Table 6A: Evolution of variables with HYAT + ATMED CR of 2 μm Ti plasmas with P0 = 2000 for several coordinates x (μm) and instants, including the last cell affected by the irradiation before the first non-perturbed one (4.5070 g/cm3) in the material, the cell of a peak in density, two intermediate ones and the first cell affected of target on laser irradiated side, giving way to a similar parabolic evolution of mass density as equal as in HELIOS 1D, Figures 11 and Figure 12.

x (μm) at 0.1 ns 7.8317 1.9935 1.9175 1.8832 1.8523 1.8177 1.6599
ρ (g/cm3) 5.28E - 04 1.6003 4.5843 6.1419 5.5544 4.9024 4.5071
Te (eV) 70.1076 3.60E - 02 2.67E - 02 2.62E - 02 2.60E - 02 2.58E - 02 2.59E - 02
TIon (eV) 70.0909 3.60E -02 2.67E - 02 2.62E - 02 2.60E - 02 2.59E - 02 2.58E - 02
x (μm) at 0.2 ns 1.9951 1.8428 1.7945 1.7234 1.6911 1.6564 1.4999
ρ (g/cm3) 1.704 3.325 4.2568 5.7168 5.4331 4.992 4.5073
Te (eV) 2.68E - 02 2.59E - 02 2.59E - 02 2.59E - 02 2.58E - 02 2.58E - 02 2.58E - 02
TIon (eV) 2.68E - 02 2.59E - 02 2.59E - 02 2.59E - 02 2.58E - 02 2.58E - 02 2.58E - 02
x (μm) at 0.3 ns 1.9132 1.7198 1.6342 1.5665 1.5329 1.4972 1.3399
ρ (g/cm3) 2.1192 3.665 4.8962 5.5166 5.2335 4.8774 4.5073
Te (eV) 2.59E - 02 2.58E - 02 2.58E - 02 2.58E - 02 2.58E - 02 2.58E - 02 2.58E - 02
TIon (eV) 2.59E - 02 2.58E - 02 2.58E - 02 2.58E - 02 2.58E - 02 2.58E - 02 2.58E - 02
x (μm) at 0.4 ns 1.988 1.6902 1.5533 1.4836 1.4154 1.3784 1.2199
ρ (g/cm3) 1.7252 3.3378 4.7221 5.492 5.0254 4.7268 4.5071
Te (eV) 2.59E - 02 2.58E - 02 2.58E - 02 2.58E - 02 2.58E - 02 2.58E - 02 2.58E - 02
TIon (eV) 2.59E - 02 2.58E - 02 2.58E - 02 2.58E - 02 2.58E - 02 2.58E - 02 2.58E - 02
x (μm) at 0.5 ns 1.9842 1.6136 1.4337 1.3643 1.3306 1.2584 1.0999
ρ (g/cm3) 1.7262 3.3521 4.8378 5.4297 5.2798 4.7228 4.5072
Te (eV) 2.59E - 02 2.58E - 02 2.58E - 02 2.58E - 02 2.58E - 02 2.58E - 02 2.58E - 02
TIon (eV) 2.59E - 02 2.58E - 02 2.58E - 02 2.58E - 02 2.58E - 02 2.58E - 02 2.58E - 02