Table 5B: Evolution of variables with HYAT + ATMED CR of 25/50 μm silicon plasmas at several coordinates x (μm) and instants, including the last cell affected by the irradiation before the first non-perturbed one (2.330 g/cm3) and cells inside/outside the target on laser irradiated side, observing a heat wave propagation from the irradiated side outwards the Si target with time progression as in Figure 10.
x (μm) at 0.03 ns | N1: 27.5108 | N1: 24.8751 | N1: 24.7083 | N4: 52.5110 | N4: 49.9194 | N4: 49.5833 |
ρ (g/cm3) | 1.22E - 02 | 2.3242 | 2.3299 | 1.22E - 02 | 2.2555 | 2.3299 |
Te (eV) | 0.9962 | 2.58E - 02 | 2.58E - 02 | 1.9266 | 2.58E - 02 | 2.58E - 02 |
TIon (eV) | 0.996 | 2.58E - 02 | 2.58E - 02 | 1.9257 | 2.58E - 02 | 2.58E - 02 |
x (μm) at 0.1 ns | N1: 27.6905 | N1: 24.7085 | N1: 24.4583 | N4: 52.7576 | N4: 49.7533 | N4: 49.2500 |
ρ (g/cm3) | 1.20E - 02 | 2.3183 | 2.3299 | 1.14E - 02 | 2.2457 | 2.3299 |
Te (eV) | 1.1099 | 2.58E - 02 | 2.58E - 02 | 2.6072 | 2.58E - 02 | 2.58E - 02 |
TIon (eV) | 1.1097 | 2.58E - 02 | 2.58E - 02 | 2.6063 | 2.58E - 02 | 2.58E - 02 |
x (μm) at 0.6 ns | N1: 30.2972 | N1: 24.3966 | N1: 23.6250 | N4: 57.1741 | N4: 49.4509 | N4: 48.2499 |
ρ (g/cm3) | 7.33E - 03 | 1.9305 | 2.3299 | 4.66E - 03 | 1.8952 | 2.3299 |
Te (eV) | 1.278 | 2.58E - 02 | 2.58E - 02 | 3.6157 | 2.58E - 02 | 2.58E - 02 |
TIon (eV) | 1.2778 | 2.58E - 02 | 2.58E - 02 | 3.6146 | 2.58E - 02 | 2.58E - 02 |
x (μm) at 3 ns | N1: 66.4673 | N1: 21.8487 | N1: 20.2083 | N4: 114.0613 | N4: 47.1475 | N4: 45.2499 |
ρ (g/cm3) | 9.42E - 04 | 1.9762 | 2.3299 | 5.25E - 04 | 1.9694 | 2.3299 |
Te (eV) | 3.624 | 2.58E - 02 | 2.58E - 02 | 17.1967 | 2.58E - 02 | 2.58E - 02 |
TIon (eV) | 3.594 | 2.58E - 02 | 2.58E - 02 | 17.2004 | 2.58E - 02 | 2.58E - 02 |
x (μm) at 6 ns | N1: 128.2621 | N1: 19.2237 | N1: 16.9583 | N4: 430.8407 | N4: 44.1979 | N4: 38.5832 |
ρ (g/cm3) | 3.61E - 04 | 1.9764 | 2.3299 | 1.29E - 04 | 1.9649 | 2.3301 |
Te (eV) | 38.8305 | 2.58E - 02 | 2.58E - 02 | 368.8628 | 2.58E - 02 | 2.58E - 02 |
TIon (eV) | 38.7025 | 2.58E - 02 | 2.58E - 02 | 368.8627 | 2.58E - 02 | 2.58E - 02 |