Chenjing Quan, Xiao Xing, Sihao Huang, Mengfeifei Jin, Tongchao Shi, Zeyu Zhang, Weidong Xiang, Zhanshan Wang, Yuxin Leng, "Nonlinear optical properties of CsPbClxBr3-x nanocrystals embedded glass," Photonics Res. 9, 1767 (2021)

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- Photonics Research
- Vol. 9, Issue 9, 1767 (2021)

Fig. 1. Experimental setup for the Z-scan technique.

Fig. 2. (a) XRD patterns and (b) PL emission spectra of CsPbCl 1.5 Br 1.5 NCs glasses under different treatment temperature excited by femtosecond pulses at 365 nm.

Fig. 3. OA Z-scan results of CsPbCl 1.5 Br 1.5 NCs glasses with different treatment temperatures. (a) Under pump intensity 25.5 GW / cm 2 at a wavelength of 800 nm and (b) under pump intensity 217 GW / cm 2 at a wavelength of 1300 nm. (The balls are the experimental data, and the solid lines are fitting curves.) The fitting results of (c) β and (d) γ of CsPbCl 1.5 Br 1.5 NCs glass with different treatment temperatures. (Inset, the schematic of a two-level model.)

Fig. 4. (a) OA Z-scan curves and (b) corresponding fitting results of β (black ball), Im χ ( 3 ) (pink), and FOM (blue) of the CsPbCl 1.5 Br 1.5 NCs glass at the wavelength of 800 nm with different incident pump intensity.

Fig. 5. OA Z-scan results of CsPbCl x Br 3 − x (x = 1 , 1.5, 2) NCs glasses. (a) Under pump intensity 178 GW / cm 2 at a wavelength of 800 nm and (b) under pump intensity 535 GW / cm 2 at a wavelength of 1300 nm. (The balls are the experimental data, and the solid lines are fitting curves.) (c) PL emission spectra of CsPbCl x Br 3 − x (x = 1 , 1.5, 2) NCs glasses for 500°C treatment temperature excited by femtosecond pulses at 365 nm; (d) fitting the results of 2PA coefficient (β , purple bar) and 3PA coefficient (γ , red bar) obtained in (a) and (b), respectively.

Fig. 6. (a) Transmission electron microscopy (TEM) images of CsPbClx Br3-x (x = 1, 1.5, 2) NCs and (b) high-resolution TEM images of CsPbCl1.5Br1.5 NCs.

Fig. 7. (a) Amplified spontaneous emission (ASE) measurement on CsPbCl1.5Br1.5 NCs glass under an 800 nm pulsed laser at room temperature and (b) corresponding full-width at half-maxima (FWHM) and output as a function of incident pump intensity.

Fig. 8. (α h υ )2-h υ plot of CsPbClx Br3-x (x = 1 , 2 , 3 ) NCs glass.

Fig. 9. Open-aperture Z-scan curves of the (a) CsPbCl1Br2 and (b) CsPbCl2Br1 NCs glasses at the wavelength of 800 nm with different incident pump intensity.

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