2005
DOI: 10.1086/429384
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Shock Geometry, Seed Populations, and the Origin of Variable Elemental Composition at High Energies in Large Gradual Solar Particle Events

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Cited by 367 publications
(370 citation statements)
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“…Many of these shock-related parameters (geometry, compression ratio, speed) are available or can be deduced from in-situ measurements at 1 AU. None, however, is actually measured in the low corona where the highest energy particles originate (≤10 R s , Tylka 2005). Moreover, the large scatter in the correlation between CME speeds and SEP peak intensities suggests a complex interplay among the CME speed, the acceleration mechanism(s) and the ambient environment.…”
Section: Science Question 6: 'What Are the Roles Of Shocks Reconnectmentioning
confidence: 99%
See 1 more Smart Citation
“…Many of these shock-related parameters (geometry, compression ratio, speed) are available or can be deduced from in-situ measurements at 1 AU. None, however, is actually measured in the low corona where the highest energy particles originate (≤10 R s , Tylka 2005). Moreover, the large scatter in the correlation between CME speeds and SEP peak intensities suggests a complex interplay among the CME speed, the acceleration mechanism(s) and the ambient environment.…”
Section: Science Question 6: 'What Are the Roles Of Shocks Reconnectmentioning
confidence: 99%
“…Fermi acceleration is the likely acceleration mechanism for quasi-parallel shocks while gradient-drift acceleration operates at quasi-perpendicular shocks (e.g., Lee 2000). The geometry of the shock seems to play a further role in the observed variability of the spectral characteristics and composition of SEPs (Tylka 2005). The shock compression ratio determines the power law index of the SEP spectrum under some simplifying assumptions such as equilibrium conditions.…”
Section: Science Question 6: 'What Are the Roles Of Shocks Reconnectmentioning
confidence: 99%
“…However, not all CMEs that satisfy the two factors can lead to large SEP events or GLEs (e.g., Kahler & Vourlidas 2005;Ding et al 2013), indicating other processes are important for producing large SEP events as well. The proposed factors include the background energetic particles that provide seed particles for the shock acceleration to high energies (e.g., Kahler et al 2000;Kahler 2001;Cliver 2006), preceding CMEs that may provide both seed particles and enhanced turbulence for more efficient particle acceleration (e.g., Gopalswamy et al 2004;Li et al 2012;Ding et al 2013;Zhao & Li 2014), and the CME shock geometry that allows a perpendicular shock region to rapidly accelerate particles to high energies (e.g., Tylka et al 2005). …”
Section: Introductionmentioning
confidence: 99%
“…Note, however, that self-excited waves produced by streaming energetic particles may further enhance particle acceleration at parallel shocks (e.g., Lee 1983Lee , 2005Li et al 2003;Rice et al 2003). When a CME-driven shock develops in the corona, the nonplanar shock front sweeps through the coronal magnetic field with a range of different shock angles, which has been proposed to have significant effects on particle acceleration (e.g., Giacalone 2005aGiacalone , 2005bTylka et al 2005). By including large-scale magnetic field variation, the transport effect is found to be important in the shock region, creating hot spots where most high-energy particles are concentrated (Guo et al 2010).…”
Section: Introductionmentioning
confidence: 99%
“…At higher energies the gradual SEP events start to show substantial event-to-event variations (Tylka et al 2005), especially in abundance ratios and charge states. It has been debated that in some cases these variations are caused either by a particle component accelerated at a solar flare accompanying the CME (Cane et al 2006), or that the DSA accelerates a mixed seed particle population that contains remnant flare suprathermals in addition to the coronal material (Tylka et al 2005).…”
Section: Introductionmentioning
confidence: 99%