text: on the model (see above). The purely two-dimensional character of the KMC was extended to 
  
  a ‘pseudo three-dimensional’ one by making the effective chemical potential dependent on the 
  
  mean liquid coverage [38]. As the latter is related to a mean ﬁlm thickness, this corresponds to 
  
  the introduction of a ‘global’ thickness-dependent disjoining pressure into the evaporation term 
  
  without an explicit consideration of a ﬁlm thickness. The amended model can reproduce bimodal 
  
  structures that are beyond the scope of the purely two-dimensional model [38, 39]. Fully three- 
  
  dimensional models are also discussed in the literature [76, 77]. 