RBSP observations: Poloidal ULF waves and drift-resonance wave particle interaction Lei Dai, Kazue Takahashi, John Wygant, EFW team. EMFISIS and ECT(MagEIS)

Slides:



Advertisements
Similar presentations
Multiple reconnections and explosive events and in MST and solar flares Gennady Fiksel CMSO workshop, Princeton, NJ, Oct 5-8, 2005.
Advertisements

S. Elkington, GEM 2003 Transport in the Radiation Belts and the role of Magnetospheric ULF Waves Scot R. Elkington LASP, University of Colorado With many.
Jacob Bortnik 1,2, PhD 1 Department of Atmospheric & Oceanic Sciences, University of California at Los Angeles, CA 2 Visiting Scholar, Center for Solar-Terrestrial.
U N C L A S S I F I E D Operated by the Los Alamos National Security, LLC for the DOE/NNSA Direct measurements of chorus wave effects on electrons in the.
Electron Acceleration in the Van Allen Radiation Belts by Fast Magnetosonic Waves Richard B. Horne 1 R. M. Thorne 2, S. A. Glauert 1, N. P. Meredith 1.
Evidence at Saturn for an Inner Magnetospheric Convection Pattern, Fixed in Local Time M. F. Thomsen (1), R. L. Tokar (1), E. Roussos (2), M. Andriopoulou.
REPW-07 Brian Fraser Centre for Space Physics, University of Newcastle, Callaghan, NSW, Australia With contributions from: Jerry Goldstein, Tom Immel,
ESS 7 Lecture 14 October 31, 2008 Magnetic Storms
Ion Pickup One of the fundamental processes in space plasma physics.
Jasper S. Halekas Space Sciences Laboratory
INTRODUCTION OF WAVE-PARTICLE RESONANCE IN TOKAMAKS J.Q. Dong Southwestern Institute of Physics Chengdu, China International School on Plasma Turbulence.
Auxiliary slides. ISEE-1 ISEE-2 ISEE-1 B Locus of  = 90 degree pitch angles Will plot as a sinusoid on a latitude/longitude projection of the unit.
Prob, % WinterSummer Probability of observing downward field-aligned electron energy flux >10 mW/m 2 in winter and summer hemispheres.
ULF Wave Modelling With A Motive: Effects on Energetic Paritcles Mary Hudson, Scot Elkington, Brian Kress, Kara Perry, John Lyon, Mike Wiltberger.
Coupling the RCM to LFM Frank Toffoletto (Rice) and John Lyon (Dartmouth)
CISM Radiation Belt Models CMIT Mary Hudson CISM Seminar Nov 06.
Lecture 3 Introduction to Magnetic Storms. An isolated substorm is caused by a brief (30-60 min) pulse of southward IMF. Magnetospheric storms are large,
ULF Energy Transport Induced by Magnetospheric Boundary Oscillations Bill Lotko and Jeff Proehl Thayer School of Engineering Dartmouth College Boundary.
Magnetospheric Cavity Modes Driven by Solar Wind Dynamic Pressure Fluctuations: Initial results from LFM simulations Seth G. Claudepierre (Dartmouth College)
Magnetospheric Morphology Prepared by Prajwal Kulkarni and Naoshin Haque Stanford University, Stanford, CA IHY Workshop on Advancing VLF through the Global.
Case studies of coordinated THEMIS-SuperDARN observations of field line resonances Elsayed R. Talaat The Johns Hopkins University Applied Physics Laboratory.
Observation and Theory of Substorm Onset C. Z. (Frank) Cheng (1,2), T. F. Chang (2), Sorin Zaharia (3), N. N. Gorelenkov (4) (1)Plasma and Space Science.
Science Questions What is responsible for the "near" prompt onset of convection in the inner magnetosphere? Fast mode rarefraction wave?. How is the dayside.
Van Allen Probes, NOAA, and Ground Observations of a Pc 1 Wave Event Extending 12 Hours in MLT Mark Engebretson 1, Jennifer Posch 1, John Wygant 2, Craig.
V. M. Sorokin, V.M. Chmyrev, A. K. Yaschenko and M. Hayakawa Strong DC electric field formation in the ionosphere over typhoon and earthquake regions V.
Tuija I. Pulkkinen Finnish Meteorological Institute Helsinki, Finland
Kinetic Effects in the Magnetosphere Richard E Denton Dartmouth College.
D. Sibeck, R. Millan, H. Spence
Does Fermi Acceleration of account for variations of the fluxes of radiation belt particles observations at low altitudes during geomagnetic storms? J.
Comparisons of Inner Radiation Belt Formation in Planetary Magnetospheres Richard B Horne British Antarctic Survey Cambridge Invited.
1 Barry Mauk, Nicola Fox, David Sibeck, Shrikanth Kanekal, Joseph Grebowsky, Ramona Kessel RBSP Project Science Team This document has been reviewed for.
Outline > does the presence of NL waves affect the conclusion that QL acceleration suffices? > it depends... Outline Large amplitude whistler waves Limitations.
Large-Amplitude Electric Fields Associated with Bursty Bulk Flow Braking in the Earth’s Plasma Sheet R. E. Ergun et al., JGR (2014) Speaker: Zhao Duo.
