Up and Down the Black Hole Radio/X-ray Correlation: the 2017 mini-outbursts from Swift J1753.5-0127

(2017)

Authors:

RM Plotkin, J Bright, JCA Miller-Jones, AW Shaw, JA Tomsick, TD Russell, G-B Zhang, DM Russell, RP Fender, J Homan, P Atri, F Bernardini, JD Gelfand, F Lewis, TM Cantwell, SH Carey, KJB Grainge, J Hickish, YC Perrott, N Razavi-Ghods, AMM Scaife, PF Scott, DJ Titterington

A star formation study of the ATLAS3D early-type galaxies with the AKARI all-sky survey

Astronomy and Astrophysics EDP Sciences 605 (2017) A74

Authors:

T Kokusho, H Kaneda, Martin Bureau, T Suzuki, K Murata, A Kondo, M Yamagishi

Abstract:

The star formation properties of early-type galaxies (ETGs) are currently the subject of considerable interest, particularly whether they differ from those of gas-rich spirals. We perform a systematic study of star formation in a large sample of local ETGs using polycyclic aromatic hydrocarbon (PAH) and dust emission, focusing on the galaxies' star formation rates (SFRs) and star formation efficiencies (SFEs). Our sample is composed of the 260 ETGs from the ATLAS3D survey, from which we use the cold gas measurements (HI and CO). The SFRs are estimated from stellar, PAH and dust fits to spectral energy distributions created from new AKARI measurements and literature data from WISE and 2MASS. The mid-infrared luminosities of non-CO-detected galaxies are well correlated with their stellar luminosities, showing that they trace (circum)stellar dust emission. CO-detected galaxies show an excess above these correlations, uncorrelated with their stellar luminosities, indicating that they likely contain PAHs and dust of interstellar origin. PAH and dust luminosities of CO-detected galaxies show tight correlations with their molecular gas masses, and the derived current SFRs are typically 0.01-1 Msun/yr. These SFRs systematically decrease with stellar age at fixed stellar mass, while they correlate nearly linearly with stellar mass at fixed age. The majority of local ETGs follow the same star-formation law as local star-forming galaxies, and their current SFEs do not depend on either stellar mass or age. Our results clearly indicate that molecular gas is fueling current star formation in local ETGs, that appear to acquire this gas via mechanisms regulated primarily by stellar mass. The current SFEs of local ETGs are similar to those of local star-forming galaxies, indicating that their low SFRs are likely due to smaller cold gas fractions rather than a suppression of star formation.

Paving the way to simultaneous multi-wavelength astronomy

(2017)

Authors:

MJ Middleton, P Casella, P Gandhi, E Bozzo, G Anderson, N Degenaar, I Donnarumma, G Israel, C Knigge, A Lohfink, S Markoff, T Marsh, N Rea, S Tingay, K Wiersema, D Altamirano, D Bhattacharya, WN Brandt, S Carey, P Charles, M Diaz Trigo, C Done, M Kotze, S Eikenberry, R Fender, P Ferruit, F Fuerst, J Greiner, A Ingram, L Heil, P Jonker, S Komossa, B Leibundgut, T Maccarone, J Malzac, V McBride, J Miller-Jones, M Page, EM Rossi, DM Russell, T Shahbaz, GR Sivakoff, M Tanaka, DJ Thompson, M Uemura, P Uttley, G van Moorsel, M Van Doesburgh, B Warner, B Wilkes, J Wilms, P Woudt

The KMOS Cluster Survey (KCS). I. The fundamental plane and the formation ages of cluster galaxies at redshift 1.4 < Z < 1.6

Astrophysical Journal American Astronomical Society 846:2 (2017) 1-25

Authors:

A Beifiori, JT Mendel, JCC Chan, RP Saglia, R Bender, Michele Cappellari, Roger L Davies, A Galametz, Ryan CW Houghton, Laura J Prichard, R Smith, John P Stott, DJ Wilman, Ian J Lewis, R Sharples, M Wegner

Abstract:

The American Astronomical Society. All rights reserved. We present the analysis of the fundamental plane (FP) for a sample of 19 massive red-sequence galaxies (M· > ×4 10 10 M·) in three known overdensities at 1.39 1.61 < < z from the K-band Multi-object Spectrograph (KMOS) Cluster Survey, a guaranteed-time program with spectroscopy from the KMOS at the VLT and imaging from the Hubble Space Telescope. As expected, we find that the FP zero-point in B band evolves with redshift, from the value 0.443 of Coma to -0.10±0.09, -0.19±0.05, and -0.29±0.12 for our clusters at z = 1.39, z = 1.46, and z = 1.61, respectively. For the most massive galaxies (log 1 M M· > 1) in our sample, we translate the FP zero-point evolution into a mass-to-light-ratio M/L evolution, finding D log 0.46 0.10 M L z B = - (D log )0.52 0.07 M L z B = -to(D log ) 0.55 0.10 M L z B = - respectively. We assess the potential contribution of the galaxy structural and stellar velocity dispersion evolution to the evolution of the FP zero-point and find it to be ∼6%-35% of the FP zero-point evolution. The rate of M/L evolution is consistent with galaxies evolving passively. Using single stellar population models, we find an average age of 2.33- +0.51 0.86 Gyr for the log 1 M M· > 1 galaxies in our massive and virialized cluster at z = 1.39,1.59- +0.62 1.40 Gyr in a massive but not virialized cluster at z = 1.46, and 1.20- +0.47 1.03 Gyr in a protocluster at z = 1.61. After accounting for the difference in the age of the universe between redshifts, the ages of the galaxies in the three overdensities are consistent within the errors, with possibly a weak suggestion that galaxies in the most evolved structure are older.

Spectral differences between the jets in ‘radio loud’ and ‘radio quiet’ hard state black hole binaries

Monthly Notices of the Royal Astronomical Society Oxford University Press 473:3 (2017) 4122-4129

Authors:

M Espinasse, Robert Fender

Abstract:

We have compiled from the available literature a large set of radio measurements of black hole binaries in the hard X-ray state for which measurements of the gigahertz frequency radio spectral index are possible. We separate the sample into `radio loud' and `radio quiet' subsets based upon their distribution in the radio -- X-ray plane, and investigate the distribution of radio spectral indices within each subset. The distribution of spectral indices of the `radio loud' subset is well described by a Gaussian distribution with mean spectral index $\alpha = +0.2$ and standard deviation $0.2$ (here spectral index is defined such that a positive spectral index means more flux at higher frequencies). The sparser sample for the `radio quiet' subset can be approximated, less well, by a Gaussian with mean $\alpha = -0.2$ and standard deviation $0.3$; alternatively the simple mean of the distribution of the radio quiet subset is $-0.3$. The two spectral index distributions are different at high statistical significance. Confirming previous work in the literature, we test to see if the differences in observed spectra could result from different distributions of jet viewing angles, but find no evidence for this. We conclude therefore that the jets in the two groups are physically different in some way, and briefly discuss possible origins and further possible diagnostics. Finally we note that extrapolating to lower frequencies the two subsets move closer together in the radio -- X-ray plane, and approximately merge into a single distribution at around 400 MHz.