Cesam2k20: A code for a new generation of stellar evolution models I. Description of the code L. Manchon, M. Deal, J. P. C. Marques, Y. Lebreton Astronomy and Astrophysics, 2025 We present Cesam2k20, the latest version of the hydrostatic stellar evolution code CESAM originally developed by P. Morel and collaborators. Over the last three decades, it has undergone many improvements and has been extensively tested against other stellar evolution codes before being selected to compute the first-generation grid of stellar models for the PLATO mission. Among all the developments made thus far, Cesam2k20 now implements state-of-the-art models for the transport of chemical elements and angular momentum. It was recently made publicly available with an ecosystem of other codes interfaced with it: 1D and 2D oscillation codes ADIPLS and ACOR, optimisation program OSM, and Python utility package pycesam . This paper recalls the numerical peculiarities of Cesam2k20, namely, the use of a collocation method where the structure variables are decomposed as piecewise polynomials projected on a B-spline basis. Here, we review the options available for modelling the different physical processes. In particular, we illustrate the improvements made in the transport of chemical elements and angular momentum with a series of standard and non-standard solar models.
The efficiency of mixed modes for angular momentum transport B. Bordadágua, F. Ahlborn, Q. Coppée, J.P. Marques, K. Belkacem, S. Hekker Astronomy and Astrophysics, 2025 Core rotation rates of red giant stars inferred from asteroseismic observations are substantially lower than ones predicted by current stellar models. This indicates the lack of an efficient angular momentum transport mechanism in radiative interiors. Mixed pressure-gravity modes are a promising candidate to extract angular momentum from the core of red giants. We focus on determining the effect of mixed modes on the rotation rates of stars evolving along the red giant branch (RGB). We developed a post-processing code that computes the angular momentum transport by meridional currents, shear-induced turbulence, and mixed modes. Rotation rates were computed for models along the RGB with different stellar masses and different initial rotation profiles. We find that the mixed modes can explain some of the spin-down observed in red giant stars; however, the values of non-radial mode amplitudes strongly affect the efficiency of this mechanism. Rotation rates from models neglecting radiative damping on the mixed mode amplitudes overlap with observations and produce a localised spin-down around the hydrogen-burning shell, whereas the inclusion of radiative damping strongly suppresses and delays this spin-down. We also show that including an additional viscosity term with values in the range of $10^3-10^4; cm s $ redistributes the localised spin-down due to the mixed modes, enhancing their efficiency. Our results reveal that the mixed mode amplitudes need to be constrained to precisely quantify the spin-down of red giant cores. Nevertheless, the mixed mode mechanism by itself cannot explain the full spread in observed core rotation rates along the RGB. This will only be possible with an additional mechanism for angular momentum transport.
The PLATO mission Heike Rauer, Conny Aerts, Juan Cabrera, Magali Deleuil, Anders Erikson, Laurent Gizon, Mariejo Goupil, Ana Heras, Thomas Walloschek, Jose Lorenzo-Alvarez, Filippo Marliani, César Martin-Garcia, J. Miguel Mas-Hesse, Laurence O’Rourke, Hugh Osborn, Isabella Pagano, Giampaolo Piotto, Don Pollacco, Roberto Ragazzoni, Gavin Ramsay, Stéphane Udry, Thierry Appourchaux, Willy Benz, Alexis Brandeker, Manuel Güdel, Eduardo Janot-Pacheco, Petr Kabath, Hans Kjeldsen, Michiel Min, Nuno Santos, Alan Smith, Juan-Carlos Suarez, Stephanie C. Werner, Alessio Aboudan, Manuel Abreu, Lorena Acuña, Moritz Adams, Vardan Adibekyan, Laura Affer, François Agneray, Craig Agnor, Victor Aguirre Børsen-Koch, Saad Ahmed, Suzanne Aigrain, Ashraf Al-Bahlawan, Ma de los Angeles Alcacera Gil, Eleonora Alei, Silvia Alencar, Richard Alexander, Julia Alfonso-Garzón, Yann Alibert, Carlos Allende Prieto, Leonardo Almeida, Roi Alonso Sobrino, Giuseppe Altavilla, Christian Althaus, Luis Alonso Alvarez Trujillo, Anish Amarsi, Matthias Ammler-von Eiff, Eduardo Amôres, Laerte Andrade, Alexandros Antoniadis-Karnavas, Carlos António, Beatriz Aparicio del Moral, Matteo Appolloni, Claudio Arena, David Armstrong, Jose Aroca Aliaga, Martin Asplund, Jeroen Audenaert, Natalia Auricchio, Pedro Avelino, Ann Baeke, Kevin Baillié, Ana Balado, Pau Ballber Balagueró, Andrea Balestra, Warrick Ball, Herve Ballans, Jerome Ballot, Caroline Barban, Gaële Barbary, Mauro Barbieri, Sebastià Barceló Forteza, Adrian Barker, Paul Barklem, Sydney Barnes, David Barrado Navascues, Oscar Barragan, Clément Baruteau, Sarbani Basu, Frederic Baudin, Philipp Baumeister, Daniel Bayliss, Michael Bazot, Paul