“…(The at coordinates t 1 , ..., t n can be expressed via Casimirs of the original Poisson bracket and action variables and wave n umbers along the invariant tori -see details in [53,54].) To de ne a tensor c (t) o n M (or, equivalently, the \primary free energy" F(t)) we need to use a semiclassical limit of the -function of the original hierarchy [87,88,44,45,133]. For the dispersionless limit the de nition of the semiclassical -function reads log semiclassical (T 0 ; T 1 ; : : : ) = lim !0 2 log ( t 0 ; t 1 ; : : : ) : (6:20) Then F = log semiclassical (6:21) for a particular -function of the hierarchy.…”