changes

main.tex

@@ -601,11 +601,11 @@ license.
  but is already high enough to change the local optical
  properties. Below the MD resonance $R \approx 100$~nm, the EHP is
  mostly localized in the front side of the NP as shown in
- Fig.~\ref{plasma-grid}(c). The highest stationary asymmetry factor
+ Fig.~\ref{plasma-grid}(c). The highest quasi-stationary asymmetry factor
  $G_{N_e} \approx 0.5$--$0.6$ is achieved in this case. At the MD
  resonance conditions, the EHP distribution has a toroidal shape and
  is much closer to the homogeneous distribution. In contrast, above
- the MD resonant size for $R = 115$~nm, and the $G_{N_e} < 0$ due to
+ the MD resonant size for $R = 115$~nm the $G_{N_e} < 0$ due to
  the fact that EHP is dominantly localized in the back side of the NP.
 
  Once again, due to presence of continous pumping the Stage~3 is
@@ -635,13 +635,12 @@ license.
  
  For the higher excitation conditions, the optical properties of
  silicon change significantly according to the equations
- (\ref{Index}). As a result, the non-resonant ED
- contributes to the forward shifting of EHP density
- maximum. Therefore, EHP is localized in the front part of the NP,
- influencing the asymmetry factor $G_{N_e}$ in
- Fig.~\ref{time-evolution}. Approximately at the pulse peak, the critical
- electron density $N_{cr} = 5\cdot{10}^{21}$~cm$^{-3}$ for silicon,
- which corresponds to the transition to quasi-metallic state
+ (\ref{Index}). As a result, the we observe the forward shifting of
+ EHP density maximum. Therefore, EHP is localized in the front part of
+ the NP, influencing the asymmetry factor $G_{N_e}$ in
+ Fig.~\ref{time-evolution}. Approximately at the pulse peak, the
+ critical electron density $N_{cr} = 5\cdot{10}^{21}$~cm$^{-3}$ for
+ silicon, which corresponds to the transition to quasi-metallic state
  $Re(\epsilon) \approx 0$ and to the electron plasma resonance, is
  overcome. Further irradiation leads to a decrease in the asymmetry
  parameter down to $G_{N_e} = 0$ for higher EHP densities, as one can