  The actual definition of the Nekrasov functions participating in the AGT
relations implies a peculiar choice of contours in the LMNS and Dotsenko-Fateev
integrals. Once made explicit and applied to the original triply-deformed
(6-dimensional) version of these integrals, this approach reduces the AGT
relations to symmetry in q_{1,2,3}, which is just an elementary identity for an
appropriate choice of the integration contour (which is, however, a little
non-traditional). We illustrate this idea with the simplest example of N=(1,1)
U(1) SYM in six dimensions, however, all other cases can be evidently
considered in a completely similar way.