G. Beck, Kevin Belkacem, Earl Bellinger, Serena Benatti, Othman Benomar, Diane Bérard, Maria Bergemann, Maria Bergomi, Pierre Bernardo, Katia Biazzo, Andrea Bignamini, Lionel Bigot, Nicolas Billot, Martin Binet, David Biondi, Federico Biondi, Aaron C. Birch, Bertram Bitsch, Paz Victoria Bluhm Ceballos, Attila Bódi, Zsófia Bognár, Isabelle Boisse, Emeline Bolmont, Alfio Bonanno, Mariangela Bonavita, Andrea Bonfanti, Xavier Bonfils, Rosaria Bonito, Aldo Stefano Bonomo, Anko Börner, Sudeshna Boro Saikia, Elisa Borreguero Martín, Francesco Borsa, Luca Borsato, Diego Bossini, Francois Bouchy, Gwenaël Boué, Rodrigo Boufleur, Patrick Boumier, Vincent Bourrier, Dominic M. Bowman, Enrico Bozzo, Louisa Bradley, John Bray, Alessandro Bressan, Sylvain Breton, Daniele Brienza, Ana Brito, Matteo Brogi, Beverly Brown, David J. A. Brown, Allan Sacha Brun, Giovanni Bruno, Michael Bruns, Lars A. Buchhave, Lisa Bugnet, Gaël Buldgen, Patrick Burgess, Andrea Busatta, Giorgia Busso, Derek Buzasi, José A. Caballero, Alexandre Cabral, Juan-Francisco Cabrero Gomez, Flavia Calderone, Robert Cameron, Andrew Cameron, Tiago Campante, Néstor Campos Gestal, Bruno Leonardo Canto Martins, Christophe Cara, Ludmila Carone, Josep Manel Carrasco, Luca Casagrande, Sarah L. Casewell, Santi Cassisi, Marco Castellani, Matthieu Castro, Claude Catala, Irene Catalán Fernández, Márcio Catelan, Heather Cegla, Chiara Cerruti, Virginie Cessa, Merieme Chadid, William Chaplin, Stephane Charpinet, Cristina Chiappini, Simone Chiarucci, Andrea Chiavassa, Simonetta Chinellato, Giovanni Chirulli, Jørgen Christensen-Dalsgaard, Ross Church, Antonio Claret, Cathie Clarke, Riccardo Claudi, Lionel Clermont, Hugo Coelho, Joao Coelho, Fabrizio Cogato, Josep Colomé, Mathieu Condamin, Fernando Conde García, Simon Conseil, Thierry Corbard, Alexandre C. M. Correia, Enrico Corsaro, Rosario Cosentino, Jean Costes, Andrea Cottinelli, Giovanni Covone, Orlagh L. Creevey, Aurelien Crida, Szilard Csizmadia, Margarida Cunha, Patrick Curry, Jefferson da Costa, Francys da Silva, Shweta Dalal, Mario Damasso, Cilia Damiani, Francesco Damiani, Maria Liduina das Chagas, Melvyn Davies, Guy Davies, Ben Davies, Gary Davison, Leandro de Almeida, Francesca de Angeli, Susana Cristina Cabral de Barros, Izan de CastroLeão, Daniel Brito de Freitas, Marcia Cristina de Freitas, Domitilla De Martino, José Renan de Medeiros, Luiz Alberto de Paula, Álvaro de Pedraza Gómez, Jelle de Plaa, Joris De Ridder, Morgan Deal, Leen Decin, Hans Deeg, Scilla Degl’Innocenti, Sebastien Deheuvels, Carlos del Burgo, Fabio Del Sordo, Elisa Delgado-Mena, Olivier Demangeon, Tilmann Denk, Aliz Derekas, Jean-Michel Desert, Silvano Desidera, Marc Dexet, Marcella Di Criscienzo, Anna Maria Di Giorgio, Maria Pia Di Mauro, Federico Jose Diaz Rial, José-Javier Díaz-García, Marco Dima, Giacomo Dinuzzi, Odysseas Dionatos, Elisa Distefano, Jose-Dias do Nascimento, Albert Domingo, Valentina D’Orazi, Caroline Dorn, Lauren Doyle, Elena Duarte, Florent Ducellier, Luc Dumaye, Xavier Dumusque, Marc-Antoine Dupret, Patrick Eggenberger, David Ehrenreich, Philipp Eigmüller, Johannes Eising, Marcelo Emilio, Kjell Eriksson, Marco Ermocida, Riano Isidoro Escate Giribaldi, Yoshi Eschen, Lucía Espinosa Yáñez, Inês Estrela, Dafydd Wyn Evans, Damian Fabbian, Michele Fabrizio, João Pedro Faria, Maria Farina, Jacopo Farinato, Dax Feliz, Sofia Feltzing, Thomas Fenouillet, Miguel Fernández, Lorenza Ferrari, Sylvio Ferraz-Mello, Fabio Fialho, Agnes Fienga, Pedro Figueira, Laura Fiori, Ettore Flaccomio, Mauro Focardi, Steve Foley, Jean Fontignie, Dominic Ford, Karin Fornazier, Thierry Forveille, Luca Fossati, Rodrigo de Marca Franca, Lucas Franco da Silva, Antonio Frasca, Malcolm Fridlund, Marco Furlan, Sarah-Maria Gabler, Marco Gaido, Andrew Gallagher, Paloma I. Gallego Sempere, Emanuele Galli, Rafael A. García, Antonio García Hernández, Antonio Garcia Munoz, Hugo García-Vázquez, Rafael Garrido Haba, Patrick Gaulme, Nicolas Gauthier, Charlotte Gehan, Matthew Gent, Iskra Georgieva, Mauro Ghigo, Edoardo Giana, Samuel Gill, Leo Girardi, Silvia Giuliatti Winter, Giovanni Giusi, João Gomes da Silva, Luis Jorge Gómez Zazo, Juan Manuel Gomez-Lopez, Jonay Isai González Hernández, Kevin Gonzalez Murillo, Alejandro Gonzalo Melchor, Nicolas Gorius, Pierre-Vincent Gouel, Duncan Goulty, Valentina Granata, John Lee Grenfell, Denis Grießbach, Emmanuel Grolleau, Salomé Grouffal, Sascha Grziwa, Mario Giuseppe Guarcello, Loïc Gueguen, Eike Wolf Guenther, Terrasa Guilhem, Lucas Guillerot, Tristan Guillot, Pierre Guiot, Pascal Guterman, Antonio Gutiérrez, Fernando Gutiérrez-Canales, Janis Hagelberg, Jonas Haldemann, Cassandra Hall, Rasmus Handberg, Ian Harrison, Diana L. Harrison, Johann Hasiba, Carole A. Haswell, Petra Hatalova, Artie Hatzes, Raphaelle Haywood, Guillaume Hébrard, Frank Heckes, Ulrike Heiter, Saskia Hekker, René Heller, Christiane Helling, Krzysztof Helminiak, Simon Hemsley, Kevin Heng, Konstantin Herbst, Aline