HARMONI first light spectroscopy for the ELT: geometrical calibration in the data reduction software

Proceedings of SPIE--the International Society for Optical Engineering SPIE, the international society for optics and photonics 11452 (2020) 114522t-114522t-16

Authors:

Laure Piqueras, Aurélien Jarno, Louise Friot-Giroux, Thomas Béchet, Javier Piqueras López, Arlette Pécontal, Johan Richard, Nicolas Bouché, Niranjan A Thatte, Matthias Tecza

HARMONI: Characterising the line-spread-function with a tunable Fabry-Pérot etalon

Proceedings of SPIE--the International Society for Optical Engineering SPIE, the international society for optics and photonics 11451 (2020) 114515w-114515w-6

Authors:

Darshan Kakkad, Matthias Tecza, Niranjan A Thatte, Javier Piqueras López, Harry Kendell

Automation and control of laser wakefield accelerators using Bayesian optimization

Nature Communications Nature Research 11:1 (2020) 6355

Authors:

Rj Shalloo, Sjd Dann, J-N Gruse, Cid Underwood, Af Antoine, C Arran, M Backhouse, Cd Baird, Md Balcazar, N Bourgeois, Ja Cardarelli, Peter Hatfield, J Kang, K Krushelnick, Spd Mangles, Cd Murphy, N Lu, J Osterhoff, K Põder, Pp Rajeev, Cp Ridgers, S Rozario, Mp Selwood, Aj Shahani, Dr Symes, Agr Thomas, C Thornton, Z Najmudin, Mjv Streeter

Abstract:

Laser wakefield accelerators promise to revolutionize many areas of accelerator science. However, one of the greatest challenges to their widespread adoption is the difficulty in control and optimization of the accelerator outputs due to coupling between input parameters and the dynamic evolution of the accelerating structure. Here, we use machine learning techniques to automate a 100 MeV-scale accelerator, which optimized its outputs by simultaneously varying up to six parameters including the spectral and spatial phase of the laser and the plasma density and length. Most notably, the model built by the algorithm enabled optimization of the laser evolution that might otherwise have been missed in single-variable scans. Subtle tuning of the laser pulse shape caused an 80% increase in electron beam charge, despite the pulse length changing by just 1%.

MIGHTEE: Are giant radio galaxies more common than we thought?

(2020)

Authors:

J Delhaize, I Heywood, M Prescott, MJ Jarvis, I Delvecchio, IH Whittam, SV White, MJ Hardcastle, CL Hale, J Afonso, Y Ao, M Brienza, M Brueggen, JD Collier, E Daddi, M Glowacki, N Maddox, LK Morabito, I Prandoni, Z Randriamanakoto, S Sekhar, Fangxia An, NJ Adams, S Blyth, RAA Bowler, L Leeuw, L Marchetti, SM Randriamampandry, K Thorat, N Seymour, O Smirnov, AR Taylor, C Tasse, M Vaccari

Dual effects of ram pressure on star formation in multiphase disk galaxies with strong stellar feedback

Astrophysical Journal IOP Science 905:1 (2020) 31

Authors:

Jaehyun Lee, Taysun Kimm, Harley Katz, Joakim Rosdahl, Julien Devriendt, Adrianne Slyz

Abstract:

We investigate the impact of ram pressure stripping due to the intracluster medium (ICM) on star-forming disk galaxies with a multiphase interstellar medium maintained by strong stellar feedback. We carry out radiation-hydrodynamic simulations of an isolated disk galaxy embedded in a 1011 M ⊙ dark matter halo with various ICM winds mimicking the cluster outskirts (moderate) and the central environment (strong). We find that both star formation quenching and triggering occur in ram pressure–stripped galaxies, depending on the strength of the winds. H i and H2 in the outer galactic disk are significantly stripped in the presence of moderate winds, whereas turbulent pressure provides support against ram pressure in the central region, where star formation is active. Moderate ICM winds facilitate gas collapse, increasing the total star formation rates by ~40% when the wind is oriented face-on or by ~80% when it is edge-on. In contrast, strong winds rapidly blow away neutral and molecular hydrogen gas from the galaxy, suppressing star formation by a factor of 2 within ~200 Myr. Dense gas clumps with n H gsim 10 M ⊙ pc−2 are easily identified in extraplanar regions, but no significant young stellar populations are found in such clumps. In our attempts to enhance radiative cooling by adopting a colder ICM of T = 106 K, only a few additional stars are formed in the tail region, even if the amount of newly cooled gas increases by an order of magnitude.