Vector-apodizing phase plate coronagraph: design, current performance, and future development [Invited].

Applied Optics Optica Publishing Group 60:19 (2021) d52-d72

Authors:

DS Doelman, F Snik, EH Por, SP Bos, GPPL Otten, M Kenworthy, SY Haffert, M Wilby, AJ Bohn, BJ Sutlieff, K Miller, M Ouellet, J de Boer, CU Keller, MJ Escuti, S Shi, NZ Warriner, K Hornburg, JL Birkby, J Males, KM Morzinski, LM Close, J Codona, J Long, L Schatz, J Lumbres, A Rodack, K Van Gorkom, A Hedglen, O Guyon, J Lozi, T Groff, J Chilcote, N Jovanovic, S Thibault, C de Jonge, G Allain, C Vallée, D Patel, O Côté, C Marois, P Hinz, J Stone, A Skemer, Z Briesemeister, A Boehle, AM Glauser, W Taylor, P Baudoz, E Huby, O Absil, B Carlomagno, C Delacroix

A self-lensing binary massive black hole interpretation of quasi-periodic eruptions (vol 503, pg 1703, 2021)

MONTHLY NOTICES OF THE ROYAL ASTRONOMICAL SOCIETY 504:4 (2021) 5512-5512

Authors:

Adam Ingram, Sara E Motta, Suzanne Aigrain, Aris Karastergiou

Comments on Barker and Astoul (2021)

(2021)

Abstract:

The tidal evolution of interacting binaries when the orbital period is short compared to the primary star's convective time scale is a problem of long-standing. Terquem (2021) has argued that, when this temporal ordering scheme is obeyed, the rate of energy transfer from tides to convection (denoted $D_R$) is given by the product of the averaged Reynolds stress associated with the tidal velocity and the mean shear associated with the convective flow. In a recent response, Barker and Astoul (2021, hereafter BA21) claim to show that $D_R$ (in this form) cannot contribute to tidal dissipation. Their analysis is based on a study of Boussinesq and anelastic models. Here, we demonstrate that BA21 misidentify the correct term responsible for energy transfer between tides and convection. As a consequence, their anelastic calculations do not prove that the $D_R$ formulation is invalidated as an energy-loss coupling between tides and convection. BA21 also carry out a calculation in the Boussinesq approximation. Here, their claim that $D_R$ once again does not contribute is based on boundary conditions that do not apply to any star or planet that radiates energy from its surface, which is a key dissipational process in the problem we consider.

High-contrast observations of brown dwarf companion HR 2562 B with the vector Apodizing Phase Plate coronagraph

(2021)

Authors:

Ben J Sutlieff, Alexander J Bohn, Jayne L Birkby, Matthew A Kenworthy, Katie M Morzinski, David S Doelman, Jared R Males, Frans Snik, Laird M Close, Philip M Hinz, David Charbonneau

Hot planets around cool stars – two short-period mini-Neptunes transiting the late K-dwarf TOI-1260

Monthly Notices of the Royal Astronomical Society Oxford University Press (OUP) 505:4 (2021) 4684-4701

Authors:

IY Georgieva, CM Persson, O Barragán, G Nowak, M Fridlund, D Locci, E Palle, R Luque, I Carleo, D Gandolfi, SR Kane, J Korth, KG Stassun, J Livingston, EC Matthews, KA Collins, SB Howell, LM Serrano, S Albrecht, A Bieryla, CE Brasseur, D Ciardi, WD Cochran, KD Colon, IJM Crossfield, Sz Csizmadia, HJ Deeg, M Esposito, E Furlan, T Gan, E Goffo, E Gonzales, S Grziwa, EW Guenther, P Guerra, T Hirano, JM Jenkins, ELN Jensen, P Kabáth, E Knudstrup, KWF Lam, DW Latham, AM Levine, RA Matson, S McDermott, HLM Osborne, M Paegert, SN Quinn, S Redfield, GR Ricker, JE Schlieder, NJ Scott, S Seager, AMS Smith, P Tenenbaum, JD Twicken, R Vanderspek, V Van Eylen, JN Winn