Hermans, JJ Hermes, Nadia Hidalgo Torres, Natalie Hinkel, David Hobbs, Simon Hodgkin, Karl Hofmann, Saeed Hojjatpanah, Günter Houdek, Daniel Huber, Joseph Huesler, Alain Hui-Bon-Hoa, Rik Huygen, Duc-Dat Huynh, Nicolas Iro, Jonathan Irwin, Mike Irwin, André Izidoro, Sophie Jacquinod, Nicholas Emborg Jannsen, Markus Janson, Harald Jeszenszky, Chen Jiang, Antonio José Jimenez Mancebo, Paula Jofre, Anders Johansen, Cole Johnston, Geraint Jones, Thomas Kallinger, Szilárd Kálmán, Thomas Kanitz, Marie Karjalainen, Raine Karjalainen, Christoffer Karoff, Steven Kawaler, Daisuke Kawata, Arnoud Keereman, David Keiderling, Tom Kennedy, Matthew Kenworthy, Franz Kerschbaum, Mark Kidger, Flavien Kiefer, Christian Kintziger, Kristina Kislyakova, László Kiss, Peter Klagyivik, Hubert Klahr, Jonas Klevas, Oleg Kochukhov, Ulrich Köhler, Ulrich Kolb, Alexander Koncz, Judith Korth, Nadiia Kostogryz, Gábor Kovács, József Kovács, Oleg Kozhura, Natalie Krivova, Arūnas Kuĉinskas, Ilyas Kuhlemann, Friedrich Kupka, Wouter Laauwen, Alvaro Labiano, Nadege Lagarde, Philippe Laget, Gunter Laky, Kristine Wai Fun Lam, Michiel Lambrechts, Helmut Lammer, Antonino Francesco Lanza, Alessandro Lanzafame, Mariel Lares Martiz, Jacques Laskar, Henrik Latter, Tony Lavanant, Alastair Lawrenson, Cecilia Lazzoni, Agnes Lebre, Yveline Lebreton, Alain Lecavelier des Etangs, Katherine Lee, Zoe Leinhardt, Adrien Leleu, Monika Lendl, Giuseppe Leto, Yves Levillain, Anne-Sophie Libert, Tim Lichtenberg, Roxanne Ligi, Francois Lignieres, Jorge Lillo-Box, Jeffrey Linsky, John Scige Liu, Dominik Loidolt, Yuying Longval, Ilídio Lopes, Andrea Lorenzani, Hans-Guenter Ludwig, Mikkel Lund, Mia Sloth Lundkvist, Xavier Luri, Carla Maceroni, Sean Madden, Nikku Madhusudhan, Antonio Maggio, Christian Magliano, Demetrio Magrin, Laurent Mahy, Olaf Maibaum, LeeRoy Malac-Allain, Jean-Christophe Malapert, Luca Malavolta, Jesus Maldonado, Elena Mamonova, Louis Manchon, Andres Manjón, Andrew Mann, Giacomo Mantovan, Luca Marafatto, Marcella Marconi, Rosemary Mardling, Paola Marigo, Silvia Marinoni, Rico Marques, Joao Pedro Marques, Paola Maria Marrese, Douglas Marshall, Silvia Martínez Perales, David Mary, Francesco Marzari, Eduard Masana, Andrina Mascher, Stéphane Mathis, Savita Mathur, Iris Martín Vodopivec, Ana Carolina Mattiuci Figueiredo, Pierre F. L. Maxted, Tsevi Mazeh, Stephane Mazevet, Francesco Mazzei, James McCormac, Paul McMillan, Lucas Menou, Thibault Merle, Farzana Meru, Dino Mesa, Sergio Messina, Szabolcs Mészáros, Nadége Meunier, Jean-Charles Meunier, Giuseppina Micela, Harald Michaelis, Eric Michel, Mathias Michielsen, Tatiana Michtchenko, Andrea Miglio, Yamila Miguel, David Milligan, Giovanni Mirouh, Morgan Mitchell, Nuno Moedas, Francesca Molendini, László Molnár, Joey Mombarg, Josefina Montalban, Marco Montalto, Mário J. P. F. G. Monteiro, Francisco Montoro Sánchez, Juan Carlos Morales, Maria Morales-Calderon, Alessandro Morbidelli, Christoph Mordasini, Chrystel Moreau, Thierry Morel, Giuseppe Morello, Julien Morin, Annelies Mortier, Benoît Mosser, Denis Mourard, Olivier Mousis, Claire Moutou, Nami Mowlavi, Andrés Moya, Prisca Muehlmann, Philip Muirhead, Matteo Munari, Ilaria Musella, Alexander James Mustill, Nicolas Nardetto, Domenico Nardiello, Norio Narita, Valerio Nascimbeni, Anna Nash, Coralie Neiner, Richard P. Nelson, Nadine Nettelmann, Gianalfredo Nicolini, Martin Nielsen, Sami-Matias Niemi, Lena Noack, Arlette Noels-Grotsch, Anthony Noll, Azib Norazman, Andrew J. Norton, Benard Nsamba, Aviv Ofir, Gordon Ogilvie, Terese Olander, Christian Olivetto, Göran Olofsson, Joel Ong, Sergio Ortolani, Mahmoudreza Oshagh, Harald Ottacher, Roland Ottensamer, Rhita-Maria Ouazzani, Sijme-Jan Paardekooper, Emanuele Pace, Miriam Pajas, Ana Palacios, Gaelle Palandri, Enric Palle, Carsten Paproth, Vanderlei Parro, Hannu Parviainen, Javier Pascual Granado, Vera Maria Passegger, Carmen Pastor-Morales, Martin Pätzold, May Gade Pedersen, David Pena Hidalgo, Francesco Pepe, Filipe Pereira, Carina M. Persson, Martin Pertenais, Gisbert Peter, Antoine C. Petit, Pascal Petit, Stefania Pezzuto, Gabriele Pichierri, Adriano Pietrinferni, Fernando Pinheiro, Marc Pinsonneault, Emese Plachy, Philippe Plasson, Bertrand Plez, Katja Poppenhaeger, Ennio Poretti, Elisa Portaluri, Jordi Portell, Gustavo Frederico Porto de Mello, Julien Poyatos, Francisco J. Pozuelos, Pier Giorgio Prada Moroni, Dumitru Pricopi, Loredana Prisinzano, Matthias Quade, Andreas Quirrenbach, Julio Arturo Rabanal Reina, Maria Cristina Rabello Soares, Gabriella Raimondo, Monica Rainer, Jose Ramón Rodón, Alejandro Ramón-Ballesta, Gonzalo Ramos Zapata, Stefanie Rätz, Christoph Rauterberg, Bob Redman, Ronald Redmer, Daniel Reese, Sara Regibo, Ansgar Reiners, Timo Reinhold, Christian Renie, Ignasi Ribas, Sergio Ribeiro, Thiago Pereira Ricciardi, Ken Rice, Olivier Richard, Marco Riello, Michel Rieutord, Vincenzo Ripepi, Guy Rixon, Steve Rockstein, José Ramón Rodón Ortiz, María Teresa Rodrigo