The MeerKAT telescope as a pulsar facility: System verification and early science results from MeerTime

Publications of the Astronomical Society of Australia Cambridge University Press 37 (2020) e028

Authors:

M Bailes, A Jameson, F Abbate, Ed Barr, Ndr Bhat, L Bondonneau, M Burgay, Sj Buchner, F Camilo, Dj Champion, I Cognard, Pb Demorest, Pcc Freire, T Gautam, M Geyer, Jm Griessmeier, L Guillemot, H Hu, F Jankowski, S Johnston, A Karastergiou, R Karuppusamy, D Kaur, Mj Keith, M Kramer, J Van Leeuwen, Me Lower, Y Maan, Ma McLaughlin, Bw Meyers, S Osłowski, Ls Oswald, A Parthasarathy, T Pennucci, B Posselt, A Possenti, Sm Ransom, Dj Reardon, A Ridolfi, Ctg Schollar, M Serylak, G Shaifullah, M Shamohammadi, Rm Shannon, C Sobey, X Song, R Spiewak, Ih Stairs, Bw Stappers, W Van Straten

Abstract:

We describe system verification tests and early science results from the pulsar processor (PTUSE) developed for the newly commissioned 64-dish SARAO MeerKAT radio telescope in South Africa. MeerKAT is a high-gain low-system temperature radio array that currently operates at 580-1 670 MHz and can produce tied-array beams suitable for pulsar observations. This paper presents results from the MeerTime Large Survey Project and commissioning tests with PTUSE. Highlights include observations of the double pulsar, pulse profiles from 34 millisecond pulsars (MSPs) from a single 2.5-h observation of the Globular cluster Terzan 5, the rotation measure of Ter5O, a 420-sigma giant pulse from the Large Magellanic Cloud pulsar PSR , and nulling identified in the slow pulsar PSR J0633-2015. One of the key design specifications for MeerKAT was absolute timing errors of less than 5 ns using their novel precise time system. Our timing of two bright MSPs confirm that MeerKAT delivers exceptional timing. PSR exhibits a jitter limit of whilst timing of PSR over almost 11 months yields an rms residual of 66 ns with only 4 min integrations. Our results confirm that the MeerKAT is an exceptional pulsar telescope. The array can be split into four separate sub-arrays to time over 1 000 pulsars per day and the future deployment of S-band (1 750-3 500 MHz) receivers will further enhance its capabilities.

Up to two billion times acceleration of scientific simulations with deep neural architecture search

CoRR abs/2001.08055 (2020)

Authors:

MF Kasim, D Watson-Parris, L Deaconu, S Oliver, P Hatfield, DH Froula, G Gregori, M Jarvis, S Khatiwala, J Korenaga, J Topp-Mugglestone, E Viezzer, SM Vinko

Abstract:

Computer simulations are invaluable tools for scientific discovery. However, accurate simulations are often slow to execute, which limits their applicability to extensive parameter exploration, large-scale data analysis, and uncertainty quantification. A promising route to accelerate simulations by building fast emulators with machine learning requires large training datasets, which can be prohibitively expensive to obtain with slow simulations. Here we present a method based on neural architecture search to build accurate emulators even with a limited number of training data. The method successfully accelerates simulations by up to 2 billion times in 10 scientific cases including astrophysics, climate science, biogeochemistry, high energy density physics, fusion energy, and seismology, using the same super-architecture, algorithm, and hyperparameters. Our approach also inherently provides emulator uncertainty estimation, adding further confidence in their use. We anticipate this work will accelerate research involving expensive simulations, allow more extensive parameters exploration, and enable new, previously unfeasible computational discovery.

Full orbital solution for the binary system in the northern Galactic disc microlensing event Gaia16aye⋆

Astronomy & Astrophysics EDP Sciences 633 (2020) a98

Authors:

