  Resistive superconducting zero-field transition in amorphous In-O films in
states from the vicinity of the insulator-superconductor transition is analyzed
in terms of two characteristic temperatures: the upper one, $T_{c0}$, where the
finite amplitude of the order parameter is established and the lower one,
$T_c$, where the phase ordering takes place. It follows from the
magnetoresistance measurements that the resistance in between, $T_c<T<T_{c0}$,
cannot be ascribed to dissipation by thermally dissociated vortex pairs. So, it
is not Kosterlitz-Thouless-Berezinskii transition that happens at $T_c$.
