$\alpha$-attractor dark energy in view of next-generation cosmological surveys

(2019)

Authors:

Carlos García-García, Pilar Ruíz-Lapuente, David Alonso, M Zumalacárregui

$α$-attractor dark energy in view of next-generation cosmological surveys

ArXiv 1905.03753 (2019)

Authors:

Carlos García-García, Pilar Ruíz-Lapuente, David Alonso, M Zumalacárregui

Discovery of a radio transient in M81

(2019)

Authors:

GE Anderson, JCA Miller-Jones, MJ Middleton, R Soria, DA Swartz, R Urquhart, N Hurley-Walker, PJ Hancock, RP Fender, P Gandhi, S Marko, TP Roberts

The energetics of starburst-driven outflows at z ∼ 1 from KMOS

Monthly Notices of the Royal Astronomical Society Oxford University Press 487:1 (2019) 381-393

Authors:

AM Swinbank, CM Harrison, AL Tiley, HL Johnson, I Smail, JP Stott, PN Best, RG Bower, Martin Bureau, A Bunker, M Cirasuolo, M Jarvis, GE Magdis, RM Sharples, D Sobral

Abstract:

We present an analysis of the gas outflow energetics from KMOS observations of ∼ 529 main-sequence star-forming galaxies at z ∼ 1 using broad, underlying H α and forbidden lines of [N II] and [S II]. Based on the stacked spectra for a sample with median star-formation rates and stellar masses of SFR = 7 M⊙   yr−1 and M⋆ = (1.0 ± 0.1) × 1010 M⊙, respectively, we derive a typical mass outflow rate of M˙wind = 1–4 M⊙ yr−1 and a mass loading of M˙wind / SFR = 0.2–0.4. By comparing the kinetic energy in the wind with the energy released by supernovae, we estimate a coupling efficiency between the star formation and wind energetics of ϵ ∼  0.03. The mass loading of the wind does not show a strong trend with star-formation rate over the range ∼ 2–20 M⊙ yr−1, although we identify a trend with stellar mass such that dM / dt / SFR ∝ M0.26±0.07⋆⁠. Finally, the line width of the broad H α increases with disc circular velocity with a sub-linear scaling relation FWHMbroad ∝ v0.21 ± 0.05. As a result of this behaviour, in the lowest mass galaxies (M⋆ ≲ 1010 M⊙), a significant fraction of the outflowing gas should have sufficient velocity to escape the gravitational potential of the halo whilst in the highest mass galaxies (M⋆ ≳ 1010 M⊙) most of the gas will be retained, flowing back on to the galaxy disc at later times.

A rapidly changing jet orientation in the stellar-mass black-hole system V404 Cygni

Nature Nature Research 569 (2019) 374-377

Authors:

James CA Miller-Jones, Alexandra J Tetarenko, Gregory R Sivakoff, Matthew J Middleton, Diego Altamirano, Gemma E Anderson, Tomaso M Belloni, Rob P Fender, Peter G Jonker, Elmar G Körding, Hans A Krimm, Dipankar Maitra, Sera Markoff, Simone Migliari, Kunal P Mooley, Michael P Rupen, David M Russell, Thomas D Russell, Craig L Sarazin, Roberto Soria, Valeriu Tudose

Abstract:

Powerful relativistic jets are one of the main ways in which accreting black holes provide kinetic feedback to their surroundings. Jets launched from or redirected by the accretion flow that powers them are expected to be affected by the dynamics of the flow, which for accreting stellar-mass black holes has shown evidence for precession1 due to frame-dragging effects that occur when the black-hole spin axis is misaligned with the orbital plane of its companion star2. Recently, theoretical simulations have suggested that the jets can exert an additional torque on the accretion flow3, although the interplay between the dynamics of the accretion flow and the launching of the jets is not yet understood. Here we report a rapidly changing jet orientation—on a time scale of minutes to hours—in the black-hole X-ray binary V404 Cygni, detected with very-long-baseline interferometry during the peak of its 2015 outburst. We show that this changing jet orientation can be modelled as the Lense–Thirring precession of a vertically extended slim disk that arises from the super-Eddington accretion rate4. Our findings suggest that the dynamics of the precessing inner accretion disk could play a role in either directly launching or redirecting the jets within the inner few hundred gravitational radii. Similar dynamics should be expected in any strongly accreting black hole whose spin is misaligned with the inflowing gas, both affecting the observational characteristics of the jets and distributing the black-hole feedback more uniformly over the surrounding environment5,6.