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Detector of “Schrödinger’s Cat” States of Light

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Presentation on theme: "Detector of “Schrödinger’s Cat” States of Light"— Presentation transcript:

1 Detector of “Schrödinger’s Cat” States of Light

2 Detector of “Schrödinger’s Cat” States of Light
Scheme of the detector Photon counting Non-classical Measurements Projective but Non-Ideal ! Squeezed Vacuum

3 Detector of “Schrödinger’s Cat” States of Light
Retrodicted States and Quantum Properties : Idealized Case Projective but Non-Ideal !

4 Applications in Quantum Metrology

5 Applications in Quantum Metrology
General scheme of the Predictive Estimation of a Parameter We must wait the results of measurements !

6 Applications in Quantum Metrology
General scheme of the Retrodictive Estimation of a Parameter

7 Applications in Quantum Metrology
Fisher Information and Cramér-Rao Bound Relative distance Fisher Information

8 Applications in Quantum Metrology
Fisher Information and Cramér-Rao Bound Any estimation is limited by the Cramér-Rao bound Fisher Information is the variation rate of retrodictive probabilities under a variation of the parameter Number of repetitions

9 Applications in Quantum Metrology
Retrodictive Estimation of a Parameter Projective but Non-Ideal ! Predictive Retrodictive The result “n” is uncertain even though we prepare its target state The target state is the most probable preparation leading to the result “n”

10 Applications in Quantum Metrology
Illustration : Estimation of a phase-space displacement Optimal Minimum noise influence Fisher Information is optimal only when the measurement is projective and ideal

11 Applications in Quantum Metrology
Predictive and Retrodictive Estimations of a phase-space displacement The Quantum Cramér-Rao Bound is reached …


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