2018
DOI: 10.1103/physreva.98.043813
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Gaussian functions are optimal for waveguided nonlinear-quantum-optical processes

Abstract: Many nonlinear optical technologies require the two-mode spectral amplitude function that describes them-the joint spectral amplitude (JSA)-to be separable. We prove that the JSA factorizes only when the incident pump field and phase-matching function are Gaussian functions. We show this by mapping our problem to a known result, in continuous variable quantum information, that only squeezed states remain unentangled when combined on a beam splitter. We then conjecture that only a squeezed state minimizes entan… Show more

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Cited by 29 publications
(18 citation statements)
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“…Finally, we can easily run circuit simulations on special-purpose hardware like GPUs or TPUs. 68 By taking advantage of these additional functionalities of the TensorFlow backend, we can straightforwardly perform optimization and machine learning on quantum circuits in Strawberry Fields [64,65]. A complete code example for optimization of a quantum circuit is located in Appendix C.…”
Section: Optimization and Quantum Machine Learningmentioning
confidence: 99%
“…Finally, we can easily run circuit simulations on special-purpose hardware like GPUs or TPUs. 68 By taking advantage of these additional functionalities of the TensorFlow backend, we can straightforwardly perform optimization and machine learning on quantum circuits in Strawberry Fields [64,65]. A complete code example for optimization of a quantum circuit is located in Appendix C.…”
Section: Optimization and Quantum Machine Learningmentioning
confidence: 99%
“…In this paper, we consider three distinct pulse shapes: 1) Decaying Exponential, i.e. the shape of a photon emitted from a two-level quantum emitter [61], 2) Gaussian, which can be obtained from a customized heralded spontaneous parametric downconversion source [62], and 3) Rising Exponential, which is known to give maximum excitation for a single qubit [31] (see Appendix B).…”
Section: Atom Excitation Probabilitymentioning
confidence: 99%
“…στ p ≫ 1, the . Under such conditions the JSA is expressed as the product of two Gaussian functions, which is the ideal expression for obtaining a factorable state [31] in general and possesses no sidelobes in particular. It becomes more factorable as the quantity C = σ 2 1 + σ 2 2 T s T i + (στ p ) 2 gets smaller, and, in principle, can become completely factorable when C = 0.…”
Section: Measurements Of the Joint Spectral Densitymentioning
confidence: 99%