Simulated PLATO light curves Oxford 2025

(2026)

Abstract:

Simulated PLATO light curves generated at the University of Oxford in 2025. The light curves were used to test light curve filtering and transit detection algorithms. The light curves were generated in python using the PLATO Solar-like Light curve Simulator (PSLS), PySpot, and PyTransit codes. The data are primarily stored in feather files, which in python can be read using the pandas and pyarrow packages. Detailed information on the included files and contents are provided in the README file.

The Roasting Marshmallows Program with IGRINS on Gemini South. V. Atmosphere of MASCARA-1 b Is Enriched in Refractory Elements

Astronomical Journal 172:2 (2026)

Authors:

K Kanumalla, MR Line, M Chiarella, M Brogi, PCB Smith, JA Sanchez, Y Chachan, J Lothringer, JP Wardenier, H Beltz, C Saffe, EK Deibert, MW Mansfield, S Pelletier, V Parmentier, YH Choi, S Ramkumar, AB Savel, L Welbanks, JL Bean, V Panwar, TA Silva, L Pino, Y Hayashi, D Lim, CX Lu, VM Kalari, T Močnik, MG Rawlings, H Oh, RJ Diaz, C Park, JJ Lee, S Kim, U Jeong, HI Lee, W Park, Y Yu, Y Kim, MY Chun, JS Oh, S Lee, JG Jang, BH Jang, HC Seong, HJ Kim, CB Brooks, GN Mace, H Lee, JM Good, DT Jaffe, KM Kim, IS Yuk, N Hwang, BG Park, H Kim, B Chinn, F Ramos, P Prado, J White, A Olivares, V Oyarzun, E Kurz, H Stecher, C Quiroz, I Arriagada, TL Hayward, H Suh, J Miller, S Xu, EP Farina, C Figura, A Stephens, B Miller, K Labrie, P Hirst, E Tapia, Z Hartmann

Abstract:

Ultrahot Jupiters (UHJs; Teq ≳ 2000 K) enable simultaneous detection of volatile (ice-forming) and refractory (rock-forming) elements in planetary atmospheres, providing a powerful diagnostic of planet formation and atmospheric processing. We present a comprehensive high-resolution cross-correlation spectroscopy analysis of the UHJ MASCARA-1 b (Teq ≈ 2600 K) using the IGRINS and IGRINS-2 spectrographs. We detect robust (signal-to-noise ratio > 4) signals from H2O, CO, OH, Fe i, Mg i, Ca i, and Ti i, marking the most complete atmospheric inventory of MASCARA-1 b to date. Using a chemically consistent atmospheric inference framework, we constrain elemental abundances to a typical precision of ≈0.2 dex, retrieving a solar atmospheric metallicity ([M/H] (Formula presented) =0.07−0.13+0.17 ≈1.2 × solar), a C/O ratio (C/O (Formula presented) =0.65−0.08+0.08 ) consistent with solar value (C/O = 0.59), an enhanced refractory abundance ([ (Formula presented) R /H]= (Formula presented) 0.40−0.17+0.23≈2.5× solar; ≈3.8 × stellar), and a moderately supersolar refractory-to-volatile ratio ([ (Formula presented) R/V ] =  (Formula presented) 0.36−0.09+0.11 ≈ 2.3× solar). Comparison with formation models suggests that MASCARA-1 b most likely accreted material between the soot–H2O or H2O–CO snowlines (at 68% confidence). We additionally find stellar values for atmospheric Ti/Fe and Ca/Fe ratios (at 68% confidence). The Mg/Fe is also found to be consistent with stellar value at 95% confidence. Therefore, we do not find strong indication of nightside cold trapping in MASCARA-1 b. As homogeneous refractory-to-volatile measurements expand across the UHJ population, particularly with upcoming Extremely Large Telescopes, these diagnostics will enable statistically robust tests of emerging trends in giant planet formation and atmospheric evolution.

