Distinguishable Terms in a State

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SUMMARY

The discussion centers on the analysis of interference in quantum states represented by the proposition ##P\equiv \psi \equiv AB^\perp + e^{j \theta} A^\perp B##. It emphasizes the need for a projection operator ##\hat\Pi## corresponding to a specific eigenvalue of the operator ##\hat{O}## to determine the probability of observing that eigenvalue. The key question posed is how to ascertain whether interference occurs as the phase ##\theta## varies, specifically whether to sum-then-square or square-then-sum in calculations. The presence of interference is confirmed if the probability calculated as $$ <\psi|\hat\Pi|\psi>$$ changes with variations in ##\theta##.

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Let's say we have a proposition (or state, if we prefer) ##P\equiv \psi \equiv AB^\perp + e^{j \theta} A^\perp B## where, e.g., ##A^{\perp}## indicates some ket that is orthogonal to ##A##.

We also have an operator ##\hat{O}## .

Without reference to a physical context, is there a test to say whether there will be interference in the probability of observing a given eigenvalue of ##\hat{O}## as we vary the phase ##\theta## ? In other words, how would a shut-up-and-calculate robot know whether it should sum-then-square or it should square-then-sum?
 
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We need to get a projection operator ##\hat\Pi## corresponding to a given eigenvalue of ##\hat O##. Then the probability is calculated as $$ <\psi|\hat\Pi|\psi>$$ If it changes when θ changes, then we have interference.
 
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