Rodríguez, Alberto Rodríguez Amor, Luisa Fernanda Rodríguez Díaz, Juan Pablo Rodriguez Garcia, Julio Rodriguez-Gomez, Yannick Roehlly, Fernando Roig, Bárbara Rojas-Ayala, Tobias Rolf, Jakob Lysgaard Rørsted, Hugo Rosado, Giovanni Rosotti, Olivier Roth, Markus Roth, Alex Rousseau, Ian Roxburgh, Fabrice Roy, Pierre Royer, Kirk Ruane, Sergio Rufini Mastropasqua, Claudia Ruiz de Galarreta, Andrea Russi, Steven Saar, Melaine Saillenfest, Maurizio Salaris, Sebastien Salmon, Ippocratis Saltas, Réza Samadi, Aunia Samadi, Dominic Samra, Tiago Sanches da Silva, Miguel Andrés Sánchez Carrasco, Alexandre Santerne, Amaia Santiago Pé, Francesco Santoli, Ängela R. G. Santos, Rosario Sanz Mesa, Luis Manuel Sarro, Gaetano Scandariato, Martin Schäfer, Edward Schlafly, François-Xavier Schmider, Jean Schneider, Jesper Schou, Hannah Schunker, Gabriel Jörg Schwarzkopf, Aldo Serenelli, Dries Seynaeve, Yutong Shan, Alexander Shapiro, Russel Shipman, Daniela Sicilia, Maria Angeles Sierra sanmartin, Axelle Sigot, Kyle Silliman, Roberto Silvotti, Attila E. Simon, Ricardo Simoyama Napoli, Marek Skarka, Barry Smalley, Rodolfo Smiljanic, Samuel Smit, Alexis Smith, Leigh Smith, Ignas Snellen, Ádám Sódor, Frank Sohl, Sami K. Solanki, Francesca Sortino, Sérgio Sousa, John Southworth, Diogo Souto, Alessandro Sozzetti, Dimitris Stamatellos, Keivan Stassun, Manfred Steller, Dennis Stello, Beate Stelzer, Ulrike Stiebeler, Amalie Stokholm, Trude Storelvmo, Klaus Strassmeier, Paul Anthony Strøm, Antoine Strugarek, Sophia Sulis, Michal Švanda, László Szabados, Róbert Szabó, Gyula M. Szabó, Ewa Szuszkiewicz, Geert Jan Talens, Daniele Teti, Tom Theisen, Frédéric Thévenin, Anne Thoul, Didier Tiphene, Ruth Titz-Weider, Andrew Tkachenko, Daniel Tomecki, Jorge Tonfat, Nicola Tosi, Regner Trampedach, Gregor Traven, Amaury Triaud, Reidar Trønnes, Maria Tsantaki, Matthias Tschentscher, Arnaud Turin, Adam Tvaruzka, Bernd Ulmer, Solène Ulmer-Moll, Ceren Ulusoy, Gabriele Umbriaco, Diana Valencia, Marica Valentini, Adriana Valio, Ángel Luis Valverde Guijarro, Vincent Van Eylen, Valerie Van Grootel, Tim A. van Kempen, Timothy Van Reeth, Iris Van Zelst, Bart Vandenbussche, Konstantinos Vasiliou, Valeriy Vasilyev, David Vaz de Mascarenhas, Allona Vazan, Marina Vela Nunez, Eduardo Nunes Velloso, Rita Ventura, Paolo Ventura, Julia Venturini, Isabel Vera Trallero, Dimitri Veras, Eva Verdugo, Kuldeep Verma, Didier Vibert, Tobias Vicanek Martinez, Krisztián Vida, Arthur Vigan, Antonio Villacorta, Eva Villaver, Marcos Villaverde Aparicio, Valentina Viotto, Eduard Vorobyov, Sergey Vorontsov, Frank W. Wagner, Nicholas Walton, Dave Walton, Haiyang Wang, Rens Waters, Christopher Watson, Sven Wedemeyer, Angharad Weeks, Jörg Weingrill, Annita Weiss, Belinda Wendler, Richard West, Karsten Westerdorff, Pierre-Amaury Westphal, Peter Wheatley, Tim White, Amadou Whittaker, Kai Wickhusen, Thomas Wilson, James Windsor, Othon Winter, Mark Lykke Winther, Alistair Winton, Ulrike Witteck, Veronika Witzke, Peter Woitke, David Wolter, Günther Wuchterl, Mark Wyatt, Dan Yang, Jie Yu, Ricardo Zanmar Sanchez, María Rosa Zapatero Osorio, Mathias Zechmeister, Yixiao Zhou, Claas Ziemke, Konstanze Zwintz, Torsten Böhm, Léo Michel Dansac Experimental Astronomy, 2025 PLATO (PLAnetary Transits and Oscillations of stars) is ESA’s M3 mission designed to detect and characterise extrasolar planets and perform asteroseismic monitoring of a large number of stars. PLATO will detect small planets (down to <2R $$_\\textrm{Earth}$$ Earth ) around bright stars (<11 mag), including terrestrial planets in the habitable zone of solar-like stars. With the complement of radial velocity observations from the ground, planets will be characterised for their radius, mass, and age with high accuracy (5%, 10%, 10% for an Earth-Sun combination respectively). PLATO will provide us with a large-scale catalogue of well-characterised small planets up to intermediate orbital periods, relevant for a meaningful comparison to planet formation theories and to better understand planet evolution. It will make possible comparative exoplanetology to place our Solar System planets in a broader context. In parallel, PLATO will study (host) stars using asteroseismology, allowing us to determine the stellar properties with high accuracy, substantially enhancing our knowledge of stellar structure and evolution. The payload instrument consists of 26 cameras with 12cm aperture each. For at least four years, the mission will perform high-precision photometric measurements. Here we review the science objectives, present PLATO‘s target samples and fields, provide an overview of expected core science performance as well as a description of the instrument and the mission profile towards the end of the serial production of the flight cameras. PLATO is scheduled for a launch date end 2026. This overview therefore provides a summary of the mission to the community in preparation of the upcoming operational phases.
