George C. Ho1, David Lario1, Robert B. Decker1, Mihir I. Desai2,

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Presentation transcript:

Transient Shocks and Associated Energetic Particle Events Observed by ACE during Solar Cycle 23 George C. Ho1, David Lario1, Robert B. Decker1, Mihir I. Desai2, Qiang Hu3, Justin Kasper4 1The Johns Hopkins University Applied Physics Laboratory, 2Southwest Research Institute 3Institute of Geophysics and Planetary Physics, University of California at Riverside 4Center for Space Research, MIT Acknowledgement: The work at JHU/APL is supported under NASA grant NNG04GA84G

Outline Introduction ACE ESP events survey Time-intensity profiles Spectral evolution Spectral profiles Selected ACE/Wind ESP events Summary

Energetic Storm Particle (ESP) Events Energetic Storm Particle (ESP) events are increases of energetic charged particle intensities that are observed upstream and downstream of interplanetary (IP) shocks. ESP events are observed most commonly in ion intensities and have time scales ~hours. The energetic particle signatures of ESP events have been studied extensively during the 80s (Tsurutani and Lin, 1985; van Nes et al., 1984; Scholer, 1988; Decker, 1981; etc.). Lee [1983] modeled the energetic particles within ESP events with a diffusive shock acceleration model at a quasi-parallel shock, while Decker [1983] successfully applied the shock drift model to explain the shock-spike events. Fortunately, most shocks that we observe at Earth orbit have already lost most of their strength and hence do not produce strong ESP events. However, a number of shocks still retain their strength when they reach 1 AU, and locally accelerate particles up to 10 MeV. In addition, although relatively rare, there have been reports of strong ESP events that can accelerate particles up to 30 MeV, which can affect the safety of humans and systems in space. Because large ESP events are scarce, the opportunity to study them is rare.

Time-intensity Profiles of SEP and ESP Here are couple cartoons of the particle intensity profile looks like at 1 AU for both SEP and ESP events for a strong and weak shock. When the shock first forms at the Sun, it can accelerate particle into high energy and high intensity. We can measure these particles at 1 AU and call them solar energetic particle events. As the shock propagates from the Sun to 1 AU depending upon if it’s still a strong or weak shock, the particle time intensity profiles can either be flat and reach an upper limit (as was discussed by Reames as particle streaming limit) or decrease over time. But when the shock is closed to the s/c, we see the trapped particle population around the shock that we call ESP events. Reames, 1999

SEP and ESP During Cycle 22 Here are some of the stronger events in cycle 22. The dotted lines are the streaming limit for particle intensity at different energy channels from 10 to 500 MeV. Reames, 1999

Large ESP Events Lario and Simnett., 2003

Event Selection From February 1, 1998 to October 28, 2003 the SWEPAM and MAG teams identified a total of 298 interplanetary shocks. Out of these 298 interplanetary shocks, we have selected 191 shocks that were fast and forward and with clear evidences of being driven by or related to the passage of ICMEs, i.e., we have excluded: reverse shocks, slow shocks, shocks associated with CIRs and shocks associated with other structures such as magnetic holes or stream-stream interactions. A total of 97 shocks. We have also excluded those shocks associated with the most intense SEP events (such as the Bastille Day 2000 event, or the November 2001 events). A total of 10 shocks. A preliminary list of Wind interplanetary shocks indicate 124 of the 191 shocks were also detected by Wind, 5 ESP events were selected to examine in detail the spatial and temporal variations of these events in the Earth’s vicinity.

Classification of the 191 ESP events according to their intensity-time profile 63% IP shocks accelerated >47 keV ions 32% IP shocks accelerated >2 MeV ions 20% IP shocks accelerated >38 keV e-

Upstream Magnetic Field Direction (θBn) Smith (1985)

Correlation between shock parameters and particle signatures Vs

Correlation between shock parameters and particle signatures MA

Correlation between shock parameters and particle signatures rn

Correlation between shock parameters and particle signatures

Correlation between shock parameters and particle signatures

1300-1448 UT 297/2003 Magnetic field power spectrum pc = proton gyrofrequency Normalized magnetic helicity spectrum 297/2003

Ambient, shock and peak spectra

Correlation between ambient and peak spectra

Heavy Ion Spectral Signature Desai et al., 2004

ACE Wind Locations 128 events

March 18, 2002 (DOY 77) #1

April 23, 2003 (DOY 113) #2

July 17, 2002 (DOY 198) #4

Shock Compression Comparison

Shock Speed Comparison

Shock Travel Time vs Observed Transit Time

Physical Separation vs Inferred Separation

Summary We classified 191 ESP events detected on ACE according to: Energetic ion and electron time-intensity profile Spectral index 63% of transient forward IP shock accelerated ions at >47 keV, while only 32% IP shock accelerated ions at >1.9 MeV The spectral index of energetic ion: Monotonically increased across the shock; or Fluctuated across the shock crossing Most of the ion spectral index do not follow the diffusive shock theoretical prediction for an equilibrium spectrum (many shock interactions) Ion spectra often soften at the shock We studied 5 ESP events using particles, field, and plasma instruments on both ACE and Wind The particle intensity and spectra index were very similar at the two spacecraft despite the fact that they were in time separate by more than 400 RE

Summary (continue) The agreement between the calculated transits times using the fitted shock speeds on ACE with the actual measured transit times is good only up to ~30 minutes The disagreement between estimated transit time and measured transit time increase when the GSE Y separation were large (> 200 RE) This implies a) the shock may not be spherically symmetric at 1 AU, or; b) the shock may not propagate radially, or both There is relatively good agreement between the fitted shock speed and density compression ratio for the same shock on Wind and ACE