TY - CHAP
T1 - Dawn-dusk Asymmetries in the Auroral Particle Precipitation and Their Modulations by Substorms
AU - Johnson, Jay R.
AU - Wing, Simon
AU - Camporeale, Enrico
PY - 2017
Y1 - 2017
N2 - Auroral particle precipitation exhibits dawn‐dusk asymmetries that reflect the asymmetries in the particle populations, waves, and processes in the magnetosphere. The diffuse auroral electrons can be observed mainly in 22:00–09:00 MLT, which coincides with much of the spatial distribution of the whistler‐mode chorus waves that have been shown to be the predominant mechanism for pitch‐angle scattering magnetospheric electrons into the loss cone. On the other hand, the monoenergetic auroral electrons can be observed in the dusk‐midnight sector. The monoenergetic electrons are magnetospheric electrons that have gone through a quasistatic parallel electric field in the upward field‐aligned current regions. The broadband auroral electrons can be found mostly at 22:00–02:00 MLT where a peak in the Poynting flux of Alfvén waves is observed. Alfvén waves are known to cause broadband acceleration of electrons. There may be a connection between monoenergetic and broadband electrons in that the low‐frequency Alfvén wave–electron interaction can result in monoenergetic electron signature. Substorms increase the power of the diffuse, monoenergetic, and broadband electron aurora by 310%, 71%, and 170%, respectively. The duration of the substorm cycle for monenergetic and broadband auroral is ~5 h, but it is larger than 5 h for diffuse auroral electrons.
AB - Auroral particle precipitation exhibits dawn‐dusk asymmetries that reflect the asymmetries in the particle populations, waves, and processes in the magnetosphere. The diffuse auroral electrons can be observed mainly in 22:00–09:00 MLT, which coincides with much of the spatial distribution of the whistler‐mode chorus waves that have been shown to be the predominant mechanism for pitch‐angle scattering magnetospheric electrons into the loss cone. On the other hand, the monoenergetic auroral electrons can be observed in the dusk‐midnight sector. The monoenergetic electrons are magnetospheric electrons that have gone through a quasistatic parallel electric field in the upward field‐aligned current regions. The broadband auroral electrons can be found mostly at 22:00–02:00 MLT where a peak in the Poynting flux of Alfvén waves is observed. Alfvén waves are known to cause broadband acceleration of electrons. There may be a connection between monoenergetic and broadband electrons in that the low‐frequency Alfvén wave–electron interaction can result in monoenergetic electron signature. Substorms increase the power of the diffuse, monoenergetic, and broadband electron aurora by 310%, 71%, and 170%, respectively. The duration of the substorm cycle for monenergetic and broadband auroral is ~5 h, but it is larger than 5 h for diffuse auroral electrons.
KW - Auroral particle precipitation
KW - Broadband electron aurora
KW - Diffuse electron aurora
KW - Earth's magnetic field lines
KW - Electron auroral dawn‐dusk asymmetry
KW - Modulations
KW - Ion aurora monoenergetic electron
KW - Aurora nightside electron auroral power
KW - Planetary plasma environments
KW - Substorm cycle
UR - https://digitalcommons.andrews.edu/pubs/700
U2 - 10.1002/9781119216346.ch20
DO - 10.1002/9781119216346.ch20
M3 - Chapter (peer-reviewed)
SN - 9781119216322
T3 - Geophysical Monograph Series
SP - 255
EP - 272
BT - Dawn‐Dusk Asymmetries in Planetary Plasma Environments
A2 - Haaland, Stein
A2 - Runov, Andrei
A2 - Forsyth, Conln
PB - Wiley
CY - Hoboken, NJ
ER -