Modeling of two CoRoT solar analogues constrained by seismic and spectroscopic analysis M Castro, F Baudin, O Benomar, R Samadi, T Morel, C Barban, J D do Nascimento, Y Lebreton, P Boumier, J P Marques, J S da Costa Monthly Notices of the Royal Astronomical Society, 2021 Solar analogues are important stars to study for understanding the properties of the Sun. Combined with seismic and spectroscopic analysis, evolutionary modelling becomes a powerful method to characterize stellar intrinsic parameters, such as mass, radius, metallicity and age. However, these characteristics, relevant for other aspects of astrophysics or exoplanetary system physics, for example, are difficult to obtain with high precision and/or accuracy. The goal of this study is to characterize the two solar analogues, HD 42618 and HD 43587, observed by CoRoT. In particular, we aim to infer their precise mass, radius and age, using evolutionary modelling constrained by spectroscopic, photometric and seismic analysis. These stars show evidence of being older than the Sun but with a relatively large lithium abundance. We present the seismic analysis of HD 42618, and the modelling of the two solar analogues, HD 42618 and HD 43587 using the cestam stellar evolution code. Models were computed to reproduce the spectroscopic (effective temperature and metallicity) and seismic (mode frequency) data, and the luminosity of the stars, based on Gaia parallaxes. We infer very similar values of mass and radius for both stars compared with the literature, within the uncertainties, and we reproduce correctly the seismic constraints. The modelling shows that HD 42618 is slightly less massive and older than the Sun, and that HD 43587 is more massive and older than the Sun, in agreement with previous results. The use of chemical clocks improves the reliability of our age estimates.
Analysis of eclipsing binaries in multiple stellar systems: The case of V1200 Centauri F Marcadon, K G Hełminiak, J P Marques, R Pawłaszek, P Sybilski, S K Kozłowski, M Ratajczak, M Konacki Monthly Notices of the Royal Astronomical Society, 2020 We present a new analysis of the multiple-star V1200 Centauri based on the most recent observations for this system. We used the photometric observations from the Solaris network and the Transiting Exoplanet Survey Satellite telescope, combined with the new radial velocities from the CHIRON spectrograph and those published in the literature. We confirmed that V1200 Cen consists of a 2.5-d eclipsing binary orbited by a third body. We derived the parameters of the eclipsing components, which are $M_{\\mathrm{ Aa}} = 1.393\\pm 0.018\\,$M⊙, $R_{\\mathrm{ Aa}} = 1.407\\pm 0.014\\,$R⊙, and $T_{{\\rm eff},\\mathrm{ Aa}} = 6588\\pm 58\\,$K for the primary, and $M_{\\mathrm{ Ab}} = 0.8633\\pm 0.0081\\,$M⊙, $R_{\\mathrm{ Ab}} = 1.154\\pm 0.014\\,$R⊙, and $T_{{\\rm eff},\\mathrm{ Ab}} = 4475\\pm 68\\,$K for the secondary. Regarding the third body, we obtained significantly different results than those previously published. The period of the outer orbit is found to be 180.4 d, implying a minimum mass of $M_\\mathrm{ B} = 0.871\\pm 0.020\\,$M⊙. Thus, we argue that V1200 Cen is a quadruple system with a secondary pair composed of two low-mass stars. Finally, we determined the ages of each eclipsing component using two evolution codes, namely mesa and cestam. We obtained ages of 16–18.5 and 5.5–7 Myr for the primary and the secondary, respectively. In particular, the secondary appears larger and hotter than that predicted at the age of the primary. We concluded that dynamical and tidal interactions occurring in multiples may alter the stellar properties and explain the apparent non-coevality of V1200 Centauri.
