Choose the infinite well as with real eigenfunctions . This fixes the relative phase convention for the specified initial plus state. Each of the first two states has probability in the left half. Their cross integral is
The evolving superposition therefore gives
Since , the angular frequency and ordinary frequency are
The probability varies between and remains in . 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.
Figure 1.
Original two-state transition and left-half well probabilities over two recurrence periods
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