1 The Inner Magnetosphere Nathaniel Stickley George Mason University.
Dynamics of the Radiation Belts & the Ring Current Ioannis A. Daglis Institute for Space Applications Athens.
Space Science MO&DA Programs - September Page 1 SS It is known that the aurora is created by intense electron beams which impact the upper atmosphere.
Kinetic-scale electric field structures at plasma boundaries in the inner magnetosphere (including injection fronts) David Malaspina 1, John Wygant 2,
SOLAR EXTREME EVENTS AND GRATE GEOMAGNETIC STORMS E.E. Antonova, M.V. Stepanova Skobeltsyn Institute of Nuclear Physics Moscow State University, Moscow,
Drift Resonant Interactions of Radiation Belt Electrons with ULF waves. L. G. Ozeke, I. R. Mann, A. Degeling, V. Amalraj, and I. J. Rae University of Alberta.
1 THEMIS Inner Magnetosphere Review, Dec 20, 2008 Summary of THEMIS results in the inner magnetosphere Future mission operations discussion: –Science targets.
Injections of MeV particles via intense substorm electric fields Lei Dai, John Wygant and EFW team. EFW/BARREL Science team meeting, June, 2014 Minnesota.
Coupling of the Magnetosphere and Ionosphere by Alfvén Waves at High and Mid-Latitudes Bob Lysak, Yan Song, University of Minnesota, MN, USA Murray Sciffer,
October CME Shock Event Hudson, Paral, Kress, Turner SWE ACE Solar Wind Electron Proton Alpha Monitor K0>5-Min
Scott Thaller Van Allen Probes EFW meeting University of Minnesota June 10-12, 2014.
Radiation Storms in the Near Space Environment Mikhail Panasyuk, Skobeltsyn Institute of Nuclear Physics of Lomonosov Moscow State University.
The Geoeffectiveness of Solar Cycle 23 as inferred from a Physics-Based Storm Model LWS Grant NAG Principal Investigator: Vania K. Jordanova Institute.
Multi-point observations of dispersionless injection fronts inside geostationary orbit: propagation and structure Authors (preliminary) David Malaspina.
NASA NAG Structure and Dynamics of the Near Earth Large-Scale Electric Field During Major Geomagnetic Storms P-I John R. Wygant Assoc. Professor.
1 ESS200C Pulsations and Waves Lecture Magnetic Pulsations The field lines of the Earth vibrate at different frequencies. The energy for these vibrations.
1 Magnetic components existing in geodesic acoustic modes Deng Zhou Institute of Plasma Physics, Chinese Academy of Sciences.
ENA generation mechnism Krimigis et al, 2004 Some Questions about the Interaction between Trapped Particles and Neutrals l What is the source of trapped.
Multi-Spacecraft Observation of Compressional Mode ULF Waves Excitation and Relativistic Electron Acceleration X. Shao 1, L. C. Tan 1, A. S. Sharma 1,
Magnetospheric Current System During Disturbed Times.
Nonlinear electric field structures in the inner magnetosphere D. M. Malaspina 1, L. Andersson 1, R. E. Ergun 1, J. R. Wygant 2, J. W. Bonnell 3, C. Kletzing.
Storm-dependent Radiation Belt Dynamics Mei-Ching Fok NASA Goddard Space Flight Center, USA Richard Horne, Nigel Meredith, Sarah Glauert British Antarctic.
Kinetic Alfvén Waves in the Inner Magnetosphere Triggered by an Interplanetary Shock David Malaspina 1, Seth Claudepierre 2, Kazue Takahashi 3, Allison.
ENA generation mechnism Krimigis et al, 2004 Some Questions about the Interaction between Trapped Particles and Neutrals l What is the source of trapped.
SuperDARN Observations of ULF Pulsations During a Substorm Expansion Phase Onset N. A. Frissell, J. B. H. Baker, J. M. Ruohoniemi, L. B. N. Clausen, R.
A Global Hybrid Simulation Study of the Solar Wind Interaction with the Moon David Schriver ESS 265 – June 2, 2005.
Evolution of the poloidal Alfven waves in 3D dipole geometry Jiwon Choi and Dong-Hun Lee School of Space Research, Kyung Hee University 5 th East-Asia.
Modulation of chorus wave intensity by ULF waves from Van Allen Probes Observation Lunjin Chen 1, Zhiyang Xia 1, Lei Dai 2 1 Physics Dept., The University.
Plasma Wave Excitation Regions in the Earth’s Global Magnetosphere
Magnetospheric waves Lauren Blum.
Substorm current wedge, Alfven waves, ion injections, Pi2 pulsations, and ion outflows: A THEMIS look The THEMIS team.
ESS 154/200C Lecture 19 Waves in Plasmas 2
Substorm current wedge, Alfven waves, ion injections, Pi2 pulsations, and ion outflows: A THEMIS look The THEMIS team.
Yuki Takagi1*, Kazuo Shiokawa1, Yuichi Otsuka1, and Martin Connors2  
Richard B. Horne British Antarctic Survey Cambridge UK
Three Regions of Auroral Acceleration
Presentation transcript:

