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      Colloquium: Understanding Quantum Weak Values: Basics and Applications

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          Abstract

          Since its introduction 25 years ago, the quantum weak value has gradually transitioned from a theoretical curiosity to a practical laboratory tool. While its utility is apparent in the recent explosion of weak value experiments, its interpretation has historically been a subject of confusion. Here a pragmatic introduction to the weak value in terms of measurable quantities is presented, along with an explanation for how it can be determined in the laboratory. Further, its application to three distinct experimental techniques is reviewed. First, as a large interaction parameter it can amplify small signals above technical background noise. Second, as a measurable complex value it enables novel techniques for direct quantum state and geometric phase determination. Third, as a conditioned average of generalized observable eigenvalues it provides a measurable window into nonclassical features of quantum mechanics. In this selective review, a single experimental configuration to discuss and clarify each of these applications is used.

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          Most cited references52

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          Observation of the spin hall effect of light via weak measurements.

          We have detected a spin-dependent displacement perpendicular to the refractive index gradient for photons passing through an air-glass interface. The effect is the photonic version of the spin Hall effect in electronic systems, indicating the universality of the effect for particles of different nature. Treating the effect as a weak measurement of the spin projection of the photons, we used a preselection and postselection technique on the spin state to enhance the original displacement by nearly four orders of magnitude, attaining sensitivity to displacements of approximately 1 angstrom. The spin Hall effect can be used for manipulating photonic angular momentum states, and the measurement technique holds promise for precision metrology.
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            A Suggested Interpretation of the Quantum Theory in Terms of "Hidden" Variables. II

            David Bohm (1952)
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              Observing the average trajectories of single photons in a two-slit interferometer.

              A consequence of the quantum mechanical uncertainty principle is that one may not discuss the path or "trajectory" that a quantum particle takes, because any measurement of position irrevocably disturbs the momentum, and vice versa. Using weak measurements, however, it is possible to operationally define a set of trajectories for an ensemble of quantum particles. We sent single photons emitted by a quantum dot through a double-slit interferometer and reconstructed these trajectories by performing a weak measurement of the photon momentum, postselected according to the result of a strong measurement of photon position in a series of planes. The results provide an observationally grounded description of the propagation of subensembles of quantum particles in a two-slit interferometer.
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                Author and article information

                Journal
                30 May 2013
                2014-03-31
                Article
                10.1103/RevModPhys.86.307
                1305.7154
                52ac68d6-3f4f-4e19-b79f-9e2f79ebfc80

                http://arxiv.org/licenses/nonexclusive-distrib/1.0/

                History
                Custom metadata
                Rev. Mod. Phys. 86, 307 (2014)
                11 pages, 5 figures, published version
                quant-ph physics.optics

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