• Photonics Research
  • Vol. 5, Issue 6, B29 (2017)
Fuming Xie1, Ni Yao2, Wei Fang2, Haifeng Wang1, Fuxing Gu1、*, and Songlin Zhuang1
Author Affiliations
  • 1Shanghai Key Laboratory of Modern Optical Systems, Engineering Research Center of Optical Instrument and System (Ministry of Education), University of Shanghai for Science and Technology, Shanghai 200093, China
  • 2State Key Laboratory of Modern Optical Instrumentation, College of Optical Science and Engineering, Zhejiang University, Hangzhou 310027, China
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    DOI: 10.1364/PRJ.5.000B29 Cite this Article Set citation alerts
    Fuming Xie, Ni Yao, Wei Fang, Haifeng Wang, Fuxing Gu, Songlin Zhuang. Single-mode lasing via loss engineering in fiber-taper-coupled polymer bottle microresonators[J]. Photonics Research, 2017, 5(6): B29 Copy Citation Text show less
    (a) Definition of Dout, Dfiber, and L. (b) Moving a microresonator droplet by using a fiber taper probe. (c) Merging two adjacent droplets into a bigger one. (d) Microscope image of many polymer bottle microresonators with similar shapes. (e) PL intensity and lasing intensity correspond to time when exciting a typical R6G-doped bottle microresonator with power around a lasing threshold. Green dots: initial PL intensity. Orange dots: initial lasing intensity.
    Fig. 1. (a) Definition of Dout, Dfiber, and L. (b) Moving a microresonator droplet by using a fiber taper probe. (c) Merging two adjacent droplets into a bigger one. (d) Microscope image of many polymer bottle microresonators with similar shapes. (e) PL intensity and lasing intensity correspond to time when exciting a typical R6G-doped bottle microresonator with power around a lasing threshold. Green dots: initial PL intensity. Orange dots: initial lasing intensity.
    Principle of single WGM lasing in a polymer bottle microresonator. (a) Multimode lasing behavior under uniform pump. (b) Single WGM lasing by adjusting the coupling position to suppress high-order modes.
    Fig. 2. Principle of single WGM lasing in a polymer bottle microresonator. (a) Multimode lasing behavior under uniform pump. (b) Single WGM lasing by adjusting the coupling position to suppress high-order modes.
    (a) Illustration of fiber-taper-coupled bottle microresonator. Definition of DFT is denoted. (b) Microscope image of a polymer bottle microresonator (Dout=5.5 μm, Dfiber=3.2 μm, and L=7.5 μm) coupled with a fiber taper. (c) Emission spectra under fiber-taper-coupled excitation with different pump pulse energy. Inset: dark-field microscope image of the microresonator with Pin=26.1 nJ. (d) Emission intensity of the 603.4 nm wavelength peak versus the pump pulse energy.
    Fig. 3. (a) Illustration of fiber-taper-coupled bottle microresonator. Definition of DFT is denoted. (b) Microscope image of a polymer bottle microresonator (Dout=5.5  μm, Dfiber=3.2  μm, and L=7.5  μm) coupled with a fiber taper. (c) Emission spectra under fiber-taper-coupled excitation with different pump pulse energy. Inset: dark-field microscope image of the microresonator with Pin=26.1  nJ. (d) Emission intensity of the 603.4 nm wavelength peak versus the pump pulse energy.
    (a) Lasing spectra and (b) their corresponding microscope images of a polymer bottle microresonator (Dout=6.1 μm, Dfiber=3.9 μm, and L=10.8 μm) under uniform and fiber taper coupling pump. (c) Lasing spectra and (d) their corresponding microscope images of another polymer bottle microresonator (Dout=5.3 μm, Dfiber=3.9 μm, and L=7.6 μm) under different diameters of fiber taper coupling pump.
    Fig. 4. (a) Lasing spectra and (b) their corresponding microscope images of a polymer bottle microresonator (Dout=6.1  μm, Dfiber=3.9  μm, and L=10.8  μm) under uniform and fiber taper coupling pump. (c) Lasing spectra and (d) their corresponding microscope images of another polymer bottle microresonator (Dout=5.3  μm, Dfiber=3.9  μm, and L=7.6  μm) under different diameters of fiber taper coupling pump.
    Electric field-intensity distributions of (a) TM431, (b) TM422, (c) TM423, and (d) TM414 modes, respectively.
    Fig. 5. Electric field-intensity distributions of (a) TM431, (b) TM422, (c) TM423, and (d) TM414 modes, respectively.
    (a) Lasing spectra and (b) their corresponding microscope images of a polymer bottle microresonator (Dout=6.1 μm, Dfiber=3.9 μm, and L=10.8 μm) under uniform and fiber taper coupling pump. (c) Lasing spectra and (d) their corresponding microscope images of another polymer bottle microresonator (Dout=5.3 μm, Dfiber=3.9 μm, and L=7.6 μm) under different diameters of fiber taper coupling pump.
    Fig. 6. (a) Lasing spectra and (b) their corresponding microscope images of a polymer bottle microresonator (Dout=6.1  μm, Dfiber=3.9  μm, and L=10.8  μm) under uniform and fiber taper coupling pump. (c) Lasing spectra and (d) their corresponding microscope images of another polymer bottle microresonator (Dout=5.3  μm, Dfiber=3.9  μm, and L=7.6  μm) under different diameters of fiber taper coupling pump.
    Fuming Xie, Ni Yao, Wei Fang, Haifeng Wang, Fuxing Gu, Songlin Zhuang. Single-mode lasing via loss engineering in fiber-taper-coupled polymer bottle microresonators[J]. Photonics Research, 2017, 5(6): B29
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