PDF file, 7Mb - MIT Haystack Observatory

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PDF file, 7Mb - MIT Haystack Observatory
Dynamics and Structure of SubAuroral
Polarization Streams
Evgeny Mishin
Boston College ISR
With contributions from & thanks to Bill Burke
MIT Haystack Observatory
November 7, 2005
1
OUTLINE
•
Prompt SAPS response to the substorm onset
and solar wind oscillations: DMSP and ISR
•
SAPS-wave structures: The benchmark of RC
injections
•
Plasma waves and heating/acceleration in the
ring current- plasmasphere overlap
2
Solar wind & IMF oscillations
[Mishin et al., 2002]
Sept 25, 1998
12-min oscillations
3
A stormtime substorm
21.0 MLT& 66 MLat
dipolarization
The substorm onset at 08:18 UT
4
Response to the substorm onset
Before
Onset: 0818 UT
SAPS
after
21.0 MLT & L~6
SAPS: 0830 UT
15.5 MLT & L~3
SAPS
15.5 MLT
ÙL~3
&ÙMLT~5.5
in 12 min
VR~ 30 km/s
Vϕ~ 15 km/s
5
Solar wind- & IMF-driven
SAPS- modulation
~12-min
oscillations
6
Structured SAPS
Nov 6, 2001
Onset at ~0350 UT
PS equatorial boundary
7
Strong SAPSWS:
The benchmark of RC injections
DMSP F14, April 6, 2000
electrons
[Mishin et al., 2004]
RC ions
ions
“Strong”
oscillations ≥ mean
SAPSWS:
Meso-scale
Alfven wave
Electron temperature
Ion temperature
Density
troughs
8
RC-injection events: Waves
[Mishin & Burke, 2005]
CRRES & DMSP, June 5, 1991
UHR
LHR
inner edge
Plasma Sheet boundary
Electrons
Ions
NOSE
SAPSWS
Suprathermal
electrons &
ions
Density trough
Alfven
wavestructure
SAPSWS maps to
the wave structure
observed by
CRRES at 17 MLT
9
Alfve’n waves in RC- plasmasphere overlap:
Current-convective instability
ω ' = ω − k|| gJ || /(ene )
[Volkov& Maltsev, 1986]
(Static approximation)
Transverse motion of
RC cloud favors
generation of
short-scale modes
ω ' = ω − k|| gJ || /(ene ) − k⊥ gU D
10
SAPSWS evolution after substorm injections
June 5, 1991 [Mishin and Burke, 2005]
electr
ons
ions
Density
troughs
substorm onsets
11
Electron Heating
Wanted
Heating source of plasmaspheric electrons at
the RC’s inner edge
Collisional
heating rate
12
Diamagnetic current LH instability
diamagnetic current
LaBelle& Treumann [1988]
13
Plasma heating/acceleration: LH collapse
LH collapse threshold
near RC’s inner edge
14
SUMMARY (“RC/SAPS”)
•Substorm injections quickly affect already existing SAPS.
•SAPS wave-structures (SAPSWS) follow injections of RC particles
and are generated by the current-convective instability at the forefront.
•Precipitating ion & electron fluxes, elevated electron temperatures,
and highly-structured density troughs accompany the SAPSWS.
•The energy source for the electron heating/acceleration equatorward
of the SAPSWS is likely the LH turbulence driven by the diamagnetic
current at the RC inner edge.
15
Trough & elevated Te
troug
h
troug
h
Foster et al [1994]
Elevated Te is due to heat
transport from the plasmasphere
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Plasmaspheric plasma heating/acceleration
near the RC’s inner edge
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Elevated Te and density troughs
Topside
ionosphere
Charge Transfer
Hot electrons pump N2
vibrational levels.
recombination of NO+
leads to plasma depletion.
105
Trough depth
CT rate coefficient
O + + N 2 (V ) → N O + + N * increases, and fast
400 km
18
Density trough
Scenario of the high-Te
related density trough
19