Quantum and CircuitsReading edition

Identical histograms can hide orthogonal states

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Identical histograms can hide orthogonal states

Erasing the signs leaves sample probabilities unchanged and changes the state. Let \(\chi_n=|c_{12}(n)|/\sqrt{48}\). Both states are normalized and

\[ |\psi_n|^2=|\chi_n|^2\quad\text{for every }n, \qquad\langle\psi,\chi\rangle=0. \]
The top panel shows the phase information carried by negative amplitudes. The bottom panel is shared by the two states because measurement in this basis depends only on squared magnitudes.
The top panel shows the phase information carried by negative amplitudes. The bottom panel is shared by the two states because measurement in this basis depends only on squared magnitudes.

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The orthogonality follows from equal positive-support and negative-support energies: each contributes \(24\) before division by \(48\). A sample-basis probability histogram therefore cannot reconstruct the coherent state.

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