Fig. 1: Classical experiment with postselection. | Nature Communications

Fig. 1: Classical experiment with postselection.

From: Quantum advantage in postselected metrology

Fig. 1

A nonoptimal input device initializes a particle in one of two states, with probabilities p and 1 − p, respectively. The particle undergoes a transformation Γθ set by an unknown parameter θ. Only the part of the transformation that acts on particles in the lower path depends on θ. If the final measurement is expensive, the particles in the upper path should be discarded: they possess no information about θ.

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