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Table 1.
Four cases corresponding to different thermal velocities α0 and αb (in units of c), and for each case another four distinct subcases (a–d) defined by different relative number densities of the electron background n0/ne or beams nb/ne. For all cases Ub/c = 0.065 and βp = 1.96.
| Case | α0/c | αb/c | n0/ne | nb/ne | β0 | βb |
|---|---|---|---|---|---|---|
| 1.a | 0.07 | 0.07 | 0.6 | 0.20 | 1.176 | 0.392 |
| 1.b | 0.07 | 0.07 | 0.5 | 0.25 | 0.980 | 0.490 |
| 1.c | 0.07 | 0.07 | 0.3 | 0.35 | 0.588 | 0.686 |
| 1.d | 0.07 | 0.07 | 0.1 | 0.45 | 0.196 | 0.882 |
| 2.a | 0.04 | 0.07 | 0.6 | 0.20 | 0.384 | 0.392 |
| 2.b | 0.04 | 0.07 | 0.5 | 0.25 | 0.320 | 0.490 |
| 2.c | 0.04 | 0.07 | 0.4 | 0.30 | 0.256 | 0.588 |
| 2.d | 0.04 | 0.07 | 0.1 | 0.45 | 0.064 | 0.882 |
| 3.a | 0.02 | 0.07 | 0.6 | 0.20 | 0.096 | 0.392 |
| 3.b | 0.02 | 0.07 | 0.5 | 0.25 | 0.08 | 0.490 |
| 3.c | 0.02 | 0.07 | 0.3 | 0.35 | 0.048 | 0.686 |
| 3.d | 0.02 | 0.07 | 0.1 | 0.45 | 0.016 | 0.882 |
| 4.a | 0.07 | 0.04 | 0.6 | 0.20 | 1.176 | 0.128 |
| 4.b | 0.07 | 0.04 | 0.5 | 0.25 | 0.980 | 0.160 |
| 4.c | 0.07 | 0.04 | 0.4 | 0.30 | 0.784 | 0.192 |
| 4.d | 0.07 | 0.04 | 0.3 | 0.35 | 0.588 | 0.224 |
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