• Photonics Research
  • Vol. 9, Issue 9, 1767 (2021)
Chenjing Quan1、2、†, Xiao Xing2、†, Sihao Huang2, Mengfeifei Jin3, Tongchao Shi2, Zeyu Zhang2、4、5, Weidong Xiang3、6、*, Zhanshan Wang1、7、*, and Yuxin Leng2、4、8、*
Author Affiliations
  • 1School of Physics Science and Engineering, Tongji University, Shanghai 200092, China
  • 2State Key Laboratory of High Field Laser Physics and CAS Center for Excellence in Ultra-intense Laser Science, Shanghai Institute of Optics and Fine Mechanics (SIOM), Chinese Academy of Sciences (CAS), Shanghai 201800, China
  • 3College of Chemistry and Materials Engineering, Wenzhou University, Wenzhou 325035, China
  • 4Hangzhou Institute for Advanced Study, University of Chinese Academy of Sciences, Hangzhou 310024, China
  • 5School of Physics and Electronics, Shandong Normal University, Jinan 250014, China
  • 6e-mail: xiangweidong001@126.com
  • 7e-mail: wangzs@tongji.edu.cn
  • 8e-mail: lengyuxin@mail.siom.ac.cn
  • show less
    DOI: 10.1364/PRJ.427155 Cite this Article Set citation alerts
    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[J]. Photonics Research, 2021, 9(9): 1767 Copy Citation Text show less
    Experimental setup for the Z-scan technique.
    Fig. 1. Experimental setup for the Z-scan technique.
    (a) XRD patterns and (b) PL emission spectra of CsPbCl1.5Br1.5 NCs glasses under different treatment temperature excited by femtosecond pulses at 365 nm.
    Fig. 2. (a) XRD patterns and (b) PL emission spectra of CsPbCl1.5Br1.5 NCs glasses under different treatment temperature excited by femtosecond pulses at 365 nm.
    OA Z-scan results of CsPbCl1.5Br1.5 NCs glasses with different treatment temperatures. (a) Under pump intensity 25.5 GW/cm2 at a wavelength of 800 nm and (b) under pump intensity 217 GW/cm2 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 CsPbCl1.5Br1.5 NCs glass with different treatment temperatures. (Inset, the schematic of a two-level model.)
    Fig. 3. OA Z-scan results of CsPbCl1.5Br1.5 NCs glasses with different treatment temperatures. (a) Under pump intensity 25.5  GW/cm2 at a wavelength of 800 nm and (b) under pump intensity 217  GW/cm2 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 CsPbCl1.5Br1.5 NCs glass with different treatment temperatures. (Inset, the schematic of a two-level model.)
    (a) OA Z-scan curves and (b) corresponding fitting results of β (black ball), Imχ(3) (pink), and FOM (blue) of the CsPbCl1.5Br1.5 NCs glass at the wavelength of 800 nm with different incident pump intensity.
    Fig. 4. (a) OA Z-scan curves and (b) corresponding fitting results of β (black ball), Imχ(3) (pink), and FOM (blue) of the CsPbCl1.5Br1.5 NCs glass at the wavelength of 800 nm with different incident pump intensity.
    OA Z-scan results of CsPbClxBr3−x (x=1, 1.5, 2) NCs glasses. (a) Under pump intensity 178 GW/cm2 at a wavelength of 800 nm and (b) under pump intensity 535 GW/cm2 at a wavelength of 1300 nm. (The balls are the experimental data, and the solid lines are fitting curves.) (c) PL emission spectra of CsPbClxBr3−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. 5. OA Z-scan results of CsPbClxBr3x (x=1, 1.5, 2) NCs glasses. (a) Under pump intensity 178  GW/cm2 at a wavelength of 800 nm and (b) under pump intensity 535  GW/cm2 at a wavelength of 1300 nm. (The balls are the experimental data, and the solid lines are fitting curves.) (c) PL emission spectra of CsPbClxBr3x (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.
    (a) Transmission electron microscopy (TEM) images of CsPbClxBr3-x (x = 1, 1.5, 2) NCs and (b) high-resolution TEM images of CsPbCl1.5Br1.5 NCs.
    Fig. 6. (a) Transmission electron microscopy (TEM) images of CsPbClxBr3-x (x = 1, 1.5, 2) NCs and (b) high-resolution TEM images of CsPbCl1.5Br1.5 NCs.
    (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. 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.
    (αhυ)2-hυ plot of CsPbClxBr3-x (x=1, 2, 3) NCs glass.
    Fig. 8. (αhυ)2-hυ plot of CsPbClxBr3-x (x=1,2,3) NCs glass.
    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.
    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.
    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[J]. Photonics Research, 2021, 9(9): 1767
    Download Citation