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Ionization by cosmic rays of the atmosphere of Titan
Institution:1. LESIA, Observatoire de Paris, PSL Research University, CNRS, Sorbonne Universités, UPMC Univ. Paris 06, Univ. Paris Diderot, Sorbonne Paris Cité, 5 place Jules Janssen, Meudon 92195, France;2. Université Grenoble Alpes, CNRS, Institut de Planétologie et d’Astrophysique de Grenoble (IPAG), France;3. GSMA, UMR CNRS 6089, Univ. de Reims Champagne-Ardenne, France;4. Institut Villebon - Georges Charpak, Département de Physique - UFR Sciences, Université Paris Sud, Bat. 490, rue Hector Berlioz, Orsay 91400, France;5. Department of Physdical Geography, Utrecht University, 3508 TC Utrecht, P.O. Box 80115, The Netherlands;6. NASA/Goddard Space Flight Center, Code 693, Greenbelt, MD, 20771, USA;1. Department of Comparative Biomedicine and Food Science, University of Padova, Italy;2. Regional Centre of Advanced Technologies and Materials, Department of Physical Chemistry, Palacky University in Olomouc, Czech Republic;3. Department of Molecular Medicine, University of Padova, Italy;1. Programa de Biologia Marinha e Ambientes Costeiros, Instituto de Biologia, Universidade Federal Fluminense, Niterói, RJ 24020-150, Brazil;2. Programa Dinâmica dos Oceanos e da Terra, Instituto de Geociências, Universidade Federal Fluminense, Niterói, RJ 24210-346, Brazil
Abstract:Cosmic ray radiation is the main mechanism for ionizing the lower atmosphere of Titan. Their higher penetration power, in comparison with solar photons, allows cosmic rays to penetrate deep into the atmosphere of Titan, ionizing the neutral molecules and generating an ionosphere with an electron density peak, placed at around 90 km, similar in magnitude to the ionospheric peak produced by solar radiation in the upper atmosphere. In the lower atmosphere, the electron density profile, in the absence of a magnetic field, depends mainly on the modulation of cosmic rays by the solar wind and on the nature of the ionizable particles. We present here the first results of a new numerical model developed to calculate the concentration of electrons and most abundant ions in the Titan lower atmosphere. The present knowledge of Titan’s atmosphere permits us to include new neutral and ionic species, such as oxygen derivates, in a more detailed ion-chemistry calculation than previous lower ionospheric models of Titan. The electron density peaks at 90 km with a magnitude of 2150 cm?3. The ion distribution obtained predicts that cluster cations and hydrocarbon cations are the most abundant ions below and above the electron density peak, respectively. We also discuss the effect of solar activity at the distance of the Saturn orbit on the spectrum of the cosmic particles. We obtain that from solar minimum to solar maximum the ionization rate at the energy deposition peak changes by a factor of 1.2 at 70 km, and by a factor of 2.6 at altitudes as high as 400 km. The electron density at the concentration peak changes by a factor of 1.1 at 90 km, and by a factor of 1.6 at 400 km.
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