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Discover insights into solar flare particles and the interplanetary magnetic field's structure based on observations and models. Explore issues like velocity dispersion, particle injections, and event variations.
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Review of Observations of Particles From Solar Flares and Their Clues to the Structure of the IMF Joe Mazur The Aerospace Corporation Glenn Mason Johns Hopkins/APL Joe Dwyer Florida Institute of Technology Joe Giacalone & Randy Jokipii University of Arizona Ed Stone California Institute of Technology
Introduction • Energetic ions from solar flares sometimes arrive at Earth with velocity dispersion that allows us to see individual particle injections from active regions at the sun. • The particle events often have drop-outs in intensity across all energies that are an effect of the structure of the interplanetary magnetic field, and not of particle release at the flare source. • This talk will briefly review the observations and their interpretation using a model magnetic field that was developed to interpret the transport of energetic particles above the ecliptic plane via meandering field lines. 2
~10 seconds Velocity dispersion is common to many acceleration sites Field-aligned beams in aurora: propagation distance ~103 km GEODESIC rocket flight data courtesy of J. Clemmons Drift echoes from substorms: propagation distance ~105 km CRRES/MICS data courtesy of J. Fennell 3
Velocity dispersion in energetic particles from solar flares • Propagation distance ~108 km • Multiple particle injections from a solar active region • Particle intensity often varies by >10x during an event • Sometimes do not observe the entire injection Mason, Mazur, & Dwyer ApJ Letters 525, L133-L136,1999 4
Solar flares & escaping ions • Events have been studied since the 1970’s • Enhanced in 3He (~1000x), Ne-Fe (~10x), trans-Fe (~1000x) compared to solar corona • Sometimes fully stripped up to Si • Beams of 10-100 keV electrons • Gyroresonant wave-particle interaction in a 3-5 MK plasma may account for enrichments (3He: Temerin & Roth 1992, Ne-Fe: Miller et al. 1993) M. Aschwanden, Space Sci. Rev. 101, 1-227, 2002 5
Glimpses of small-scale (~1 hour) variations in solar energetic particles Anderson & Dougherty, Solar Phys. 103, 165-175, 1986. Buttighoffer, Astron. & Astrophysics 335, 295-302, 1998 6
Glimpses of small-scale variations in solar energetic particles McCracken & Ness, JGR 71, pp. 3315-3318, 1966 7
Ultra-Low Energy Isotope Spectrometer • 0.02-10 MeV/nucleon • Dual time-of-flight measurements for improved mass resolution • m/m ~ 0.03 8
Mass 3He 9 Time
A new look with ULEIS sensitivity • New views of the time-dependence of solar particle events • Low-energy threshold so an event lasts many hours • Large collecting area for low-intensity events that previous instruments would have missed 10
Puzzling cases of “missing” ions Mason, Mazur, & Dwyer ApJ Letters 525, L133-L136,1999 11
Time& spatial scales of events • 25 events 11/97 to 7/99 • Tallied duration of “sub-intervals” • Factored in solar wind speed to convert to a spatial size • Edges of drop-outs as sharp as ~2 minutes (~5x104 km or ~ few gyroradii of 1 MeV/n 56Fe+18) Mazur et al. ApJ Letters 532, L79-L82, 2000 12
CME-related events • Events associated with large coronal mass ejections do not have drop-outs Reames et al., ApJ, 466, 1996 13
Survey results Solar wind correlation length: Matthaeus, Goldstein, & King, JGR 91, 59-69, 1986 14
Suprathermal electrons • Common features in ions and suprathermal electrons (<1.4 keV) (akin to electron obs. of Anderson & Dougherty 1986) • Gosling et al. (2004) showed 2 events where the ions had dropouts but the electrons did not, possibly indicating a more uniform and/or broad electron source ions electrons Gosling et al. ApJ 614, 412-419, 2004 15
Simultaneous Wind/ACE observations C-Fe C-Fe • Simultaneous observations of the same flare injection on 12 August 2000: ACE & Wind spacecraft • The later arrival of empty flux tubes at Wind is consistent with solar wind convection UT 16
Numerical simulations of particle transport • Model field used to study propagation of particles from corotating interaction regions to high heliographic latitudes (Giacalone 1999) • Model was based on earlier work by Jokipii & Parker (1968) and Jokipii & Kota (1989) • Random motion of field line footpoints in the photosphere over ~4x104 km, time scales of ~1 day 17
The model followed the trajectories of 8 keV/n to 20 MeV/n oxygen from an impulsive flare • The particles traveled through pre-existing IMF structures • After ~1 day, ions were still present inside 1 AU and populated field lines spanning ~10º in longitude Giacalone, Jokipii, & Mazur, ApJ Lett. 532, 2000 18
Simulated velocity dispersion & time-dependence with two different source sizes • Same realization of the magnetic field • Large sources (corresponding to a CME shock) generate continuous event profiles Giacalone, Jokipii, & Mazur, ApJ Lett. 532, 2000 19
Closer look at dropout “edges”: iron At 1700Z: B ~ 24 nT Vsw ~ 580 km/sec 21
Questions • What observables in the 1 AU solar particle data might be used to establish the source of these dispersionless features (i.e. turbulence or field-line mixing from footpoint motion at the sun)? • What inner heliosphere measurements of the IMF and of the energetic particles, on Sentinels for example, would clearly establish the origin of these features? • Are the Ulysses observations of Jovian electrons as far as ~2 AU from Jupiter (McKibben et al. 2006) a valuable constraint on either the turbulence or random walk model? • What other observables in these data would be of use? (solar cycle dependence; statistics of the scale of the ‘dropout’ edges)
New Capability: Advanced Composition Explorer • ACE launched in August 1997 • The ACE objective is to collect samples of matter in the solar system using large instruments • We do the collecting by letting the matter come to ACE and transmitting the results to Earth 24
3He-rich Solar Flares 3He • Discovered in late 1960s • 3He/4He ratio in solar wind ~5x10-4 • The events drew attention because 3He/4He> 0.1 without any accompanying 2H or other secondaries as one might expect from spallation in the solar atmosphere • Later found enhancements of heavy ions up to iron by factor of 5-10 as well as: • Impulsive electron events • Scatter-free propagation • Often lack of any flare association on Sun • Sometimes ions fully stripped of electrons 4He Mason et al. ApJ 574, 1039--1058, 2002 25
ACE Survey of Flare Spectra • Searched for periods with clear flare velocity dispersion • Deleted events with local acceleration • Required complete observation of event (i.e. that ACE remained connected to it) for whole energy range of instrument • Cases often involved multiple injections; each event separated, and fluences calculated Mason, Dwyer, & Mazur ApJ Lett. 545, 2000 26