The connection between the UV/optical and X-ray emission in the neutron star low-mass X-ray binary Aql X-1

Monthly Notices of the Royal Astronomical Society Oxford University Press (OUP) 493:1 (2020) 940-951

Authors:

E López-Navas, N Degenaar, AS Parikh, JV Hernández Santisteban, J van den Eijnden

Cosmic Evolution of Stellar-mass Black Hole Merger Rate in Active Galactic Nuclei

(2020)

Authors:

Y Yang, I Bartos, Z Haiman, B Kocsis, S Márka, H Tagawa

Design and operation of the ATLAS Transient Science Server

(2020)

Authors:

KW Smith, SJ Smartt, DR Young, JL Tonry, L Denneau, H Flewelling, AN Heinze, HJ Weiland, B Stalder, A Rest, CW Stubbs, JP Anderson, T-W Chen, P Clark, A Do, F Förster, M Fulton, J Gillanders, OR McBrien, D O'Neill, S Srivastav, DE Wright

Particle acceleration in astrophysical jets

(2020)

Authors:

James Matthews, Anthony Bell, Katherine Blundell

Uncovering the orbital dynamics of stars hidden inside their powerful winds: application to $η$ Carinae and RMC 140

Monthly Notices of the Royal Astronomical Society Oxford University Press 494:1 (2020) 17-35

Authors:

David Grant, Katherine Blundell, James Matthews

Abstract:

Determining accurate orbits of binary stars with powerful winds is challenging. The dense outflows increase the effective photospheric radius, precluding direct observation of the Keplerian motion; instead the observables are broad lines emitted over large radii in the stellar wind. Our analysis reveals strong, systematic discrepancies between the radial velocities extracted from different spectral lines: the more extended a line's emission region, the greater the departure from the true orbital motion. To overcome these challenges, we formulate a novel semi-analytical model which encapsulates both the star's orbital motion and the propagation of the wind. The model encodes the integrated velocity field of the out-flowing gas in terms of a convolution of past motion due to the finite flow speed of the wind. We test this model on two binary systems. (1), for the extreme case $\eta$ Carinae, in which the effects are most prominent, we are able to fit the model to 10 Balmer lines from H-alpha to H-kappa concurrently with a single set of orbital parameters: time of periastron $T_{0}=2454848$ (JD), eccentricity $e=0.91$, semi-amplitude $k=69$ km/s and longitude of periastron $\omega=241^\circ$. (2) for a more typical case, the Wolf-Rayet star in RMC 140, we demonstrate that for commonly used lines, such as He II and N III/IV/V, we expect deviations between the Keplerian orbit and the predicted radial velocities. Our study indicates that corrective modelling, such as presented here, is necessary in order to identify a consistent set of orbital parameters, independent of the emission line used, especially for future high accuracy work.