G2 can Illuminate the Black Hole Population near the Galactic Center

(2013)

Authors:

Imre Bartos, Zoltan Haiman, Bence Kocsis, Szabolcs Marka

LOFAR detections of low-frequency radio recombination lines towards Cassiopeia A

ArXiv 1302.3128 (2013)

Authors:

Ashish Asgekar, JBR Oonk, S Yatawatta, RJ van Weeren, JP McKean, G White, N Jackson, J Anderson, IM Avruch, F Batejat, R Beck, ME Bell, MR Bell, I van Bemmel, MJ Bentum, G Bernardi, P Best, L Birzan, A Bonafede, R Braun, F Breitling, RH van de Brink, J Broderick, WN Brouw, M Bruggen, HR Butcher, W van Cappellen, B Ciardi, JE Conway, F de Gasperin, E de Geus, A de Jong, M de Vos, S Duscha, J Eisloffel, H Falcke, RA Fallows, C Ferrari, W Frieswijk, MA Garrett, J-M Griesmeier, T Grit, AW Gunst, TE Hassall, G Heald, JWT Hessels, M Hoeft, M Iacobelli, H Intema, E Juette, A Karastergiou, J Kohler, VI Kondratiev, M Kuniyoshi, G Kuper, C Law, J van Leeuwen, P Maat, G Macario, G Mann, S Markoff, D McKay-Bukowski, M Mevius, JCA Miller-Jones, JD Mol, R Morganti, DD Mulcahy, H Munk, MJ Norden, E Orru, H Paas, M Pandey-Pommier, VN Pandey, R Pizzo, AG Polatidis, W Reich, H Rottgering, B Scheers, A Schoenmakers, J Sluman, O Smirnov, C Sobey, M Steinmetz, M Tagger, Y Tang, C Tasse, R Vermeulen, C Vocks, RAMJ Wijers, MW Wise, O Wucknitz, P Zarka

Abstract:

Cassiopeia A was observed using the Low-Band Antennas of the LOw Frequency ARray (LOFAR) with high spectral resolution. This allowed a search for radio recombination lines (RRLs) along the line-of-sight to this source. Five carbon-alpha RRLs were detected in absorption between 40 and 50 MHz with a signal-to-noise ratio of > 5 from two independent LOFAR datasets. The derived line velocities (v_LSR ~ -50 km/s) and integrated optical depths (~ 13 s^-1) of the RRLs in our spectra, extracted over the whole supernova remnant, are consistent within each LOFAR dataset and with those previously reported. For the first time, we are able to extract spectra against the brightest hotspot of the remnant at frequencies below 330 MHz. These spectra show significantly higher (15-80 %) integrated optical depths, indicating that there is small-scale angular structure on the order of ~1 pc in the absorbing gas distribution over the face of the remnant. We also place an upper limit of 3 x 10^-4 on the peak optical depths of hydrogen and helium RRLs. These results demonstrate that LOFAR has the desired spectral stability and sensitivity to study faint recombination lines in the decameter band.

PESSTO monitoring of SN 2012hn: further heterogeneity among faint type I supernovae

(2013)

Authors:

S Valenti, F Yuan, S Taubenberger, K Maguire, A Pastorello, S Benetti, SJ Smartt, E Cappellaro, DA Howell, L Bildsten, K Moore, M Stritzinger, JP Anderson, S Benitez-Herrera, F Bufano, S Gonzalez-Gaitan, MG McCrum, G Pignata, M Fraser, A Gal-Yam, L Le Guillou, C Inserra, DE Reichart, R Scalzo, M Sullivan, O Yaron, DR Young

Spectroscopic Observations of SN 2012fr: A Luminous Normal Type Ia Supernova with Early High Velocity Features and Late Velocity Plateau

(2013)

Authors:

MJ Childress, RA Scalzo, SA Sim, BE Tucker, F Yuan, BP Schmidt, SB Cenko, JM Silverman, C Contreras, EY Hsiao, M Phillips, N Morrell, SW Jha, C McCully, AV Filippenko, JP Anderson, S Benetti, F Bufano, T de Jaeger, F Forster, A Gal-Yam, L Le Guillou, K Maguire, J Maund, PA Mazzali, G Pignata, S Smartt, J Spyromilio, M Sullivan, F Taddia, S Valenti, DDR Bayliss, M Bessell, GA Blanc, DJ Carson, KI Clubb, C de Burgh-Day, TD Desjardins, JJ Fang, OD Fox, EL Gates, I-T Ho, S Keller, PL Kelly, C Lidman, NS Loaring, JR Mould, M Owers, S Ozbilgen, L Pei, T Pickering, MB Pracy, JA Rich, BE Schaefer, N Scott, M Stritzinger, FPA Vogt, G Zhou

Jet spectral breaks in black hole x-ray binaries

Monthly Notices of the Royal Astronomical Society 429:1 (2013) 815-832

Authors:

DM Russell, S Markoff, P Casella, AG Cantrell, R Chatterjee, RP Fender, E Gallo, P Gandhi, J Homan, D Maitra, JCA Miller-Jones, K O'Brien, T Shahbaz

Abstract:

In X-ray binaries, compact jets are known to commonly radiate at radio to infrared frequencies, whereas at optical to -ray energies, the contribution of the jet is debated. The total luminosity, and hence power of the jet, is critically dependent on the position of the break in its spectrum, between optically thick (self-absorbed) and optically thin synchrotron emission. This break, or turnover, has been reported in just one black hole X-ray binary (BHXB) thus far, GX 339-4, and inferred via spectral fitting in two others, A0620-00 and Cyg X-1. Here, we collect a wealth of multi-wavelength data from the outbursts of BHXBs during hard X-ray states, in order to search for jet breaks as yet unidentified in their spectral energy distributions. In particular, we report the direct detection of the jet break in the spectrum of V404 Cyg during its 1989 outburst, at b = (1.8 ± 0.3) × 1014 Hz (1.7 ± 0.2 μm). We increase the number of BHXBs with measured jet breaks from three to eight. Jet breaks are found at frequencies spanning more than two orders of magnitude, from b = (4.5 ± 0.8) × 1012 Hz for XTE J1118+480 during its 2005 outburst, to b > 4.7 × 1014 Hz for V4641 Sgr in outburst. A positive correlation between jet break frequency and luminosity is expected theoretically; b L ~0.5 ,jet if other parameters are constant. With constraints on the jet break in a total of 12 BHXBs including two quiescent systems, we find a large range of jet break frequencies at similar luminosities and no obvious global relation (but such a relation cannot be ruled out for individual sources). We speculate that different magnetic field strengths and/or different radii of the acceleration zone in the inner regions of the jet are likely to be responsible for the observed scatter between sources. There is evidence that the high-energy cooling break in the jet spectrum shifts from UV energies at LX ~ 10-8LEdd (implying the jet may dominate the X-ray emission in quiescence) to X-ray energies at ~10-3LEdd. Finally, we find that the jet break luminosity scales as L,jet L0.56±0.05 X (very similar to the radio-X-ray correlation), and radio-faint BHXBs have fainter jet breaks. In quiescence the jet break luminosity exceeds the X-ray luminosity. © 2012 The Authors.