RBSP observations: Poloidal ULF waves and drift-resonance wave particle interaction Lei Dai, Kazue Takahashi, John Wygant, EFW team. EMFISIS and ECT(MagEIS) team. EFW/BARREL Science team meeting, June, 2014 Minnesota

Poloidal ULF waves with intense azimuthal electric fields near equator Large azimuthal electric fields near equator: symmetric poloidal mode/fundamental mode

RBSP observations: Excitations of poloidal ULF waves through drift- resonance wave-particle interaction Dai et al., 2013 GRL, selected by AGU as a ‘Research spotlight’.

RBSP Data Oscillations of ion fluxes. Phase is energy dependent. Azimuthal electric field ~10mv/m. Radial magnetic field ~3-4nT 88keV ions is in-phase and has a high coherence with the azimuthal electric fields, direct evidence of drift-resonance At 88keV.

Drift-resonance N=0, drift-resonance with a symmetric (fundamental) mode Existence of the fundamental mode are hinted from ground observations of Giant Pulsations before. [Green, 1979; Thompson and Kivelson, 2001] Only recently have observations started to identify the fundamental (symmetric) mode of poloidal waves in space [Takahashi et al., 2011;Takahashi et al., 2013] and reveal their correspondence to Giant Pulsations on the ground [Glassmeier et al., 1999;Takahashi et al., 2011]

Identification of the fundamental mode poloidal waves Model results of the fundamental mode poloidal mode [Cummings et al., 1969] with realistic ionosphere boundary condition. courtesy of Kazue Takahashi Fundamental poloidal mode

Free energy source for the wave generation Resonant ions~ meV/G Particles lose energy to waves when drifting outward. Free energy for waves= more ions “closer” than “farther out”.

What’s next Fundamental mode Poloidal waves as the source of Giant Pulsations on the ground. The occurrence rate and location dependence of Poloidal waves produced by drift/drift-bounce resonance in the inner magnetosphere. Drift-bounce resonance instability may accelerate relativistic-energy electrons.

END

Intense poloidal ULF waves when the dst index increased at rate faster than normal.

Resonance interaction with ~ keV ions. However, This is not the core population Of ring current.

END

Intense azimuthal wave electric field and radial wave magnetic fields, with some mixture of compression magnetic field component.

Resonance interaction with ~ keV ions