Choose the infinite well as 0<x<a with real eigenfunctions ψn=2/asin(nπx/a). This fixes the relative phase convention for the specified initial plus state. Each of the first two states has probability1/2 in the left half. Their cross integral is
The probability varies between 1/2±4/(3π) and remains in [0,1]. Changing the sign convention of one eigenfunction while keeping the same physical initial state requires changing its superposition coefficient too; otherwise one has prepared the other initial state and reversed the initial spatial bias.