• Photonics Research
  • Vol. 7, Issue 2, 137 (2019)
Hongbo Lu1、2、7、*, Cheng Wei1, Qiang Zhang1, Miao Xu1、2, Yunsheng Ding2, Guobing Zhang1、2, Jun Zhu1、2, Kang Xie3, Xiaojuan Zhang4, Zhijia Hu3、4、5、6、*, and Longzhen Qiu1、2
Author Affiliations
  • 1Key Laboratory of Special Display Technology, National Engineering Laboratory of Special Display Technology, State Key Laboratory of Advanced Display Technology, Academy of Opto-Electronic Technology, Hefei University of Technology, Hefei 230009, China
  • 2Key Laboratory of Advanced Functional Materials and Devices, Anhui Province, School of Chemistry and Chemical Engineering, Hefei University of Technology, Hefei 230009, China
  • 3School of Instrument Science and Opto-Electronics Engineering, Hefei University of Technology, Hefei 230009, China
  • 4Aston Institute of Photonic Technologies, Aston University, Birmingham B4 7ET, UK
  • 5State Key Laboratory of Environment-Friendly Energy Materials, Southwest University of Science and Technology, Mianyang 621000, China
  • 6e-mail: zhijiahu@hfut.edu.cn
  • 7e-mail: bozhilu@hfut.edu.cn
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    DOI: 10.1364/PRJ.7.000137 Cite this Article Set citation alerts
    Hongbo Lu, Cheng Wei, Qiang Zhang, Miao Xu, Yunsheng Ding, Guobing Zhang, Jun Zhu, Kang Xie, Xiaojuan Zhang, Zhijia Hu, Longzhen Qiu. Wide tunable laser based on electrically regulated bandwidth broadening in polymer-stabilized cholesteric liquid crystal[J]. Photonics Research, 2019, 7(2): 137 Copy Citation Text show less
    Chemical structures of chiral dopant R6N, liquid-crystal monomer RM257, and laser dye pyrromethene 597 and the fluorescence spectrum and absorption spectrum of laser dye PM597 in a nematic LC mixture.
    Fig. 1. Chemical structures of chiral dopant R6N, liquid-crystal monomer RM257, and laser dye pyrromethene 597 and the fluorescence spectrum and absorption spectrum of laser dye PM597 in a nematic LC mixture.
    Optical path structure.
    Fig. 2. Optical path structure.
    Emission characteristics of lasers in the CLC and PSCLC. (a) Formation of the PSCLC, (b) the transmission and corresponding laser emission spectra of the dye-doped CLC and dye-doped PSCLC samples, and (c) the emission intensity of the lasers as a function of the pump energy.
    Fig. 3. Emission characteristics of lasers in the CLC and PSCLC. (a) Formation of the PSCLC, (b) the transmission and corresponding laser emission spectra of the dye-doped CLC and dye-doped PSCLC samples, and (c) the emission intensity of the lasers as a function of the pump energy.
    Electric-field-dependent broadening of the selective reflection band together with the electrical tunability of the emission wavelength of the laser. (a) The microphotographs observed under a polarized optical microscope and photographs of the dye-doped PSCLC under various voltages, (b) the transmission and corresponding laser emission spectra of the dye-doped PSCLC under various voltages with an excited pump energy of ∼1.4 μJ, and (c) the schematic illustration of the pitch distribution under different electric fields.
    Fig. 4. Electric-field-dependent broadening of the selective reflection band together with the electrical tunability of the emission wavelength of the laser. (a) The microphotographs observed under a polarized optical microscope and photographs of the dye-doped PSCLC under various voltages, (b) the transmission and corresponding laser emission spectra of the dye-doped PSCLC under various voltages with an excited pump energy of 1.4  μJ, and (c) the schematic illustration of the pitch distribution under different electric fields.
    (a) Lasing threshold at different wavelength positions and (b) lasing threshold distribution compared to fluorescence spectrum.
    Fig. 5. (a) Lasing threshold at different wavelength positions and (b) lasing threshold distribution compared to fluorescence spectrum.
    Electric field response characteristics of the dye-doped PSCLC. (a) The relationship between the driving voltage and the peak wavelength of the laser, (b) the response speed of the laser, and (c) characterization of the electric field response stability when switching the electric field ON\OFF.
    Fig. 6. Electric field response characteristics of the dye-doped PSCLC. (a) The relationship between the driving voltage and the peak wavelength of the laser, (b) the response speed of the laser, and (c) characterization of the electric field response stability when switching the electric field ON\OFF.
    Laser emission spectra of the dye-doped PSCLC measured for right-handed and left-handed circularly polarized (RCP and LCP, respectively) states under 0 V and 31 V, respectively.
    Fig. 7. Laser emission spectra of the dye-doped PSCLC measured for right-handed and left-handed circularly polarized (RCP and LCP, respectively) states under 0 V and 31 V, respectively.
    Voltage (V)0171820212223.52630
    Wavelength (nm)673.30659.81646.73627.81613.06602.06589.79573.76561.17
    FWHM (nm)0.360.500.390.380.640.360.350.540.35
    Table 1. Peak Position and FWHM of the Laser Obtained by Different Drive Voltages
    Hongbo Lu, Cheng Wei, Qiang Zhang, Miao Xu, Yunsheng Ding, Guobing Zhang, Jun Zhu, Kang Xie, Xiaojuan Zhang, Zhijia Hu, Longzhen Qiu. Wide tunable laser based on electrically regulated bandwidth broadening in polymer-stabilized cholesteric liquid crystal[J]. Photonics Research, 2019, 7(2): 137
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