Energetic Neutral Atom Imaging of Planetary Environments

TL;DR

This paper explores the use of energetic neutral atom imaging to study planetary environments, offering a global, real-time view of magnetospheric plasma and surface interactions, surpassing traditional in situ measurement limitations.

Contribution

It demonstrates the application of ENA imaging to Earth, Mars, and Mercury, highlighting its advantages for comprehensive, instantaneous plasma and surface analysis over prior methods.

Findings

ENA imaging provides a global view of planetary magnetospheres.

It enables the study of thermal neutral populations and surface composition.

The technique allows for real-time monitoring of dynamic plasma phenomena.

Abstract

The aim of this work is to investigate the applications of the neutral atom imaging to the environments of the Earth, Mars and Mercury. This innovative technique permits the study of energetic plasma by means of analysing the result of the interaction of this plasma with a neutral thermal population or with a surface. The main advantage, when compared to the direct ion detection, is that it is possible to have an instantaneous survey of the whole magnetosphere of a planet. An example could help. Before the first ENA data, most of the knowledge about the Earth magnetospheric plasma came from in situ measurements of ions, electrons and electromagnetic fields. Those measurements, of course, could not represent any real instantaneous situation, but only an averaged picture of it, since the temporal and spatial variation cannot be easily be distinguished. Some short time scale phenomena, such as substorms, have been found difficult to comprehend without a global and continuous imaging. Even if some information about the plasma may be extracted from other sources, such as UV imaging [like aurorae, e.g. Horwitz, 1987], some populations (for example, the ring current) remained invisible. Furthermore, neutral atom imaging gives information not only about the energetic plasma, but also about the thermal neutral population (in the case of charge-exchange) or about the surface composition (in the case of sputtering). Conversely, it is necessary to set up some dedicated unfolding techniques to recover the 3D plasma distributions from the 2D ENA images.