Direct Imaging Discovery of Giant Exoplanet β Pictoris d: A Decade-long Game of Hide-and-seek

The Astrophysical Journal Letters American Astronomical Society 1006:1 (2026) l10

Authors:

Ben J Sutlieff, Markus J Bonse, Valentin Christiaens, Clémence Fontanive, Elisabeth C Matthews, Luke T Parker, Tim D Pearce, Jayne L Birkby, Beth A Biller, Trent J Dupuy, Emily O Garvin, Leyla Iskandarli, Jens Kammerer, Yifan Zhou, Robert J De Rosa, Aarynn L Carter, Sasha Hinkley, Matthew A Kenworthy, William O Balmer, Iain Hammond, James Mang, Caroline V Morley, Mark J Neeser, Olivier Absil, Anthony Boccaletti, Mariangela Bonavita, Brendan P Bowler, Xueqing Chen, Felix A Dannert, Julien H Girard, Markus Kasper, Anne-Marie Lagrange, Pengyu Liu, Gilles Orban de Xivry, Michael Poon, Sascha P Quanz, Benoît Serra, Johanna M Vos, Kevin Wagner, Jason Wang, Bernhard Schölkopf, Guido Agapito, Alex Agudo Berbel, Dániel Apai, Andrea Baruffolo, Martin Black, Marco Bonaglia, Runa Briguglio, Yixian Cao, Luca Carbonaro, Lee Chapman, Giovanni Cresci, Yigit Dallilar, Richard Davies, Matthias Deysenroth, Ivan Di Antonio, Amico Di Cianno, Gianluca Di Rico, David Doelman, Mauro Dolci, Frank Eisenhauer, Simone Esposito, Debora Ferruzzi, Helmut Feuchtgruber, Natascha Förster-Schreiber, Kyle Franson, Reinhard Genzel, Stefan Gillessen, Eileen C Gonzales, Michael Hartl, Jean Hayoz, Heinrich Huber, Christoph Keller, Kateryna Kravchenko, Jarron Leisenring, John Lightfoot, David Lunney, Dieter Lutz, Mike Macintosh, Filippo Mannucci, Stanimir Metchev, Thomas Ott, David Pearson, Alfio Puglisi, Sebastian Rabien, Christian Rau, Armando Riccardi, Bernardo Salasnich, Taro Shimizu, Frans Snik, Eckhard Sturm, Genaro Suárez, Linda Tacconi, Xianyu Tan, William Taylor, Christopher Waring, Marco Xompero

Abstract:

We report the direct imaging discovery of a third exoplanet in the β Pictoris (β Pic) system. We detect β Pictoris d (β Pic d) in noncoronagraphic observations obtained with the Very Large Telescope (VLT) Enhanced Resolution Imager and Spectrograph (ERIS), as well as multi-epoch archival datasets from the JWST Near Infrared Camera (NIRCam) and VLT/SPHERE. Astrometric measurements over an 11 yr baseline demonstrate that it is consistent with a gravitationally bound source with orbital motion. Joint multi-planet orbit fits of all three planets in the system yield a semimajor axis of 26.0−6.1+2.2 au and inclination 89.0−0.6+0.7 deg for planet d. β Pic d has a larger orbital semimajor axis than the other known planets in the system, but is coplanar with the inner two planets, and its orbit is consistent with sculpting the inner edge of the debris disk. β Pic d has a contrast of ΔL′=12.11±0.15 mag, with colors and luminosity that closely match those of 51 Eri b, another exoplanet in the β Pic moving group. Its VLT/ERIS and JWST/NIRCam colors are distinct from those of free-floating planetary-mass objects of a similar age and temperature. Its red F410M − F444W color indicates strong CO2 absorption in its atmosphere and suggests significant enhancement in metals compared to free-floating objects. From the ATMO hot-start evolutionary models, we estimate an effective temperature of 600−60+45 K and mass of 2.4 ± 0.6 MJup, which also closely matches similar estimates for 51 Eri b. β Pic d is among the lowest-mass exoplanets imaged from the ground. This discovery highlights the deep sensitivity achievable with ground-based imaging in the mid-infrared and the discovery potential of future high-contrast observations with the Extremely Large Telescope.

