| "Chanruangrith Channok,1 David Ruffolo..." |
| Slide 2 |
| Slide 3 |
| "Fe/O at IP shocks..." |
| Spectra and abundances for Nov. 24 2001 IP shock |
| Why do ESP spectra roll
over at ~ 0.1 - 10 MeV/n? (data - see also: Gosling et al. 1981; van Nes et al. 1985) |
| Finite-Time Shock Acceleration |
| We solve the PDE É |
| Rollover energy (Ec /A) |
| Slide 10 |
| Event #3: λ0 = 0.24 AU, α = 0.18 |
| Event #2: λ0 = 0.042 AU, α = 0.10 |
| Event #1: λ0 = 4.0x10-3 AU, α = 0.07 |
| Fe/O ratios |
| Slide 15 |
| É but wait Ð thereÕs
more! Key processes of interplanetary transport |
| Pitch-angle transport equation [DR, ApJ Õ95] |
| "Fitting SEP data" |
| Magnetic Configurations |
| Results of fitting GLE
data (relativistic solar protons) |
| Comparison with EM timing |
| Slide 22 |
| Thank you for your
attention ขอบคุณครับ |
| Slide 24 |
| Slide 25 |
| Early observations [Bryant et al. 1962] |
| Slide 28 |
| Upstream and SEP Abundances
(Desai et al. 2003 ApJ 558, 1149). |
| Slide 30 |
| Fe/O Ratio at shock versus Fe/O ratio upstream (Desai et al. 2003 ApJ vol. 558, 1149) |
| 3. Particle acceleration in
space: Shock acceleration |
| Fundamental mechanism of shock acceleration |
| Slide 34 |
| Slide 35 |
| Slide 36 |
| Slide 37 |
| Slide 38 |
| Slide 39 |
| Slide 40 |
| Slide 41 |
| Application to an
interplanetary shock: What if e, r vary with time? |
| r, e varying - ODE model |
| More model parameters ... |
| Numerical Results |
| Four Lines of Work: |