There is no Plan B for dealing with the climate crisis

BULLETIN OF THE ATOMIC SCIENTISTS Informa UK Limited 75:5 (2019) 215-221

Abstract:

© 2019, © 2019 Bulletin of the Atomic Scientists. To halt global warming, the emission of carbon dioxide into the atmosphere by human activities such as fossil fuel burning, cement production, and deforestation needs to be brought all the way to zero. The longer it takes to do so, the hotter the world will get. Lack of progress towards decarbonization has created justifiable panic about the climate crisis. This has led to an intensified interest in technological climate interventions that involve increasing the reflection of sunlight to space by injecting substances into the stratosphere which lead to the formation of highly reflective particles. When first suggested, such albedo modification schemes were introduced as a “Plan B,” in case the world economy fails to decarbonize, and this scenario has dominated much of the public perception of albedo modification as a savior waiting in the wings to protect the world against massive climate change arising from a failure to decarbonize. But because of the mismatch between the millennial persistence time of carbon dioxide and the sub-decadal persistence of stratospheric particles, albedo modification can never safely play more than a very minor role in the portfolio of solutions. There is simply no substitute for decarbonization.

Scaling Relations for Terrestrial Exoplanet Atmospheres from Baroclinic Criticality

(2019)

Authors:

Thaddeus D Komacek, Malte F Jansen, Eric T Wolf, Dorian S Abbot

Ethane in Titan's Stratosphere from Cassini CIRS Far- and Mid-Infrared Spectra

(2019)

Authors:

Nicholas A Lombardo, Conor A Nixon, Melody Sylvestre, Donald E Jennings, Nicholas Teanby, Patrick GJ Irwin, F Michael Flasar

ESA Voyage 2050 White Paper: Detecting life outside our solar system with a large high-contrast-imaging mission

arXiv e-prints (2019) arXiv:1908.01803-arXiv:1908.01803

Authors:

Ignas Snellen, Simon Albrecht, Guillem Anglada-Escude, Isabelle Baraffe, Pierre Baudoz, Willy Benz, Jean-Luc Beuzit, Beth Biller, Jayne Birkby, Anthony Boccaletti, Roy van Boekel, Jos de Boer, Matteo Brogi, Lars Buchhave, Ludmila Carone, Mark Claire, Riccardo Claudi, Brice-Olivier Demory, Jean-Michel Desert, Silvano Desidera, Scott Gaudi, Raffaele Gratton, Michael Gillon, John Lee Grenfell, Olivier Guyon, Thomas Henning, Sasha Hinkley, Elsa Huby, Markus Janson, Christiane Helling, Kevin Heng, Markus Kasper, Christoph Keller, Matthew Kenworthy, Oliver Krause, Laura Kreidberg, Nikku Madhusudhan, Anne-Marie Lagrange, Ralf Launhardt, Tim Lenton, Manuel Lopez-Puertas, Anne-Lise Maire, Nathan Mayne, Victoria Meadows, Bertrand Mennesson, Giuseppina Micela, Yamila Miguel, Julien Milli, Michiel Min, Ernst de Mooij, David Mouillet, Mamadou N’Diaye, Valentina D’Orazi, Enric Palle, Isabella Pagano, Giampaolo Piotto, Didier Queloz, Heike Rauer, Ignasi Ribas, Garreth Ruane, Franck Selsis, Frans Snik, Alessandro Sozzetti, Daphne Stam, Christopher Stark, Arthur Vigan, Pieter de Visser

The Fukang pallasite: Characterization and implications for the history of the Main‐group parent body

Meteoritics & Planetary Science Wiley 54:8 (2019) 1781-1807

Authors:

Daniella N DellaGiustina, Namrah Habib, Kenneth J Domanik, Dolores H Hill, Dante S Lauretta, Yulia S Goreva, Marvin Killgore, Yang Hexiong, Robert T Downs

Abstract:

AbstractWe report the results of a study of the Fukang pallasite that includes measurements of bulk composition, mineral chemistry, mineral structure, and petrology. Fukang is a Main‐group pallasite that consists of semiangular olivine grains (Fo 86.3) embedded in an Fe‐Ni matrix with 9–10 wt% Ni and low‐Ir (45 ppb). Olivine grains sometimes occur in large clusters up to 11 cm across. The Fe‐Ni phase is primarily kamacite with accessory taenite and plessite. Minor phases include schreibersite, chromite, merrillite, troilite, and low‐Ca pyroxene. We describe a variety of silicate inclusions enclosed in olivine that contain phases rarely or not previously reported in Main‐group pallasites, including clinopyroxene (augite), tridymite, K‐rich felsic glass, and an unknown Ca‐Cr silicate. Pressure constraints determined from tridymite (<0.4 GPa), two‐pyroxene barometry (0.39 ± 0.07 GPa), and geophysical calculations that assume pallasite formation at the core–mantle boundary (CMB), provide an upper estimate on the size of the Main‐group parent body from which Fukang originated. We conclude that Fukang originated at the CMB of a large differentiated planetesimal 400–680 km in radius.