4.7 Article

Second-order hyperpolarizability and all-optical-switching of intensity-modulated spatial self-phase modulation in CsPbBr1.5I1.5 perovskite quantum dot

Journal

OPTICS AND LASER TECHNOLOGY
Volume 140, Issue -, Pages -

Publisher

ELSEVIER SCI LTD
DOI: 10.1016/j.optlastec.2021.107090

Keywords

Averaged second-order hyperpolarizability; Spatial self-phase modulation; All-optical switching

Funding

  1. NASA [NNX15AQ03A]
  2. ARO [W911NF-15-1-0535]
  3. NSF EPSCoR LINK program
  4. NASA [802892, NNX15AQ03A] Funding Source: Federal RePORTER

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The study characterized the averaged second-order hyperpolarizability of pervoskite quantum dots using intensity-dependent spatial self-phase modulation (SSPM), revealing the nonlinear refraction coefficients of the QDs and the all-optical switching characteristics. The input intensity of optical switching was estimated to be around 1.05 MW/m(2).
The averaged second-order hyperpolarizability of pervoskite (CsPbBr1.5I1.5) quantum dots (QDs) was characterized using the intensity-dependent spatial self-phase modulation (SSPM). The radial intensity variation of the Gaussian beam displayed the diffraction profile of concentric rings at the far-field due to the coherent superposition of transverse wave vectors with characteristic spatial nonlinear phases. The number of concentric rings as a function of input-intensity revealed the nonlinear refraction coefficients of the QDs. The nonlinear refraction coefficient or the real part of third-order nonlinear susceptibility as a function of concentration of QDs characterized the averaged second-order hyperpolarizability which is the nonlinear refraction coefficient of a single perovskite QD. The vertically asymmetric diffraction ring of SSPM indicates the phase distortion of the optical field due to the heat convection. All-optical switching characteristics of perovskite QDs is attributable to the intensity-modulated SSPM. The input intensity of optical switching by the SSPM was estimated to be similar to 1.05 MW/m(2).

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