Chemical mixing in low mass stars: I. Rotation against atomic diffusion including radiative acceleration M. Deal, M.-J. Goupil, J. P. Marques, D. R. Reese, Y. Lebreton Astronomy and Astrophysics, 2020 Context. When modelling stars with masses higher than 1.2 M⊙ with no observed chemical peculiarity, atomic diffusion is often neglected because, on its own, it causes unrealistic surface abundances compared with those observed. The reality is that atomic diffusion is in competition with other transport processes. Rotation is one of the processes able to prevent excessively strong surface abundance variations. Aims. The purpose of this study is to quantify the opposite or conjugated effects of atomic diffusion (including radiative acceleration) and rotationally induced mixing in stellar models of low mass stars, and to assess whether rotational mixing is able to prevent the strong abundance variations induced by atomic diffusion in F-type stars. Our second goal is to estimate the impact of neglecting both rotational mixing and atomic diffusion in stellar parameter inferences for stars with masses higher than 1.3 M⊙. Methods. Using the Asteroseismic Inference on a Massive Scale (AIMS) stellar parameter inference code, we infer the masses and ages of a set of representative artificial stars for which models were computed with the Code d’Evolution Stellaire Adaptatif et Modulaire (CESTAM; the T stands for Transport) evolution code, taking into account rotationally induced mixing and atomic diffusion, including radiative acceleration. The observed constraints are asteroseismic and classical properties. The grid of stellar models used for the optimization search include neither atomic diffusion nor rotationally induced mixing. The differences between real and retrieved parameters then provide an estimate of the errors made when neglecting transport processes in stellar parameter inference. Results. We show that for masses lower than 1.3 M⊙, rotation dominates the transport of chemical elements and strongly reduces the effect of atomic diffusion, with net surface abundance modifications similar to solar values. At higher mass, atomic diffusion and rotation are competing equally. Above 1.44 M⊙, atomic diffusion dominates in stellar models with initial rotation lower than 80 km s−1 producing a chemical peculiarity which is not observed in Kepler Legacy stars. This indicates that a transport process of chemical elements is missing, probably linked to the missing transport process of angular momentum needed to explain rotation profiles in solar-like stars. Importantly, neglecting rotation and atomic diffusion (including radiative acceleration) in the models, when inferring the parameters of F-type stars, may lead to respective errors of ≈5%, ≈2.5%, and ≈25% for stellar masses, radii, and ages. Conclusions. Atomic diffusion (including radiative acceleration) and rotational mixing should be taken into account in stellar models in order to determine accurate stellar parameters. When atomic diffusion and shellular rotation are both included, they enable stellar evolution codes to reproduce the observed metal and helium surface abundances for stars with masses up to 1.4 M⊙ at solar metallicity. However, if rotation is actually uniform for these stars (as observations seem to indicate), then an additional chemical mixing process is needed together with a revised formulation of rotational mixing. For higher masses, an additional mixing process is needed in any case.
γ Doradus stars as a test of angular momentum transport models R.-M. Ouazzani, J. P. Marques, M.-J. Goupil, S. Christophe, V. Antoci, S. J. A. J. Salmon, J. Ballot Astronomy and Astrophysics, 2019 Helioseismology and asteroseismology of red giant stars have shown that distribution of angular momentum in stellar interiors, and the evolution of this distribution with time remains an open issue in stellar physics. Owing to the unprecedented quality and long baseline of Kepler photometry, we are able to seismically infer internal rotation rates in γ Doradus stars, which provide the main-sequence counterpart to the red-giants puzzle. Here, we confront these internal rotation rates to stellar evolution models which account for rotationally induced transport of angular momentum, in order to test angular momentum transport mechanisms. On the one hand, we used a stellar model-independent method developed by our team in order to obtain accurate, seismically inferred, buoyancy radii and near-core rotation for 37 γ Doradus stars observed by Kepler. We show that the stellar buoyancy radius can be used as a reliable evolution indicator for field stars on the main sequence. On the other hand, we computed rotating evolutionary models of intermediate-mass stars including internal transport of angular momentum in radiative zones, following the formalism developed in the series of papers started by Zahn (1992, A&A, 265, 115), with the CESTAM code. This code calculates the rotational history of stars from the birth line to the tip of the RGB. The initial angular momentum content has to be set initially, which is done here by fitting rotation periods in young stellar clusters. We show a clear disagreement between the near-core rotation rates measured in the sample and the rotation rates obtained from the evolutionary models including rotationally induced transport of angular momentum following Zahn’s prescriptions. These results show a disagreement similar to that of the Sun and red giant stars in the considered mass range. This suggests the existence of missing mechanisms responsible for the braking of the core before and along the main sequence. The efficiency of the missing mechanisms is investigated. The transport of angular momentum as formalized by Zahn and Maeder cannot explain the measurements of near-core rotation in main-sequence intermediate-mass stars we have at hand.
Building protoplanetary disks from the molecular cloud: Redefining the disk timeline K. Baillié, J. Marques, L. Piau Astronomy and Astrophysics, 2019 Context. Planetary formation models are necessary to understand the characteristics of the planets that are the most likely to survive. Their dynamics, their composition and even the probability of their survival depend on the environment in which they form. We therefore investigate the most favorable locations for planetary embryos to accumulate in the protoplanetary disk: the planet traps. Aims. We study the formation of the protoplanetary disk by the collapse of a primordial molecular cloud, and how its evolution leads to the selection of specific types of planets. Methods. We use a hydrodynamical code that accounts for the dynamics, thermodynamics, geometry and composition of the disk to numerically model its evolution as it is fed by the infalling cloud material. As the mass accretion rate of the disk onto the star determines its growth, we can calculate the stellar characteristics by interpolating its radius, luminosity and temperature over the stellar mass from pre-calculated stellar evolution models. The density and midplane temperature of the disk then allow us to model the interactions between the disk and potential planets and determine their migration. Results. At the end of the collapse phase, when the disk reaches its maximum mass, it pursues its viscous spreading, similarly to the evolution from a minimum mass solar nebula (MMSN). In addition, we establish a timeline equivalence between the MMSN and a “collapse-formed disk” that would be older by about 2 Myr. Conclusions. We can save various types of planets from a fatal type-I inward migration: in particular, planetary embryos can avoid falling on the star by becoming trapped at the heat transition barriers and at most sublimation lines (except the silicates one). One of the novelties concerns the possible trapping of putative giant planets around a few astronomical units from the star around the end of the infall. Moreover, trapped planets may still follow the traps outward during the collapse phase and inward after it. Finally, this protoplanetary disk formation model shows the early possibilities of trapping planetary embryos at disk stages that are anterior by a few million years to the initial state of the MMSN approximation.
