Axion resonances in binary pulsar systems

Journal of Cosmology and Astroparticle Physics IOP Publishing 2020:03 (2020) 061-061

Authors:

Mor Rozner, Evgeni Grishin, Yonadav Barry Ginat, Andrei P Igoshev, Vincent Desjacques

The Karl G. Jansky very large array sky survey (VLASS). Science case and survey design

Publications of the Astronomical Society of the Pacific 132:1009 (2020)

Authors:

M Lacy, SA Baum, CJ Chandler, S Chatterjee, TE Clarke, S Deustua, J English, J Farnes, BM Gaensler, N Gugliucci, G Hallinan, BR Kent, A Kimball, CJ Law, TJW Lazio, J Marvil, SA Mao, D Medlin, K Mooley, EJ Murphy, S Myers, R Osten, GT Richards, E Rosolowsky, L Rudnick, F Schinzel, GR Sivakoff, LO Sjouwerman, R Taylor, RL White, J Wrobel, H Andernach, AJ Beasley, E Berger, S Bhatnager, M Birkinshaw, GC Bower, WN Brandt, S Brown, S Burke-Spolaor, BJ Butler, J Comerford, PB Demorest, H Fu, S Giacintucci, K Golap, T Güth, CA Hales, R Hiriart, J Hodge

Abstract:

© 2020. The Astronomical Society of the Pacific. The Very Large Array Sky Survey (VLASS) is a synoptic, all-sky radio sky survey with a unique combination of high angular resolution (≈2.″5), sensitivity (a 1σ goal of 70 μJy/beam in the coadded data), full linear Stokes polarimetry, time domain coverage, and wide bandwidth (2–4 GHz). The first observations began in 2017 September, and observing for the survey will finish in 2024. VLASS will use approximately 5500 hr of time on the Karl G. Jansky Very Large Array (VLA) to cover the whole sky visible to the VLA (decl. > −40°), a total of 33 885 deg2. The data will be taken in three epochs to allow the discovery of variable and transient radio sources. The survey is designed to engage radio astronomy experts, multi-wavelength astronomers, and citizen scientists alike. By utilizing an “on the fly” interferometry mode, the observing overheads are much reduced compared to a conventional pointed survey. In this paper, we present the science case and observational strategy for the survey, and also results from early survey observations.

QUBIC: The Q & U Bolometric Interferometer for Cosmology

Journal of Low Temperature Physics Springer Science and Business Media LLC 199:1-2 (2020) 482-490

Authors:

Es Battistelli, P Ade, Jg Alberro, A Almela, G Amico, Lh Arnaldi, D Auguste, J Aumont, S Azzoni, S Banfi, P Battaglia, A Baù, B Bélier, D Bennett, L Bergé, J-Ph Bernard, M Bersanelli, M-A Bigot-Sazy, N Bleurvacq, J Bonaparte, J Bonis, A Bottani, E Bunn, D Burke, F Cavaliere

VLT/SINFONI study of black hole growth in high-redshift radio-loud quasars from the CARLA survey

Monthly Notices of the Royal Astronomical Society Oxford University Press (OUP) 492:2 (2020) 1991-2016

Authors:

M Marinello, RA Overzier, HJA Röttgering, JD Kurk, C De Breuck, J Vernet, D Wylezalek, D Stern, KJ Duncan, N Hatch, N Kashikawa, Y-T Lin, RS Nemmen, A Saxena

Reionization history constraints from neural network based predictions of high-redshift quasar continua

Monthly Notices of the Royal Astronomical Society Oxford University Press 493:3 (2020) 4256-4275

Authors:

D Ďurovčíková, H Katz, SEI Bosman, FB Davies, J Devriendt, A Slyz

Abstract:

Observations of the early Universe suggest that reionization was complete by z ∼ 6, however, the exact history of this process is still unknown. One method for measuring the evolution of the neutral fraction throughout this epoch is via observing the Lyα damping wings of high-redshift quasars. In order to constrain the neutral fraction from quasar observations, one needs an accurate model of the quasar spectrum around Lyα, after the spectrum has been processed by its host galaxy but before it is altered by absorption and damping in the intervening IGM. In this paper, we present a novel machine learning approach, using artificial neural networks, to reconstruct quasar continua around Lyα. Our QSANNDRA algorithm improves the error in this reconstruction compared to the state-of-the-art PCA-based model in the literature by 14.2% on average, and provides an improvement of 6.1% on average when compared to an extension thereof. In comparison with the extended PCA model, QSANNDRA further achieves an improvement of 22.1% and 16.8% when evaluated on low-redshift quasars most similar to the two high-redshift quasars under consideration, ULAS J1120+0641 at z = 7.0851 and ULAS J1342+0928 at z = 7.5413, respectively. Using our more accurate reconstructions of these two z > 7 quasars, we estimate the neutral fraction of the IGM using a homogeneous reionization model and find x¯H1=0.25+0.05−0.05 at z = 7.0851 and x¯H1=0.60+0.11−0.11 at z = 7.5413. Our results are consistent with the literature and favour a rapid end to reionization.