Table 2
Physical input parameters of the simulations and resulting magnetizations of the background plasma.
| ω ce / ω pe | nbg/ncs(0) | B G / B 0 | Tbg,s (K) | β s | h 0,bg,s |
|
|
σi + e(Brec) |  ,  |
|
|
|
||||||||||
| 1 | 0.1 | 0 | ion | 1.5 × 107 | 5 × 10-4 | 1 | 0.4 | 0.4 | 0.38 | 0.63, 0.53 |
| lec | ′′ | ′′ | 1.006 | 10 | 9.94 | |||||
|
|
||||||||||
| 3 | 0.31 | 0 | ion | 2 × 108 | 2.5 × 10-3 | 1 | 1.16 | 1.16 | 1.11 | 1.08, 0.73 |
| lec | ′′ | ′′ | 1.086 | 29 | 27 | |||||
|
|
||||||||||
| 3 | 0.1 | 0 | ion | 2 × 108 | 7.5 × 10-4 | 1 | 3.6 | 3.6 | 3.26 | 1.90, 0.88 |
| lec | 3 × 109 | 1.1 × 10-2 | 2.57 | 90 | 35 | |||||
|
|
||||||||||
| 3 | 0.1 | 0 | ion | 1.5 × 107 | 5.6 × 10-5 | 1 | 3.6 | 3.6 | 3.46 | 1.90, 0.88 |
| lec | ′′ | ′′ | 1.006 | 90 | 89 | |||||
|
|
||||||||||
| 3 | 0.1 | 0 | ion | 2 × 108 | 7.5 × 10-4 | 1 | 3.6 | 3.6 | 3.45 | 1.90, 0.88 |
| lec | ′′ | ′′ | 1.086 | 90 | 83 | |||||
|
|
||||||||||
| 3 | 0.1 | 0.5 | ion | 1.5 × 107 | 4.5 × 10-5 | 1 | 3.6 | 3.6 | 3.46 | 1.90, 0.81 |
| lec | ′′ | ′′ | 1.006 | 90 | 89 | |||||
|
|
||||||||||
| 3 | 0.1 | 1 | ion | 1.5 × 107 | 2.8 × 10-5 | 1 | 3.6 | 3.6 | 3.46 | 1.90, 0.66 |
| lec | ′′ | ′′ | 1.006 | 90 | 89 | |||||
|
|
||||||||||
| 6 | 0.1 | 0 | ion | 8 × 108 | 7.5 × 10-4 | 1.014 | 14.4 | 14.2 | 13.5 | 3.80, 0.97 |
| lec | ′′ | ′′ | 1.37 | 360 | 260 | |||||
Notes. The enthalpy of the background plasma is h0,bg,s. Its cold magnetization 
is defined by Eq. (4), 
by Eq. (3), and σi + e(B) by Eq. (5). In all cases, we assume Γin ~ 1. The background plasma 
includes the guide field (
). The Alfvén speeds (Sect. 2.3) do not take the temperature into account and are given in units of c. For the relativistic Alfvén speed, when there is a guide field we display the 
-projection: 
, with θ = arctanBG/B0.
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