Earth's Aurora

The Aurora Borealis and Australis (see Figure 1) are a beautiful manifestation of the Solar-Terrestrial Interaction. They result when magnetospheric electrons and protons with energies greater than around 1keV collide with neutral atoms and molecules in the upper atmosphere. The atoms are excited to a higher energy state during the collision, and in order to lose their excess energy, they emit light.

Although we have long known why light is emitted in the upper atmosphere during an auroral display, we have much less information about why aurora appear to be organized in long thin strips like the aurora in Figure 1. These strips, known as auroral arcs, are sometimes fairly static, but sometimes highly dynamic.

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Figure 1: Photograph of aurora from the International Space Station (Photo credit: NASA, ISS023-E-58455)


Auroral Acceleration

Typically, to create bright auroral arcs, electrons must be accelerated down towards the Earth from space. This acceleration happens in the direction parallel or antiparallel to the geomagnetic field. It is now generally accepted that there are two different types of acceleration:

  • Quasistatic potential drops: On time scales much longer than the time it takes for an electron to bounce between mirror points, parallel electric fields develop at low altitudes just above the Earth's ionosphere. There is a great deal of observational evidence for this type of acceleration mechanism from in-situ spacecraft measurements.

    In spacecraft measurements, the differential electron energy flux is enhanced over a very narrow range of energies as if they have all experienced the same accelerating electric field - i.e., this behaviour suggests that the electric field structure is essentially static.

  • Acceleration in Shear Alfvén waves: sometimes referred to as Alfvenic acceleration. The magnetosphere supports low-frequency electromagnetic waves that carry energy and information over vast distances. One type of low-frequency waves - Shear Alfvén waves - are transverse oscillations of the magnetic field that can support parallel electric fields when their perpendicular wavelengths are small. Under these circumstances, electrons can gain sufficient energy to create the aurora.

Auroral research in the Department of Meteorology

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Figure 2: (after Watt et al, GRL, 2006) Comparison between FAST observations (top two rows) and DK1D simulation results (bottom row) showing electron behaviour during and acceleration event.
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Figure 3: (after Watt and Rankin, PRL, 2009) Two snapshots of the electron distribution function as a function of parallel velocity (horizontal axis) and distance along geomagnetic field (vertical axis). z=0 corresponds to around 2 Earth radii above Earth's surfance
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Figure 4: (after Watt and Rankin, AGU monograph) (a) and (b) show in-situ observations of electron distribution functions from the Polar spacecraft (Janhunen et al., Space Science Reviews, 2006 and Wygant et al., Journal of Geophysical Review, 2002),(c) shows the simulation result at high altitude (e.g. at altitudes above 4 Earth radii)

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