The dynamics and stability of circumbinary orbits

MONTHLY NOTICES OF THE ROYAL ASTRONOMICAL SOCIETY 418:4 (2011) 2656-2668

Authors:

Samuel Doolin, Katherine M Blundell

The inverse-Compton ghost HDF130 and the giant radio galaxy 6C0905+3955: Matching an analytic model for double-lobed radio source evolution

Monthly Notices of the Royal Astronomical Society (2011)

Authors:

P Mocz, AC Fabian, KM Blundell, PT Goodall, SC Chapman, DJ Saikia

Radio and X-ray emission from disc winds in radio-quiet quasars

ArXiv 1012.4741 (2010)

Authors:

KC Steenbrugge, EJD Jolley, Z Kuncic, KM Blundell

Abstract:

It has been proposed that the radio spectra of radio-quiet quasars is produced by free-free emission in the optically thin part of an accretion disc wind. An important observational constraint on this model is the observed X-ray luminosity. We investigate this constraint using a sample of PG radio-quiet quasars for which XMM-Newton EPIC spectra are available. Comparing the predicted and measured luminosities for 0.5, 2 and 5 keV, we conclude that all of the studied PG quasars require a large hydrogen column density absorber, requiring these quasars to be close to or Compton-thick. Such a large column density can be directly excluded for PG 0050+124, for which a high-resolution RGS spectrum exists. Further constraint on the column density for a further 19 out of the 21 studied PG quasars comes from the EPIC spectrum characteristics such as hard X-ray power-law photon index and the equivalent width of the Fe Kalpha line; and the small equivalent width of the C IV absorber present in UV spectra. For 2 sources: PG 1001+054 and PG 1411+442 we cannot exclude that they are indeed Compton-thick, and the radio and X-ray luminosity are due to a wind originating close to the super-massive black hole. We conclude that for 20 out of 22 PG quasars studied free-free emission from a wind emanating from the accretion disc cannot mutually explain the observed radio and X-ray luminosity.

Radio and X-ray emission from disc winds in radio-quiet quasars

(2010)

Authors:

KC Steenbrugge, EJD Jolley, Z Kuncic, KM Blundell

LOFT: A large observatory for x-ray timing

Proceedings of Science (2010)

Authors:

F Muleri, M Feroci, T Belloni, J Braga, S Campana, T Courvousier, M Hernanz, R Hudec, GL Israel, PS Ray, A Santangelo, L Stella, A Vacchi, M Van Der Klis, D Walton, A Zdziarski, JM Alvarez, A Argan, G Baldazzi, M Barbera, G Bertuccio, V Bonvicini, E Bozzo, R Campana, A Collura, G Cusumano, E Del Monte, JW Den Herder, S Di Cosimo, G Di Persio, Y Evangelista, F Fuschino, JL Galvez, P Giommi, M Grassi, P Guttridge, JJM In'T Zand, D Kataria, D Klochkov, C Labanti, F Lazzarotto, P Malcovati, M Marisaldi, M Mastropietro, T Mineo, E Morelli, P Orleanski, B Phlips, L Picolli, M Rapisarda, A Rashevski, R Remillard, A Rubini, T Schanz, A Segreto, M Stolarski, C Tenzer, R Wawrzaszek, C Wilson-Hodge, B Winter, G Zampa, N Zampa, A Alpar, D Altamirano, L Amati, LA Antonelli, P Attinà, C Barbieri, L Burderi, M Bursa, GA Caliandro, P Casella, D Chakrabarty, A Corongiu, E Costa, S Covino, S Dall'Osso, F D'Amico, C Done, T Di Salvo, A Drago, D De Martino, A De Rosa, I Donnarumma, M Dovciak, U Ertan, M Falanga, R Fender, F Frontera, P Ghandi, E Gogus, W Hermsen, J Isern, J Horak, P Jonker, E Kalemci, G Kanbach, V Karas, W Kluzniak

Abstract:

LOFT (Large area Observatory For x-ray Timing) is an innovative mission submitted in response to the Cosmic Vision "Call for a Medium-size mission opportunity for a launch in 2022" recently issued by ESA. LOFT is an ideal candidate for the next generation of (extremely) large experiments for X-ray timing dedicated to the study of the physics of compact objects and to the understanding of the behavior of matter in strong gravitational fields. Recent developments in the field of large area monolithic silicon detectors allowed us to reach an effective area ∼12 m2 (15 m2 goal), more than a order of magnitude larger that RXTE/PCA, in the energy range 2-30 keV (1-40 keV goal). This Large Area Detector (LAD) will have both high timing resolution (<10 μs, 5 μs goal) and good spectral capabilities (<260 eV, <180 eV goal). A Wide Field Monitor (WFM), sensitive in the ∼1-50 keV energy range, will observe simultaneously more than a quarter of the sky in order to both discover and localize transient events and study their long term evolution. © Copyright owned by the author(s) under the terms of the Creative Commons Attribution-NonCommercial-ShareAlike Licence.