminosity and X-ray timing frequencies in neutron star and black hole X-ray binaries

Monthly Notices of the Royal Astronomical Society Oxford University Press (OUP) 363:1 (2005) 112-120

Authors:

S Migliari, RP Fender, M van der Klis

Discovery of X-Ray Jets in the Microquasar H1743–322

The Astrophysical Journal American Astronomical Society 632:1 (2005) 504-513

Authors:

S Corbel, P Kaaret, RP Fender, AK Tzioumis, JA Tomsick, JA Orosz

Direct imaging search for substellar companions around neutron stars

Proceedings of the International Astronomical Union Cambridge University Press (CUP) 1:C200 (2005) 35-40

Authors:

B Posselt, R Neuhäuser, F Haberl

Absolute polarisation position angle profiles of southern pulsars at 1.4 and 3.1 GHz

ArXiv astro-ph/0509910 (2005)

Authors:

A Karastergiou, S Johnston

Abstract:

We present here a direct comparison of the polarisation position angle (PA) profiles of 17 pulsars, observed at 1.4 and 3.1 GHz. Absolute PAs are obtained at each frequency, permitting a measurement of the difference in the profiles. By doing this, we obtain more precise rotation measure (RM) values for some of the pulsars in the current catalogue. We find that, apart from RM corrections, there are small, pulse longitude dependent differences in PA with frequency. Such differences go beyond the interpretation of a geometrical origin. We describe in detail the PA evolution between the two frequencies and discuss possible causes, such as orthogonal and non-orthogonal polarisation modes of emission. We also use the PA and total power profiles to estimate the difference in emission height at which the two frequencies originate. In our data sample, there are changes in the relative strengths of different pulse components, especially overlapping linearly polarised components, which coincide with intrinsic changes of the PA profile, resulting in interesting PA differences between the two frequencies.