Ł Wyrzykowski, P Mróz, KA Rybicki, M Gromadzki, Z Kołaczkowski, M Zieliński, P Zieliński, N Britavskiy, A Gomboc, K Sokolovsky, ST Hodgkin, L Abe, GF Aldi, A AlMannaei, G Altavilla, A Al Qasim, GC Anupama, S Awiphan, E Bachelet, V Bakış, S Baker, S Bartlett, P Bendjoya, K Benson, IF Bikmaev, G Birenbaum, N Blagorodnova, S Blanco-Cuaresma, S Boeva, AZ Bonanos, V Bozza, DM Bramich, I Bruni, RA Burenin, U Burgaz, T Butterley, HE Caines, DB Caton, S Calchi Novati, JM Carrasco, A Cassan, V Čepas, M Cropper, M Chruślińska, G Clementini, A Clerici, D Conti, M Conti, S Cross, F Cusano, G Damljanovic, A Dapergolas, G D’Ago, JHJ de Bruijne, M Dennefeld, VS Dhillon, M Dominik, J Dziedzic, O Erece, MV Eselevich, H Esenoglu, L Eyer, R Figuera Jaimes, SJ Fossey, AI Galeev, SA Grebenev, AC Gupta, AG Gutaev, N Hallakoun, A Hamanowicz, C Han, B Handzlik, JB Haislip, L Hanlon, LK Hardy, DL Harrison, HJ van Heerden, VL Hoette, K Horne, R Hudec, M Hundertmark, N Ihanec, EN Irtuganov, R Itoh, P Iwanek, MD Jovanovic, R Janulis, M Jelínek, E Jensen, Z Kaczmarek, D Katz, IM Khamitov, Y Kilic, J Klencki, U Kolb, G Kopacki, VV Kouprianov, K Kruszyńska, S Kurowski, G Latev, C-H Lee, S Leonini, G Leto, F Lewis, Z Li, A Liakos, SP Littlefair, J Lu, CJ Manser, S Mao, D Maoz, A Martin-Carrillo, JP Marais, M Maskoliūnas, JR Maund, PJ Meintjes, SS Melnikov, K Ment, P Mikołajczyk, M Morrell, N Mowlavi, D Moździerski, D Murphy, S Nazarov, H Netzel, R Nesci, C-C Ngeow, AJ Norton, EO Ofek, E Pakštienė, L Palaversa, A Pandey, E Paraskeva, M Pawlak, MT Penny, BE Penprase, A Piascik, JL Prieto, JKT Qvam, C Ranc, A Rebassa-Mansergas, DE Reichart, P Reig, L Rhodes, J-P Rivet, G Rixon, D Roberts, P Rosi, DM Russell, R Zanmar Sanchez, G Scarpetta, G Seabroke, BJ Shappee, R Schmidt, Y Shvartzvald, M Sitek, J Skowron, M Śniegowska, C Snodgrass, PS Soares, B van Soelen, ZT Spetsieri, A Stankevičiūtė, IA Steele, RA Street, J Strobl, E Strubble, H Szegedi, LM Tinjaca Ramirez, L Tomasella, Y Tsapras, D Vernet, S Villanueva, O Vince, J Wambsganss, IP van der Westhuizen, K Wiersema, D Wium, RW Wilson, A Yoldas, R Ya Zhuchkov, DG Zhukov, J Zdanavičius, S Zoła, A Zubareva

Evidence for Late-stage Eruptive Mass Loss in the Progenitor to SN2018gep, a Broad-lined Ic Supernova: Pre-explosion Emission and a Rapidly Rising Luminous Transient

The Astrophysical Journal American Astronomical Society 887:2 (2019) 169

Authors:

Anna YQ Ho, Daniel A Goldstein, Steve Schulze, David K Khatami, Daniel A Perley, Mattias Ergon, Avishay Gal-Yam, Alessandra Corsi, Igor Andreoni, Cristina Barbarino, Eric C Bellm, Nadia Blagorodnova, Joe S Bright, E Burns, S Bradley Cenko, Virginia Cunningham, Kishalay De, Richard Dekany, Alison Dugas, Rob P Fender, Claes Fransson, Christoffer Fremling, Adam Goldstein, Matthew J Graham, David Hale, Assaf Horesh, Tiara Hung, Mansi M Kasliwal, N Paul M Kuin, SR Kulkarni, Thomas Kupfer, Ragnhild Lunnan, Frank J Masci, Chow-Choong Ngeow, Peter E Nugent, Eran O Ofek, Maria T Patterson, Glen Petitpas, Ben Rusholme, Hanna Sai, Itai Sfaradi, David L Shupe, Jesper Sollerman, Maayane T Soumagnac, Yutaro Tachibana, Francesco Taddia, Richard Walters, Xiaofeng Wang, Yuhan Yao, Xinhan Zhang

Non-Gaussianity constraints using future radio continuum surveys and the multitracer technique

Monthly Notices of the Royal Astronomical Society Oxford University Press 492:1 (2019) 1513-1522

Authors:

Zahra Gomes, Stefano Camera, Matthew Jarvis, Catherine Hale, José Fonseca

Abstract:

Tighter constraints on measurements of primordial non-Gaussianity (PNG) will allow the differentiation of inflationary scenarios. The cosmic microwave background bispectrum – the standard method of measuring the local non-Gaussianity – is limited by cosmic variance. Therefore, it is sensible to investigate measurements of non-Gaussianity using the large-scale structure. This can be done by investigating the effects of non-Gaussianity on the power spectrum on large scales. In this study, we forecast the constraints on the local PNG parameter fNL that can be obtained with future radio surveys. We utilize the multitracer method that reduces the effect of cosmic variance and takes advantage of the multiple radio galaxy populations that are differently biased tracers of the same underlying dark matter distribution. Improvements on previous work include the use of observational bias and halo mass estimates, updated simulations, and realistic photometric redshift expectations, thus producing more realistic forecasts. Combinations of Square Kilometre Array simulations and radio observations were used as well as different redshift ranges and redshift bin sizes. It was found that in the most realistic case the 1σ error on fNL falls within the range 4.07–6.58, rivalling the tightest constraints currently available.