Influence of metallicity on the near-surface effect on oscillation frequencies L. Manchon, K. Belkacem, R. Samadi, T. Sonoi, J. P. C. Marques, H.-G. Ludwig, E. Caffau Astronomy and Astrophysics, 2018 Context. The CoRoT and Kepler missions have provided high-quality measurements of the frequency spectra of solar-like pulsators, enabling us to probe stellar interiors with a very high degree of accuracy by comparing the observed and modelled frequencies. However, the frequencies computed with 1D models suffer from systematic errors related to the poor modelling of the uppermost layers of stars. These biases are what is commonly named the near-surface effect. The dominant effect is thought to be related to the turbulent pressure that modifies the hydrostatic equilibrium and thus the frequencies. This has already been investigated using grids of 3D hydrodynamical simulations, which also were used to constrain the parameters of the empirical correction models. However, the effect of metallicity has not been considered so far. Aims. We aim to study the impact of metallicity on the surface effect, investigating its influence across the Hertzsprung-Russell diagram, and providing a method for accounting for it when using the empirical correction models. Methods. We computed a grid of patched 1D stellar models with the stellar evolution code CESTAM in which poorly modelled surface layers have been replaced by averaged stratification computed with the 3D hydrodynamical code CO5BOLD. It allowed us to investigate the dependence of both the surface effect and the empirical correction functions on the metallicity. Results. We found that metallicity has a strong impact on the surface effect: keeping Teff and log g constant, the frequency residuals can vary by up to a factor of two (for instance from [Fe/H] = + 0.0 to [Fe/H] = + 0.5). Therefore, the influence of metallicity cannot be neglected. We found that the correct way of accounting for it is to consider the surface Rosseland mean opacity. It allowed us to give a physically grounded justification as well as a scaling relation for the frequency differences at νmax as a function of Teff, log g and κ. Finally, we provide prescriptions for the fitting parameters of the most commonly used correction functions. Conclusions. We show that the impact of metallicity through the Rosseland mean opacity must be taken into account when studying and correcting the surface effect.
Impacts of radiative accelerations on solar-like oscillating main-sequence stars M. Deal, G. Alecian, Y. Lebreton, M. J. Goupil, J. P. Marques, F. LeBlanc, P. Morel, B. Pichon Astronomy and Astrophysics, 2018 Context. Chemical element transport processes are among the crucial physical processes needed for precise stellar modelling. Atomic diffusion by gravitational settling is usually taken into account, and is essential for helioseismic studies. On the other hand, radiative accelerations are rarely accounted for, act differently on the various chemical elements, and can strongly counteract gravity in some stellar mass domains. The resulting variations in the abundance profiles may significantly affect the structure of the star.Aims. The aim of this study is to determine whether radiative accelerations impact the structure of solar-like oscillating main-sequence stars observed by asteroseismic space missions.Methods. We implemented the calculation of radiative accelerations operating on C, N, O, Ne, Na, Mg, Al, Si, S, Ca, and Fe in the CESTAM code using the single-valued parameter method. We built and compared several grids of stellar models including gravitational settling, some with and others without radiative accelerations. We considered masses in the range [0.9, 1.5]M⊙and three values of the metallicity around the solar value. For each metallicity we determined the mass range where differences between models due to radiative accelerations exceed the uncertainties of global seismic parameters of theKeplerLegacy sample or expected for PLATO observations.Results. We found that radiative accelerations may not be neglected for stellar masses higher than 1.1M⊙at solar metallicity. The difference in age due to their inclusion in models can reach 9% for the more massive stars of our grids. We estimated that the percentage of the PLATO core program stars whose modelling would require radiative accelerations ranges between 33% and 58% depending on the precision of the seismic data.Conclusions. We conclude that in the context ofKepler, TESS, and PLATO missions which provide (or will provide) high-quality seismic data, radiative accelerations can have a significant effect when properly inferring the properties of solar-like oscillators. This is particularly important for age inferences. However, the net effect for each individual star results from the competition between atomic diffusion including radiative accelerations and other internal transport processes. Rotationally induced transport processes for instance are believed to reduce the effects of atomic diffusion. This will be investigated in a forthcoming companion paper.
