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@@ -627,9 +627,9 @@ license.
  the resulting asymmetry becomes smaller. This way variations of asymmetry
  $G_{N_e}$ synced with the period of incident light decreases.
 
- Higher excitation conditions are followed with large values of
+ Higher excitation conditions are followed by larger values of
  electric field amplitude, which lead to the appearance of high EHP
- densities causing a significant change of optical properties of
+ densities causing a significant change in the optical properties of
  silicon according to the equations (\ref{Index}). From Mie theory, the initial (at the end of Stage~3) space pattern of
  optical properties is non-homogeneous. When non-homogeneity of
  optical properties becomes strong enough it leads to the
@@ -644,11 +644,11 @@ license.
  quite different as we change the size of NP. For $R=75$~nm and
  $R=100$~nm we observe a front side asymmetry before Stage~4, however,
  the origin of it is quite different.  The $R=75$~nm NP is out of
- resonance, moreover, Mie field pattern and the one which comes from
- Stage~1 are quite similar. As soon as EHP density becomes high enough
+ resonance, moreover, Mie field pattern and the one, which comes from
+ the Stage~1 are quite similar. As soon as EHP density becomes high enough
  to change optical properties, the NP is still out of resonance,
- however, presence of EHP increases absorption in accordance with
- (\ref{Index}). This effectively leads to a partial screening, and it
+ however, the presence of EHP increases absorption in agreement with
+ (\ref{Index}). This effect effectively leads to a partial screening, and it
  becomes harder for the incident wave to penetrate deeper into EHP. Finally,
  this finishes spilling the NP`s volume with plasma reducing the
  asymmetry, see Fig.~\ref{plasma-grid}(d).
@@ -664,8 +664,8 @@ license.
  The last NP with $R=115$~nm shows the most complex behavior during
  the Stage~4. The superposition of Mie field pattern with the one from
  Stage~1 results into the presence of two EHP spatial maxima, back and
- front shifted. They serve to be a starting seed for EHP formation,
- the interplay between them forms a complex behavior of the asymmetry
+ front shifted. They serve as starting seeds for the EHP formation,
+ and an interplay between them forms a complex behavior of the asymmetry
  factor curve. Namely, the sign is changed from negative to positive
  and back during the last stage. This numerical result can hardly be
  explained in a simple qualitative manner, it is too complex to