We present an important correction to the Langer-Ambegaokar-McCumber-Halperin
theory for the resistive state of a 1D superconductor. We establish that the
identification of the saddle on the free energy surface over which Langer and
Ambegaokar had claimed the system to move in order to form thermally excited
phase slip centres is wrong. With the help of an exact solution we show that
the system has to overcome a similar free energy barrier but can actually have
vanishing amplitude of superconducting phase at a point unlike the
Langer-Ambegaokar solution