Kepler observations of the asteroseismic binary HD 176465 T. R. White, O. Benomar, V. Silva Aguirre, W. H. Ball, T. R. Bedding, W. J. Chaplin, J. Christensen-Dalsgaard, R. A. Garcia, L. Gizon, D. Stello, S. Aigrain, H. M. Antia, T. Appourchaux, M. Bazot, T. L. Campante, O. L. Creevey, G. R. Davies, Y. P. Elsworth, P. Gaulme, R. Handberg, S. Hekker, G. Houdek, R. Howe, D. Huber, C. Karoff, J. P. Marques, S. Mathur, A. McQuillan, T. S. Metcalfe, B. Mosser, M. B. Nielsen, C. Régulo, D. Salabert, T. Stahn Astronomy and Astrophysics, 2017
The PLATO 2.0 mission H. Rauer, C. Catala, C. Aerts, T. Appourchaux, W. Benz, A. Brandeker, J. Christensen-Dalsgaard, M. Deleuil, L. Gizon, M.-J. Goupil, M. Güdel, E. Janot-Pacheco, M. Mas-Hesse, I. Pagano, G. Piotto, D. Pollacco, Ċ. Santos, A. Smith, J.-C. Suárez, R. Szabó, S. Udry, V. Adibekyan, Y. Alibert, J.-M. Almenara, P. Amaro-Seoane, M. Ammler-von Eiff, M. Asplund, E. Antonello, S. Barnes, F. Baudin, K. Belkacem, M. Bergemann, G. Bihain, A. C. Birch, X. Bonfils, I. Boisse, A. S. Bonomo, F. Borsa, I. M. Brandão, E. Brocato, S. Brun, M. Burleigh, R. Burston, J. Cabrera, S. Cassisi, W. Chaplin, S. Charpinet, C. Chiappini, R. P. Church, Sz. Csizmadia, M. Cunha, M. Damasso, M. B. Davies, H. J. Deeg, R. F. Díaz, S. Dreizler, C. Dreyer, P. Eggenberger, D. Ehrenreich, P. Eigmüller, A. Erikson, R. Farmer, S. Feltzing, F. de Oliveira Fialho, P. Figueira, T. Forveille, M. Fridlund, R. A. García, P. Giommi, G. Giuffrida, M. Godolt, J. Gomes da Silva, T. Granzer, J. L. Grenfell, A. Grotsch-Noels, E. Günther, C. A. Haswell, A. P. Hatzes, G. Hébrard, S. Hekker, R. Helled, K. Heng, J. M. Jenkins, A. Johansen, M. L. Khodachenko, K. G. Kislyakova, W. Kley, U. Kolb, N. Krivova, F. Kupka, H. Lammer, A. F. Lanza, Y. Lebreton, D. Magrin, P. Marcos-Arenal, P. M. Marrese, J. P. Marques, J. Martins, S. Mathis, S. Mathur, S. Messina, A. Miglio, J. Montalban, M. Montalto, M. J. P. F. G. Monteiro, H. Moradi, E. Moravveji, C. Mordasini, T. Morel, A. Mortier, V. Nascimbeni, R. P. Nelson, M. B. Nielsen, L. Noack, A. J. Norton, A. Ofir, M. Oshagh, R.-M. Ouazzani, P. Pápics, V. C. Parro, P. Petit, B. Plez, E. Poretti, A. Quirrenbach, R. Ragazzoni, G. Raimondo, M. Rainer, D. R. Reese, R. Redmer, S. Reffert, B. Rojas-Ayala, I. W. Roxburgh, S. Salmon, A. Santerne, J. Schneider, J. Schou, S. Schuh, H. Schunker, A. Silva-Valio, R. Silvotti, I. Skillen, I. Snellen, F. Sohl, S. G. Sousa, A. Sozzetti, D. Stello, K. G. Strassmeier, M. Švanda, Gy. M. Szabó, A. Tkachenko, D. Valencia, V. Van Grootel, S. D. Vauclair, P. Ventura, F. W. Wagner, N. A. Walton, J. Weingrill, S. C. Werner, P. J. Wheatley, K. Zwintz Experimental Astronomy, 2014
On the mass estimation for FGK stars: Comparison of several methods F. J. G. Pinheiro, J. M. Fernandes, M. S. Cunha, M. J. P. F. G. Monteiro, N. C. Santos, S. G. Sousa, J. P. Marques, J.-J. Fang, A. Mortier, J. Sousa Monthly Notices of the Royal Astronomical Society, 2014
Transport of angular momentum in solar-like oscillating stars Mariejo Goupil, Sébastien Deheuvels, Joao Marques, Yveline Lebreton, Benoit Mosser, Rafa García, Kevin Belkacem, Stéphane Mathis Proceedings of the International Astronomical Union, 2014
Asteroseismic fundamental properties of solar-type stars observed by the NASA Kepler mission W. J. Chaplin, S. Basu, D. Huber, A. Serenelli, L. Casagrande, V. Silva Aguirre, W. H. Ball, O. L. Creevey, L. Gizon, R. Handberg, C. Karoff, R. Lutz, J. P. Marques, A. Miglio, D. Stello, M. D. Suran, D. Pricopi, T. S. Metcalfe, M. J. P. F. G. Monteiro, J. Molenda-Żakowicz, T. Appourchaux, J. Christensen-Dalsgaard, Y. Elsworth, R. A. García, G. Houdek, H. Kjeldsen, A. Bonanno, T. L. Campante, E. Corsaro, P. Gaulme, S. Hekker, S. Mathur, B. Mosser, C. Régulo, D. Salabert Astrophysical Journal Supplement Series, 2014
Spin down of the core rotation in red giants B. Mosser, M. J. Goupil, K. Belkacem, J. P. Marques, P. G. Beck, S. Bloemen, J. De Ridder, C. Barban, S. Deheuvels, Y. Elsworth, S. Hekker, T. Kallinger, R. M. Ouazzani, M. Pinsonneault, R. Samadi, D. Stello, R. A. García, T. C. Klaus, J. Li, S. Mathur, R. L. Morris Astronomy and Astrophysics, 2012
A precise asteroseismic age and radius for the evolved sun-like star KIC 11026764 T. S. Metcalfe, M. J. P. F. G. Monteiro, M. J. Thompson, J. Molenda-Żakowicz, T. Appourchaux, W. J. Chaplin, G. Doğan, P. Eggenberger, T. R. Bedding, H. Bruntt, O. L. Creevey, P.-O. Quirion, D. Stello, A. Bonanno, V. Silva Aguirre, S. Basu, L. Esch, N. Gai, M. P. Di Mauro, A. G. Kosovichev, I. N. Kitiashvili, J. C. Suárez, A. Moya, L. Piau, R. A. García, J. P. Marques, A. Frasca, K. Biazzo, S. G. Sousa, S. Dreizler, M. Bazot, C. Karoff, S. Frandsen, P. A. Wilson, T. M. Brown, J. Christensen-Dalsgaard, R. L. Gilliland, H. Kjeldsen, T. L. Campante, S. T. Fletcher, R. Handberg, C. Régulo, D. Salabert, J. Schou, G. A. Verner, J. Ballot, A.-M. Broomhall, Y. Elsworth, S. Hekker, D. Huber, S. Mathur, R. New, I. W. Roxburgh, K. H. Sato, T. R. White, W. J. Borucki, D. G. Koch, J. M. Jenkins Astrophysical Journal, 2010
The PMS δ Scuti star PDS2 M. Marconi, V. Ripepi, S. Bernabei, A. Ruoppo, M. J. P. F. G. Monteiro, J. P. Marques, F. Palla, S. Leccia Astrophysics and Space Science, 2010
