Analysis of temperature dependence of structural relaxation time in
supercooled liquids revealed a qualitatively distinct feature - a sharp,
cusp-like maxumum in the second derivative of its logarithm. It suggests that
the super-Arrhenius behavior of the structural relaxation time in glass-forming
liquids eventually crosses over to the Arrhenius behavior below the temperature
of maximum, and there is no divergence of the relaxation time at non-zero
temperature. The position of the maximum can be both above or below glass
transition temperature, depending on the sensitivity of the structural
relaxation time to changes in density. These results might turn the discussion
of the glass transition to the new avenue - the origin of the limiting
activation energy for structural relaxation at low temperatures