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 16 Plasmaspheric plasma heating/acceleration near the RC’s inner edge 17 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