Journal of Visualized Experiments · 2014 · 13 citations · 27 references
Natural SciencesPhysicsOpticsQuantum ComputingQuantum MechanicsNonlinear OpticsOptical ResonatorsOptical SourcesPhotonic CrystalsQuantum OpticsQuantum StatesGaussian StatesLight-matter InteractionNonlinear PhotonicsOptical Parametric OscillatorsParametric OscillatorsQuantum State EngineeringQuantum States Of LightSqueezed States
Engineering non-classical states of the electromagnetic field is a central quest for quantum optics(1,2). Beyond their fundamental significance, such states are indeed the resources for implementing various protocols, ranging from enhanced metrology to quantum communication and computing. A variety of devices can be used to generate non-classical states, such as single emitters, light-matter interfaces or non-linear systems(3). We focus here on the use of a continuous-wave optical parametric oscillator(3,4). This system is based on a non-linear χ(2) crystal inserted inside an optical cavity and it is now well-known as a very efficient source of non-classical light, such as single-mode or two-mode squeezed vacuum depending on the crystal phase matching. Squeezed vacuum is a Gaussian state as its quadrature distributions follow a Gaussian statistics. However, it has been shown that number of protocols require non-Gaussian states(5). Generating directly such states is a difficult task and would require strong χ(3) non-linearities. Another procedure, probabilistic but heralded, consists in using a measurement-induced non-linearity via a conditional preparation technique operated on Gaussian states. Here, we detail this generation protocol for two non-Gaussian states, the single-photon state and a superposition of coherent states, using two differently phase-matched parametric oscillators as primary resources. This technique enables achievement of a high fidelity with the targeted state and generation of the state in a well-controlled spatiotemporal mode.
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A scheme for efficient quantum computation with linear optics
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Realization of the Einstein-Podolsky-Rosen paradox for continuous variables
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Continuous-variable optical quantum-state tomography
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Measuring the Quantum State of Light
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