Abstract

Both heliophysics and planetary physics seek to understand the complex nature of the solar wind’s interaction with solar system obstacles like Earth’s magnetosphere, the ionospheres of Venus and Mars, and comets. Studies with this objective are frequently conducted with the help of single or multipoint in situ electromagnetic field and particle observations, guided by the predictions of both local and global numerical simulations, and placed in context by observations from far and extreme ultraviolet (FUV, EUV), hard X-ray, and energetic neutral atom imagers (ENA). Each proposed interaction mechanism (e.g., steady or transient magnetic reconnection, local or global magnetic reconnection, ion pick-up, or the Kelvin-Helmholtz instability) generates diagnostic plasma density structures. The significance of each mechanism to the overall interaction (as measured in terms of atmospheric/ionospheric loss at comets, Venus, and Mars or global magnetospheric/ionospheric convection at Earth) remains to be determined but can be evaluated on the basis of how often the density signatures that it generates are observed as a function of solar wind conditions. This paper reviews efforts to image the diagnostic plasma density structures in the soft (low energy, 0.1–2.0 keV) X-rays produced when high charge state solar wind ions exchange electrons with the exospheric neutrals surrounding solar system obstacles.The introduction notes that theory, local, and global simulations predict the characteristics of plasma boundaries such the bow shock and magnetopause (including location, density gradient, and motion) and regions such as the magnetosheath (including density and width) as a function of location, solar wind conditions, and the particular mechanism operating. In situ measurements confirm the existence of time- and spatial-dependent plasma density structures like the bow shock, magnetosheath, and magnetopause/ionopause at Venus, Mars, comets, and the Earth. However, in situ measurements rarely suffice to determine the global extent of these density structures or their global variation as a function of solar wind conditions, except in the form of empirical studies based on observations from many different times and solar wind conditions. Remote sensing observations provide global information about auroral ovals (FUV and hard X-ray), the terrestrial plasmasphere (EUV), and the terrestrial ring current (ENA). ENA instruments with low energy thresholds (sim1~mbox{keV}) have recently been used to obtain important information concerning the magnetosheaths of Venus, Mars, and the Earth. Recent technological developments make these magnetosheaths valuable potential targets for high-cadence wide-field-of-view soft X-ray imagers.Section 2 describes proposed dayside interaction mechanisms, including reconnection, the Kelvin-Helmholtz instability, and other processes in greater detail with an emphasis on the plasma density structures that they generate. It focuses upon the questions that remain as yet unanswered, such as the significance of each proposed interaction mode, which can be determined from its occurrence pattern as a function of location and solar wind conditions. Section 3 outlines the physics underlying the charge exchange generation of soft X-rays. Section 4 lists the background sources (helium focusing cone, planetary, and cosmic) of soft X-rays from which the charge exchange emissions generated by solar wind exchange must be distinguished. With the help of simulations employing state-of-the-art magnetohydrodynamic models for the solar wind-magnetosphere interaction, models for Earth’s exosphere, and knowledge concerning these background emissions, Sect. 5 demonstrates that boundaries and regions such as the bow shock, magnetosheath, magnetopause, and cusps can readily be identified in images of charge exchange emissions. Section 6 reviews observations by (generally narrow) field of view (FOV) astrophysical telescopes that confirm the presence of these emissions at the intensities predicted by the simulations. Section 7 describes the design of a notional wide FOV “lobster-eye” telescope capable of imaging the global interactions and shows how it might be used to extract information concerning the global interaction of the solar wind with solar system obstacles. The conclusion outlines prospects for missions employing such wide FOV imagers.

Highlights

  • Earth’s magnetic field carves out a cavity in the oncoming solar wind known as the magnetosphere

  • Because the decelerated and thermalized solar wind protons gyrate around magnetosheath magnetic field lines, the pre-existing directions are effectively random over the expected scale lengths of magnetosheath phenomena, and the energetic neutral atom imagers (ENA) flux seen in any direction is approximately proportional to the integrated line-of-sight (LOS) product of the plasma ion and exospheric neutral densities

  • Numerical simulations that employ magnetohydrodynamic models for solar wind densities and velocities and the results from a Monte Carlo simulation of exospheric densities indicate that the plasma density structures can be imaged in the soft (0.1–2.0 keV) X-rays generated when high charge state solar wind ions exchange electrons with exospheric neutrals

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Summary

Introduction

Earth’s magnetic field carves out a cavity in the oncoming solar wind known as the magnetosphere. A sharp magnetopause or ionopause (I) separates the magnetosheath from the planetary obstacle, whether it be the high density ionospheres with plasmas of planetary origin at Venus and Mars or the low density magnetosphere at Earth. Many micro- to macro-scale processes have been predicted and observed to occur in the vicinity of the bow shock and magnetopause, as well as throughout the foreshock, magnetosheath, and outer magnetosphere. These processes are often identified on the basis of the diagnostic density structures that they generate. Microscale features include the kinetic structures generated by wave-particle interactions within the

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Scientific Objectives
The Earth
Earth’s Magnetopause
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The Earth’s Cusps
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Transients at Earth’s Magnetopause and in the Cusps
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Earth’s Magnetosheath
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Earth’s Bow Shock
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Earth’s Foreshock
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Comets
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Mars and Venus
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The Moon
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Soft X-Ray Intensities from Solar Wind Charge Exchange
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Predicted Charge-Exchange Cross-Sections
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Experimental Measurements of Charge-Exchange Cross Sections
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The Branching Ratio and Spectra
The Flux of High Charge State Solar Wind Ions
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Neutral Densities in the Outer Exosphere
Charge Exchange Within the Magnetosphere
Other Sources of Soft X-Rays
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Solar Emissions
Emissions from the Heliosphere
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Planetary Emissions
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Cosmic Soft X-Ray Emissions
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Simulations
Relative Emission Strengths
Past Modeling Efforts
Modeling Soft X-Ray Emissions from Venus and Mars
Modeling Soft X-Ray Emissions from the Heliosphere
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Past Observations of X-Rays Generated by Charge Exchange Processes
Temporal Variability at Earth
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Spatial Variability at Earth
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Line Emissions Near Earth
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The Heliosphere
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General Considerations
Soft X-Ray Imaging Technologies
Optical Elements
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Detectors
Implementation
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Instrument Simulations
Creating the Simulations
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Data Analysis with Simulations
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Summary and Prospects
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Findings
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Full Text
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