A practical guide to the analysis of non-response and attrition in longitudinal research using a real data example

International Journal of Behavioral Development SAGE Publications 43:1 (2019) 24-34

Authors:

Nora L Eisner, Aja L Murray, Manuel Eisner, Denis Ribeaud

K2-295 b and K2-237 b: Two Transiting Hot Jupiters

ACTA ASTRONOMICA 69:2 (2019) 135-158

Authors:

AMS Smith, Sz Csizmadia, D Gandolfi, S Albrecht, R Alonso, O Barragan, J Cabrera, WD Cochran, F Dai, H Deeg, Ph Eigmueller, M Endl, A Erikson, M Fridlund, A Fukui, S Grziwa, EW Guenther, AP Hatzes, D Hidalgo, T Hirano, J Korth, M Kuzuhara, J Livingston, N Narita, D Nespral, P Niraula, G Nowak, E Palle, M Paetzold, CM Persson, J Prieto-Arranz, H Rauer, S Redfield, I Ribas, V Van Eylen

Simulating radial velocity observations of trappist-1 with SPIRou

Monthly notices of the Royal Astronomical Society 488 5144

Authors:

Baptiste Klein, Jean-François Donati

Abstract:

We simulate a radial velocity (RV) follow-up of the TRAPPIST-1 system, a faithful representative of M dwarfs hosting transiting Earth-sized exoplanets to be observed with SPIRou in the months to come. We generate an RV curve containing the signature of the seven transiting TRAPPIST-1 planets and a realistic stellar activity curve statistically compatible with the light curve obtained with the K2 mission. We find a ±5 m s-1 stellar activity signal comparable in amplitude with the planet signal. Using various sampling schemes and white noise levels, we create time-series from which we estimate the masses of the seven planets. We find that the precision on the mass estimates is dominated by (i) the white noise level for planets c, f, and e and (ii) the stellar activity signal for planets b, d, and h. In particular, the activity signal completely outshines the RV signatures of planets d and h that remain undetected regardless of the RV curve sampling and level of white noise in the data set. We find that an RV follow-up of TRAPPIST-1 using SPIRou alone would likely result in an insufficient coverage of the rapidly evolving activity signal of the star, especially with bright-time observations only, making statistical methods such as Gaussian Process Regression hardly capable of firmly detecting planet f and accurately recovering the mass of planet g. In contrast, we show that using bi-site observations with good longitudinal complementary would allow for a more accurate filtering of the stellar activity RV signal.

Three-dimensional Circulation Driving Chemical Disequilibrium in WASP-43b

The Astrophysical Journal American Astronomical Society 869:2 (2018) 107

Authors:

João M Mendonça, Shang-min Tsai, Matej Malik, Simon L Grimm, Kevin Heng

Magma ascent in planetesimals: control by grain size

Earth and Planetary Science Letters Elsevier 507 (2018) 154-165

Authors:

T Lichtenberg, T Keller, Richard Katz, GJ Golabek, TV Gerya

Abstract:

Rocky planetesimals in the early solar system melted internally and evolved chemically due to radiogenic heating from 26Al. Here we quantify the parametric controls on magma genesis and transport using a coupled petrological and fluid mechanical model of reactive two-phase flow. We find the mean grain size of silicate minerals to be a key control on magma ascent. For grain sizes ≳1 mm, melt segregation produces distinct radial structure and chemical stratification. This stratification is most pronounced for bodies formed at around 1 Myr after formation of Ca, Al-rich inclusions. These findings suggest a link between the time and orbital location of planetesimal formation and their subsequent structural and chemical evolution. According to our models, the evolution of partially molten planetesimal interiors falls into two categories. In the magma ocean scenario, the whole interior of a planetesimal experiences nearly complete melting, which would result in turbulent convection and core–mantle differentiation by the rainfall mechanism. In the magma sill scenario, segregating melts gradually deplete the deep interior of the radiogenic heat source. In this case, magma may form melt-rich layers beneath a cool and stable lid, while core formation would proceed by percolation. Our findings suggest that grain sizes prevalent during the internal heating stage governed magma ascent in planetesimals. Regardless of whether evolution progresses toward a magma ocean or magma sill structure, our models predict that temperature inversions due to rapid 26Al redistribution are limited to bodies formed earlier than ≈1 Myr after CAIs. We find that if grain size was ≲1 mm during peak internal melting, only elevated solid–melt density contrasts (such as found for the reducing conditions in enstatite chondrite compositions) would allow substantial melt segregation to occur.