Table 1 Simulations with a0 = 10: Density after hydrodynamic expansion n0/γncr, radius of the sphere R or alternative box length of the cube Lc, simulation box length Lbox and simulation cell size Δx for a laser wavelength λ = 1 μm.
From: Optimizing laser-driven proton acceleration from overdense targets
n0/γncr | R [μm] | Lc[μm] | Lbox[μm] | Δx [μm] |
|---|---|---|---|---|
4 | 10 | 16 | 39.81 | 0.011 |
2 | 25 | 20 | 50.16 | 0.016 |
1 | 32 | 25 | 63.19 | 0.023 |
0.67 | 36 | 29 | 72.34 | 0.028 |
0.5 | 40 | 32 | 79.62 | 0.032 |
0.28 | 48 | 39 | 95.95 | 0.042 |
0.2 | 54 | 44 | 108.06 | 0.049 |
0.1 | 68 | 55 | 136.14 | 0.049 |