2020
DOI: 10.1002/que2.38
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Spectrally uncorrelated biphotons generated from “the family of BBO crystal”

Abstract: Summary Spectrally intrinsically uncorrelated biphoton states generated from nonlinear crystals are very important but rare resources for quantum photonics and quantum information applications. Previously, such biphoton states were generated from several kinds of crystals, however, their wavelength ranges and nonlinear efficiencies were still limited for various applications. In order to explore new crystal for wider wavelength range and higher nonlinear efficiency, here we theoretically study the generation o… Show more

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Cited by 19 publications
(13 citation statements)
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“…In Refs. [41][42][43] the authors locate these states in the isomorphs of KTP, KDP, and BBO, adding to the list of wavelengths at which these states can be obtained. However, there is still a broad range of degeneracy wavelengths that cannot be achieved, and thus there is a trade-off; one must sacrifice high purity for the sake of degeneracy and indistinguishability, or one must sacrifice degeneracy and indistinguishability for the sake of high purity.…”
Section: Purity Constraints Of Traditional Bi-photon Sourcesmentioning
confidence: 99%
“…In Refs. [41][42][43] the authors locate these states in the isomorphs of KTP, KDP, and BBO, adding to the list of wavelengths at which these states can be obtained. However, there is still a broad range of degeneracy wavelengths that cannot be achieved, and thus there is a trade-off; one must sacrifice high purity for the sake of degeneracy and indistinguishability, or one must sacrifice degeneracy and indistinguishability for the sake of high purity.…”
Section: Purity Constraints Of Traditional Bi-photon Sourcesmentioning
confidence: 99%
“…However, the three GVM conditions listed in Eqs. (8)(9)(10) with the degenerated wavelengths are the most widely used cases in the experiments [40][41][42]. Especially, the GVM 3 condition has a symmetric distribution along the anti-diagonal direction, i.e., f (ω s , ω i ) = f (ω i , ω s ), which is the prerequisite condition for high-visibility HOM interferences.…”
Section: Theorymentioning
confidence: 99%
“…Here we make a simulation of such a HOM interference for PPRTP under type-0 and type-II phase-matching conditions. The simulation is performed with the following equation [41][42][43]:…”
Section: Calculation and Simulationmentioning
confidence: 99%