  We extend the proof from arXiv:1012.3137, which interprets the AGT relation
as the Hubbard-Stratonovich duality relation to the case of 5d gauge theories.
This involves an additional q-deformation. Not surprisingly, the extension
turns out to be trivial: it is enough to substitute all relevant numbers by
q-numbers in all the formulas, Dotsenko-Fateev integrals by the Jackson sums
and the Jack polynomials by the MacDonald ones. The problem with extra poles in
individual Nekrasov functions continues to exist, therefore, such a proof works
only for \beta = 1, i.e. for q=t in MacDonald's notation. For \beta\ne 1 the
conformal blocks are related in this way to a non-Nekrasov decomposition of the
LMNS partition function into a double sum over Young diagrams.
