2014
DOI: 10.1007/978-3-319-09749-7_6
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Suprathermal Particles in XUV-Heated and Extended Exoplanetary Upper Atmospheres

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Cited by 14 publications
(7 citation statements)
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“…This procedure is analogous to a Monte Carlo algorithm for solving the stochastic kinetic equation. In the numerical realizations of the kinetic model the following recent developments in the theory and practice of DSMC method have been used (see, e.g., Shematovich 2004;Shematovich et al 2015): (i) an effective approximation of the major frequency, where the collision probability for the chosen pair is estimated from the maximum possible frequencies and is used in choosing the next transition; (ii) the multichannel nature of the selected reaction is taken into account for the transition to be realized; this means that the transition is treated as the simultaneous drawing of all possible (elastic, inelastic, and chemically reactive) channels for each one of which the corresponding weight is transferred to the total cross section of the collisional process, proportionally to the ratio of the partial cross section for the given channel; (iii) since the algorithmic steps of both introducing suprathermal particles (in accordance with the source functions) and drawing the collisional transitions are accompanied by the formation of new model particles, it is necessary to control the total number of model particles in the numerical model. An efficient method for this control is the so-called clustering of model particles, where groups of model particles with similar parameters are combined into a single particle with weighted parameters.…”
Section: Collision Times Between Molecular Species Become Longmentioning
confidence: 99%
“…This procedure is analogous to a Monte Carlo algorithm for solving the stochastic kinetic equation. In the numerical realizations of the kinetic model the following recent developments in the theory and practice of DSMC method have been used (see, e.g., Shematovich 2004;Shematovich et al 2015): (i) an effective approximation of the major frequency, where the collision probability for the chosen pair is estimated from the maximum possible frequencies and is used in choosing the next transition; (ii) the multichannel nature of the selected reaction is taken into account for the transition to be realized; this means that the transition is treated as the simultaneous drawing of all possible (elastic, inelastic, and chemically reactive) channels for each one of which the corresponding weight is transferred to the total cross section of the collisional process, proportionally to the ratio of the partial cross section for the given channel; (iii) since the algorithmic steps of both introducing suprathermal particles (in accordance with the source functions) and drawing the collisional transitions are accompanied by the formation of new model particles, it is necessary to control the total number of model particles in the numerical model. An efficient method for this control is the so-called clustering of model particles, where groups of model particles with similar parameters are combined into a single particle with weighted parameters.…”
Section: Collision Times Between Molecular Species Become Longmentioning
confidence: 99%
“…mospheric loss on hydrogen-rich exoplanets (Shematovich et al, 2015). In our solar system, Pluto's atmosphere contains detectable CO and N 2 but lacks CO 2 (Steffl et al, 2020), whereas CO, CO 2 , and N 2 are the dominant constituents in the atmospheres of Mars and Venus, which have nearly identical UV spectra (Chaufray et al, 2012;Feldman et al, 2000;Gérard et al, 2017;Hubert et al, 2010).…”
mentioning
confidence: 86%
“…Carbon monoxide is the second most abundant molecule in interstellar space and is used as a tracer for presence of H 2 in star forming regions and molecular clouds (Ferlet et al., 2000; van Dishoeck & Black, 1986). Further, robust laboratory analysis of CO and CO 2 emission features may be an important asset in studying H 2 structures in exoplanetary upper atmospheres, the photolysis of which contributes significantly to atmospheric loss on hydrogen‐rich exoplanets (Shematovich et al., 2015). In our solar system, Pluto's atmosphere contains detectable CO and N 2 but lacks CO 2 (Steffl et al., 2020), whereas CO, CO 2 , and N 2 are the dominant constituents in the atmospheres of Mars and Venus, which have nearly identical UV spectra (Chaufray et al., 2012; Feldman et al., 2000; Gérard et al., 2017; Hubert et al., 2010).…”
Section: Introductionmentioning
confidence: 99%
“…Two main hypotheses have been put forth to explain the existence of this envelope. The first is the expansion of the planetary atmosphere due to heating by radiation from the star [260,261], which gives rise to outflows of matter at rates of ∼10 10 g/s. The second is based on the mechanism of chargeexchange of ions in the stellar wind during collisions with atoms in the atmosphere [262].…”
Section: Uv Line Emission From the Atmospheres Of Exoplanetsmentioning
confidence: 99%