Ionization processes in the atmosphere of Titan - III. Ionization by high-Z nuclei cosmic rays

Context. The Cassini-Huygens mission has revealed the importance of particle precipitation in the atmosphere of Titan thanks to in-situ measurements. These ionizing particles (electrons, protons, and cosmic rays) have a strong impact on the chemistry, hence must be modeled. Aims. We revisit our computation of ionization in the atmosphere of Titan by cosmic rays. The high-energy high-mass ions are taken into account to improve the precision of the calculation of the ion production profile. Methods. The Badhwahr and O’Neill model for cosmic ray spectrum was adapted for the Titan model. We used the TransTitan model coupled with the Planetocosmics model to compute the ion production by cosmic rays. We compared the results with the NAIRAS/HZETRN ionization model used for the first time for a body that differs from the Earth. Results. The cosmic ray ionization is computed for five groups of cosmic rays, depending on their charge and mass: protons, alpha, Z = 8 (oxygen), Z = 14 (silicon), and Z = 26 (iron) nucleus. Protons and alpha particles ionize mainly at 65 km altitude, while the higher mass nucleons ionize at higher altitudes. Nevertheless, the ionization at higher altitude is insufficient to obscure the impact of Saturn’s magnetosphere protons at a 500 km altitude. The ionization rate at the peak (altitude: 65 km, for all the different conditions) lies between 30 and 40 cm−3s−1. Conclusions. These new computations show for the first time the importance of high Z cosmic rays on the ionization of the Titan atmosphere. The updated full ionization profile shape does not differ significantly from that found in our previous calculations (Paper I: Gronoff et al. 2009, 506, 955) but undergoes a strong increase in intensity below an altitude of 400 km, especially between 200 and 400 km altitude where alpha and heavier particles (in the cosmic ray spectrum) are responsible for 40% of the ionization. The comparison of several models of ionization and cosmic ray spectra (in intensity and composition) reassures us about the stability of the altitude of the ionization peak (65 km altitude) with respect to the solar activity.

[1]  S. Atreya,et al.  Current state of modeling the photochemistry of Titan's mutually dependent atmosphere and ionosphere , 2004 .

[2]  K. Santhanam,et al.  Cosmic ray synthesis of organic molecules in Titan's atmosphere , 1980 .

[3]  M. Greco,et al.  Calculation of the TeV prompt muon component in very high energy cosmic ray showers , 1995 .

[4]  M. Storini,et al.  Ionization of the earth’s atmosphere by solar and galactic cosmic rays , 2009 .

[5]  K. O'brien Extra-nuclear hadron cascade calculations using Passow's approximation , 1969 .

[6]  W. Borucki,et al.  Influence of high abundances of aerosols on the electrical conductivity of the Titan atmosphere , 2008 .

[7]  W. Webber,et al.  Production of cosmogenic Be nuclei in the Earth's atmosphere by cosmic rays: Its dependence on solar modulation and the interstellar cosmic ray spectrum , 2003 .

[8]  Peter Velinov,et al.  Improved cosmic ray ionization model for the system ionosphere–atmosphere—Calculation of electron production rate profiles , 2008 .

[9]  Christopher J. Mertens,et al.  Geomagnetic influence on aircraft radiation exposure during a solar energetic particle event in October 2003 , 2010 .

[10]  L. Capone,et al.  The lower ionosphere of Titan , 1976 .

[11]  K. A. Smith,et al.  Absolute partial cross sections for electron-impact ionization of CH_4, H_2O, and D_2O from threshold to 1000 eV. , 1996 .

[12]  Christopher J. Mertens,et al.  Coupling of multiple Coulomb scattering with energy loss and straggling in HZETRN , 2006 .

[13]  J. Lilensten,et al.  Ionization processes in the atmosphere of Titan: I. Ionization in the whole atmosphere , 2009 .

[14]  Peter Velinov,et al.  Analytical approach to cosmic ray ionization by nuclei with charge Z in the middle atmosphere – Distribution of galactic CR effects , 2008 .

[15]  P. O'Neill Badhwar–O’Neill galactic cosmic ray model update based on advanced composition explorer (ACE) energy spectra from 1997 to present , 2004 .

[16]  L. Lara,et al.  Chemistry of the galactic cosmic ray induced ionosphere of Titan , 1999 .

[17]  Arnaldo Alves Cardoso,et al.  Sources of atmospheric acidity in an agricultural-industrial region of São Paulo State, Brazil , 2003 .

[18]  P. Falkner,et al.  Structure of Titan's low altitude ionized layer from the Relaxation Probe onboard HUYGENS , 2008 .

[19]  G. Badhwar,et al.  Galactic cosmic radiation model and its applications. , 1996, Advances in space research : the official journal of the Committee on Space Research.

[20]  P. Falkner,et al.  Electron conductivity and density profiles derived from the mutual impedance probe measurements performed during the descent of Huygens through the atmosphere of Titan , 2007 .

[21]  L. Lara,et al.  Ionization by cosmic rays of the atmosphere of Titan , 1999 .

[22]  V. Krasnopolsky A photochemical model of Titan's atmosphere and ionosphere , 2009 .

[23]  Jean Lilensten,et al.  Ionization processes in the atmosphere of Titan II. Electron precipitation along magnetic field lines , 2009 .

[24]  W. Borucki,et al.  Predictions of the electrical conductivity and charging of the aerosols in Titan's atmosphere , 1987 .

[25]  A. Coustenis,et al.  Coupling photochemistry with haze formation in Titan's atmosphere, Part II: Results and validation with Cassini/Huygens data , 2008 .

[26]  L. Capone,et al.  Galactic cosmic rays and N2 dissociation on Titan , 1983 .

[27]  V. Krasnopolsky,et al.  The photochemical model of Titan’s atmosphere and ionosphere: A version without hydrodynamic escape , 2010 .