Glossy Silicate Clouds on the Scorched Dayside of LTT9779b

Astrophysical Journal Letters 1005:2 (2026)

Authors:

S Saha, JS Jenkins, J Brande, R Ashtari, IJM Crossfield, S Stamer, D Dragomir, KB Stevenson, V Parmentier, TM Evans-Soma, T Daylan, H Beltz, E Esparza-Borges

Abstract:

Discovered deep within the “Neptunian desert,” LTT9779b remains the only known ultrahot Neptune, prompting significant speculation regarding its unique formation and evolutionary history. Its exceptionally high geometric albedo has previously been attributed either to the presence of clouds or to an extremely metal-rich atmosphere. Here, we present a comprehensive panchromatic analysis of its dayside atmosphere using JWST NIRISS and NIRSpec/G395H observations to characterize its atmospheric structure and composition. Leveraging the exceptional signal-to-noise ratio (SNR) in the observed spectra, we report a 3σ-to-5σ detection of dayside clouds, with strong evidence for Mg2SiO4(s) (silicate) condensation. This constitutes the first statistically significant detection of clouds on the dayside of a Neptunian-mass exoplanet. We demonstrate that a highly reflective cloud deck, rather than an extremely high-metallicity atmosphere, is the most likely explanation for the planet’s anomalously high optical albedo. Furthermore, our atmospheric retrievals yield robust detections of both CO (∼4.88σ) and CO2 (∼8.76σ), while providing tentative constraints on the H2O abundance and upper limits on SiO, TiO, and VO. Finally, our analysis places a robust constraint on the C/O ratio of 0.984 ± 0.019. This aligns LTT9779b with other known ultrahot Jupiters exhibiting supersolar C/O ratios, suggesting a broader trend driven by the sequestration of oxygen-bearing condensates in ultrahot atmospheres.

Spin–Orbit Geometry of AU Mic b and c from Back-to-back Transits Observed Contemporaneously with Magellan PFS, LCOGT, and CHEOPS

The Astrophysical Journal Letters American Astronomical Society 1005:1 (2026) l25

Authors:

Zitao Lin, Gyula M Szabó, Krzysztof Sz Zieliński, Zhen Guo, Zoltán Garai, R Paul Butler, Alexis Brandeker, Johanna K Teske, Davide Gandolfi, Haochuan Yu, Nicolas Billot, Suzanne Aigrain, Michael Cretignier, Liang Wang, Xuan Mao, Wei M Yuan, Hongpeng Lu, Jiayin Li, Yann Alibert, Ádám Boldog, Vincent Bourrier, Giovanni Bruno, Jeffrey D Crane, Fei Dai, Olivier DS Demangeon, Alexis Heitzmann, Zhecheng Hu, Pradip Karmakar, Levente Kriskovics, Monika Lendl, He Y Liu, Pierre FL Maxted, Hugh P Osborn, Gaetano Scandariato, Stephen A Shectman, Sérgio G Sousa, Soléne Ulmer-Moll, Mu-Tian Wang, Thomas G Wilson, Sharon X Wang

Abstract:

Young planets offer a unique window into the early stages of planetary evolution. AU Mic is one of the nearest (9.8 pc) pre-main-sequence stars (∼20 Myr), hosting two transiting Neptune-sized planets and a debris disk. Previous studies have shown that the rotations of the central star, the debris disk, and the inner planet b are all aligned, suggesting that the system has not undergone violent evolution. Here we report new Rossiter–McLaughlin measurements for both AU Mic b and c, which happened to transit back-to-back on 2024 August 24 and 25, using the Magellan Planet Finder Spectrograph, together with contemporaneous photometry from LCOGT and CHEOPS. We confirm the aligned orbit of AU Mic b (λb = 1∘ ± 12∘) and find two possible solutions for AU Mic c: we slightly favor an aligned solution (λc = −10∘ ± 16∘) but cannot rule out a polar solution ( λc=87∘−29∘+36∘ ). Broader considerations, including dynamical stability and transit possibility, also support the mutually aligned scenario. An unexpected stellar signal during ingress and the poor transit-timing variation predictions of AU Mic c prevent a precise constraint on its obliquity, and various attempts using chromatic spectral analyses fail to outperform simple data exclusion in mitigating stellar contamination. Our observation highlights the importance of understanding stellar activity across multiple timescales and channels when characterizing young, active systems. A robust solution for the AU Mic architecture will require either a better understanding of stellar activity or future observations fortuitously free from strong stellar contamination.