• Advanced Photonics
  • Vol. 4, Issue 2, 020501 (2022)
Xiang Hao* and Cuifang Kuang*
Author Affiliations
  • Zhejiang University, College of Optical Science and Technology, State Key Laboratory of Modern Optical Instrumentation, Hangzhou, China
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    DOI: 10.1117/1.AP.4.2.020501 Cite this Article Set citation alerts
    Xiang Hao, Cuifang Kuang. Towards extremely high-order optical nonlinearity at the nanoscale[J]. Advanced Photonics, 2022, 4(2): 020501 Copy Citation Text show less
    Schematic illustration of the MPA mechanism with different emitters. For the nonlinear process, nonlinear order n is defined by Iem∝Iexn, where Iem is the emission intensity and Iex is the excitation intensity. The photon avalanche firstly occurs in Yb3+/Pr3+ co-doped core and emissions from Yb3+ and Pr3+ all exhibit a nonlinear order of n=26. The avalanching energy can migrate to the third ion (Tm3+, Ho3+, etc.) via Yb3+ sublattice, triggering multiplied nonlinear upconversion luminescence. Credit: Qiuqiang Zhan, South China Normal University.
    Fig. 1. Schematic illustration of the MPA mechanism with different emitters. For the nonlinear process, nonlinear order n is defined by IemIexn, where Iem is the emission intensity and Iex is the excitation intensity. The photon avalanche firstly occurs in Yb3+/Pr3+ co-doped core and emissions from Yb3+ and Pr3+ all exhibit a nonlinear order of n=26. The avalanching energy can migrate to the third ion (Tm3+, Ho3+, etc.) via Yb3+ sublattice, triggering multiplied nonlinear upconversion luminescence. Credit: Qiuqiang Zhan, South China Normal University.
    Xiang Hao, Cuifang Kuang. Towards extremely high-order optical nonlinearity at the nanoscale[J]. Advanced Photonics, 2022, 4(2): 020501
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