In order to account for top-quark mass effects, we need to re-compute the Yadism pseudodata using the FFNS5. For this we need two classes of grids:
[x] Grids used to compute the matching pseudodata at high $Q^2$ which typically probe the $Q^2$ range between $30~\mathrm{GeV}^2$ and $500~\mathrm{GeV}^2$.
[x] Dense grids used for switching the Yadism predictions when computing the total inclusive cross sections.
In order to account for top-quark mass effects, we need to re-compute the Yadism pseudodata using the FFNS5. For this we need two classes of grids: