Stellar transits in active galactic nuclei

(2012)

Authors:

Bence Béky, Bence Kocsis

The host galaxy of the super-luminous SN 2010gx and limits on explosive nickel-56 production

(2012)

Authors:

Ting-Wan Chen, Stephen J Smartt, Fabio Bresolin, Andrea Pastorello, Rolf-Peter Kudritzki, Rubina Kotak, Matt McCrum, Morgan Fraser, Stefano Valenti

Interacting Supernovae and Supernova Impostors. SN 2009ip, is this the end?

(2012)

Authors:

A Pastorello, E Cappellaro, C Inserra, SJ Smartt, G Pignata, S Benetti, S Valenti, M Fraser, K Takats, S Benitez, MT Botticella, J Brimacombe, F Bufano, F Cellier-Holzem, MT Costado, G Cupani, I Curtis, N Elias-Rosa, M Ergon, JPU Fynbo, F-J Hambsch, M Hamuy, A Harutyunyan, KM Ivarson, E Kankare, JC Martin, R Kotak, AP LaCluyze, K Maguire, S Mattila, J Maza, M McCrum, M Miluzio, HU Norgaard-Nielsen, MC Nysewander, P Ochner, Y-C Pan, ML Pumo, DE Reichart, TG Tan, S Taubenberger, L Tomasella, M Turatto, D Wright

The progenitor mass of the Type IIP supernova SN 2004et from late-time spectral modeling

Astronomy and Astrophysics 546 (2012)

Authors:

A Jerkstrand, C Fransson, K Maguire, S Smartt, M Ergon, J Spyromilio

Abstract:

SN 2004et is one of the nearest and best-observed Type IIP supernovae, with a progenitor detection as well as good photometric and spectroscopic observational coverage well into the nebular phase. Based on nucleosynthesis from stellar evolution/explosion models we apply spectral modeling to analyze its 140-700 day evolution from ultraviolet to mid-infrared. We find a M ZAMS = 15 M âŠ(tm) progenitor star (with an oxygen mass of 0.8 M âŠ(tm)) to satisfactorily reproduce [Oâ‰i] λλ6300, 6364 and other emission lines of carbon, sodium, magnesium, and silicon, while 12 M âŠ(tm) and 19 M âŠ(tm) models under-and overproduce most of these lines, respectively. This result is in fair agreement with the mass derived from the progenitor detection, but in disagreement with hydrodynamical modeling of the early-time light curve. From modeling of the mid-infrared iron-group emission lines, we determine the density of the "Ni-bubble" to ρ(t) â‰7 × 10 -14 × (t/100 d) -3 g cm -3, corresponding to a filling factor of f = 0.15 in the metal core region (V = 1800 km≠s -1). We also confirm that silicate dust, CO, and SiO emission are all present in the spectra. ©2012 ESO.

M87 at metre wavelengths: the LOFAR picture

ArXiv 1210.1346 (2012)

Authors:

F de Gasperin, E Orru', M Murgia, A Merloni, H Falcke, R Beck, R Beswick, L Birzan, A Bonafede, M Bruggen, G Brunetti, K Chyzy, J Conway, JH Croston, T Ensslin, C Ferrari, G Heald, S Heidenreich, N Jackson, G Macario, J McKean, G Miley, R Morganti, A Offringa, R Pizzo, D Rafferty, H Roettgering, A Shulevski, M Steinmetz, C Tasse, S van der Tol, W van Driel, RJ van Weeren, JE van Zwieten, A Alexov, J Anderson, A Asgekar, M Avruch, M Bell, MR Bell, M Bentum, G Bernardi, P Best, F Breitling, JW Broderick, A Butcher, B Ciardi, RJ Dettmar, J Eisloeffel, W Frieswijk, H Gankema, M Garrett, M Gerbers, JM Griessmeier, AW Gunst, TE Hassall, J Hessels, M Hoeft, A Horneffer, A Karastergiou, J Koehler, Y Koopman, G Kuper, P Maat, G Mann, M Mevius, DD Mulcahy, H Munk, R Nijboer, M Kuniyoshi, J Noordam, H Paas, M Pandey, VN Pandey, A Polatidis, W Reich, AP Schoenmakers, J Sluman, O Smirnov, C Sobey, B Stappers, J Swinbank, M Tagger, Y Tang, I van Bemmel, W van Cappellen, AP van Duin, M van Haarlem, J van Leeuwen, R Vermeulen, C Vocks, S White, M Wise, O Wucknitz, P Zarka

Abstract:

M87 is a giant elliptical galaxy located in the centre of the Virgo cluster, which harbours a supermassive black hole of mass 6.4x10^9 M_sun, whose activity is responsible for the extended (80 kpc) radio lobes that surround the galaxy. The energy generated by matter falling onto the central black hole is ejected and transferred to the intra-cluster medium via a relativistic jet and morphologically complex systems of buoyant bubbles, which rise towards the edges of the extended halo. Here we present the first observations made with the new Low-Frequency Array (LOFAR) of M87 at frequencies down to 20 MHz. Images of M87 were produced at low radio frequencies never explored before at these high spatial resolution and dynamic range. To disentangle different synchrotron models and place constraints on source magnetic field, age and energetics, we also performed a detailed spectral analysis of M87 extended radio-halo using these observations together with archival data. We do not find any sign of new extended emissions; on the contrary the source appears well confined by the high pressure of the intra-cluster medium. A continuous injection of relativistic electrons is the model that best fits our data, and provides a scenario in which the lobes are still supplied by fresh relativistic particles from the active galactic nuclei. We suggest that the discrepancy between the low-frequency radio-spectral slope in the core and in the halo implies a strong adiabatic expansion of the plasma as soon as it leaves the core area. The extended halo has an equipartition magnetic field strength of ~10 uG, which increases to ~13 uG in the zones where the particle flows are more active. The continuous injection model for synchrotron ageing provides an age for the halo of ~40 Myr, which in turn provides a jet kinetic power of 6-10x10^44 erg/s.