Jun Ren1、2, Han Lin1、5、6, Xiaorui Zheng1, Weiwei Lei3, Dan Liu3, Tianling Ren2, Pu Wang4, and Baohua Jia1、5、6、*
Author Affiliations
1Centre for Translational Atomaterials, School of Science, Computing and Engineering Technologies, Swinburne University of Technology, P. O. Box 218, Hawthorn, Victoria 3122, Australia2School of Integrated circuits, Tsinghua University, Haidian, Beijing 100084, China3Institute for Frontier Materials, Deakin University, Geelong, Victoria 3216, Australia4Institute of Laser Engineering, Beijing University of Technology, Chaoyang, Beijing 100124, China5The Australian Research Council (ARC) Industrial Transformation Training, Centre in Surface Engineering for Advanced Materials (SEAM), Swinburne University of Technology, Hawthorn, Victoria 3122, Australia6School of Science, RMIT University, Melbourne, Victoria 3000, Australiashow less
DOI: 10.29026/oes.2022.210013
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Jun Ren, Han Lin, Xiaorui Zheng, Weiwei Lei, Dan Liu, Tianling Ren, Pu Wang, Baohua Jia. Giant and light modifiable third-order optical nonlinearity in a free-standing h-BN film[J]. Opto-Electronic Science, 2022, 1(6): 210013
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Fig. 1. (a) Photo of the freestanding vacuum-assisted filtrated h-BN film. (b) TEM image of the prepared h-BN nanosheets by drop coating the ball-milled h-BN solution on a carbon-coated copper grid. (c) HRTEM image of the h-BN nanosheets with five layers. (d) Laser patterned micro-pattern of an Australian map on a free-standing h-BN film.
Fig. 2. (a) FTIR spectra of the pristine h-BN film (blue line) and laser irradiated h-BN film (red line). (b) Raman spectra with laser excitation at the wavelength of 532 nm of the pristine h-BN film (blue line) and laser irradiated h-BN film (red line). (c) Atomic structure of pristine h-BN film and localized oxidation area after laser irradiation (red dash area).
Fig. 3. (a) UV-VIS absorption characterization in the pristine h-BN film (blue line) and the laser patterned area (red line). (b) The refractive index (n0) of the pristine h-BN film (blue line) and laser patterned area (red line). (c) The extinction coefficient (ĸ) of the pristine h-BN film (blue line) and laser patterned area (red line).
Fig. 4. (a) Open aperture Z-scan results before laser oxidation. (b) Close aperture Z-scan results before laser oxidation. (c) Open aperture Z-scan results after laser irradiated optical breakdown. (d) Close aperture Z-scan result after laser oxidation.
Fig. 5. (a) The measured nonlinear absorption coefficient β and (b) nonlinear refractive index n2 of the pristine h-BN film. (c) The measured nonlinear absorption coefficient β and (d) nonlinear refractive index n2 of the laser oxidized h-BN film.
Fig. 6. FWM spectra of the h-BN film excited with pump wavelengths (865 nm, 1200 nm), compared to that of a standard gold film.
Material | β (cm/GW) | n2 (cm2/GW) | Im(χ(3)) (×10–12 esu) | Re(χ(3)) (×10–9 esu) | |χ(3)| (×10–9 esu) | FoM | Reference | Liquid exfoliated h-BN nanosheets | 74.84 | 1.2×10–13 | NA | NA | NA | NA | ref.23 | Monolayer CVD h-BN | 104 | 10 | NA | NA | NA | NA | ref.24 | Chemical-weathering h-BN | 0.079 | NA | NA | NA | NA | NA | ref.50 | Free-standing h-BN (pristine) | 4.11 | 0.0086 | 4.11 | 16.38 | 16.38 | 26.15 | Our work | Free-standing h-BN (laser oxidized) | 6.71 | 0.1638 | 4.85 | 11.84 | 11.84 | 305.14 | Our work |
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Table 1. The compared results of different kinds of h-BN with their nonlinear absorption coefficient β, nonlinear refractive index n2, the imaginary part Imχ(3) and the real part Reχ(3) and the effective third-order susceptibility |χ(3)| of complex third-order susceptibility χ(3).