• Photonics Research
  • Vol. 6, Issue 5, 396 (2018)
Jinqiu Zheng1, Ao Yang1, Teng Wang1, Xianglong Zeng1、*, Ning Cao2, Mei Liu2, Fufei Pang1, and Tingyun Wang1
Author Affiliations
  • 1Key Laboratory of Specialty Fiber Optics and Optical Access Networks, Joint International Research Laboratory of Specialty Fiber Optics and Advanced Communication, Shanghai Institute for Advanced Communication and Data Science, Shanghai University, Shanghai 200444, China
  • 2School of Mechatronic Engineering and Automation, Shanghai University, Shanghai 200072, China
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    DOI: 10.1364/PRJ.6.000396 Cite this Article Set citation alerts
    Jinqiu Zheng, Ao Yang, Teng Wang, Xianglong Zeng, Ning Cao, Mei Liu, Fufei Pang, Tingyun Wang. Wavelength-switchable vortex beams based on a polarization-dependent microknot resonator[J]. Photonics Research, 2018, 6(5): 396 Copy Citation Text show less
    Experimental setup used to excite OVB pulse. WDM, wavelength division multiplexing coupler; EDF, erbium-doped fiber; PC, polarization controller; OSA, optical spectrum analyzer; CCD, charge-coupled infrared camera; PMF, polarization-maintaining fiber.
    Fig. 1. Experimental setup used to excite OVB pulse. WDM, wavelength division multiplexing coupler; EDF, erbium-doped fiber; PC, polarization controller; OSA, optical spectrum analyzer; CCD, charge-coupled infrared camera; PMF, polarization-maintaining fiber.
    Microscopy image of (a) the fabricated MKR and (b) the overlapping region.
    Fig. 2. Microscopy image of (a) the fabricated MKR and (b) the overlapping region.
    Spectral response of MKR: (a) Transmission spectrum with different incident states of polarization (SOP); (b) transmission spectra from 1553 nm to 1557 nm; and (c) polarization-dependent loss of the MKR.
    Fig. 3. Spectral response of MKR: (a) Transmission spectrum with different incident states of polarization (SOP); (b) transmission spectra from 1553 nm to 1557 nm; and (c) polarization-dependent loss of the MKR.
    Simulation results: (a) Coupling efficiency as a function of the wavelengths; and (b) power exchange in the coupling region when LP01 mode in SMF converts to LP11 mode in FMF.
    Fig. 4. Simulation results: (a) Coupling efficiency as a function of the wavelengths; and (b) power exchange in the coupling region when LP01 mode in SMF converts to LP11 mode in FMF.
    Output near-field intensity distribution from a mode selective coupler by inputting a femtosecond pulse. (a), (e) Intensity profiles of the LP11 and LP21 modes; (b), (f) donut-shaped OAM mode patterns when pressing the output FMF; (c) and (d), and (g) and (h) corresponding clockwise and anticlockwise spiral interferograms of OAM±1 and OAM±2, respectively.
    Fig. 5. Output near-field intensity distribution from a mode selective coupler by inputting a femtosecond pulse. (a), (e) Intensity profiles of the LP11 and LP21 modes; (b), (f) donut-shaped OAM mode patterns when pressing the output FMF; (c) and (d), and (g) and (h) corresponding clockwise and anticlockwise spiral interferograms of OAM±1 and OAM±2, respectively.
    Output spectra of successively tunable (a) single-, (b) dual-, (c) triple-, and (d) quadruple-wavelength lasing operations.
    Fig. 6. Output spectra of successively tunable (a) single-, (b) dual-, (c) triple-, and (d) quadruple-wavelength lasing operations.
    Stability of triple-wavelength output spectrum. (a) Repeat scans of triple-wavelength output spectrum every minute. (b) Power fluctuation (black) and central wavelength (blue) of each channel in the triple-wavelength output every minute.
    Fig. 7. Stability of triple-wavelength output spectrum. (a) Repeat scans of triple-wavelength output spectrum every minute. (b) Power fluctuation (black) and central wavelength (blue) of each channel in the triple-wavelength output every minute.
    Near-field distribution of LP11 intensities, OAM patterns, spiral interferograms, and the out spectra of wavelength-switchable laser. Four columns present (a)–(e) single-, (f)–(j) dual-, (k)–(o) triple-, and (p)–(t) quadruple-wavelength lasing operations. First row, LP11 intensity profiles; second row, donut-shaped mode patterns of vortex beams; third and fourth rows, corresponding clockwise and anticlockwise spiral interferograms; and fifth row, the output spectra.
    Fig. 8. Near-field distribution of LP11 intensities, OAM patterns, spiral interferograms, and the out spectra of wavelength-switchable laser. Four columns present (a)–(e) single-, (f)–(j) dual-, (k)–(o) triple-, and (p)–(t) quadruple-wavelength lasing operations. First row, LP11 intensity profiles; second row, donut-shaped mode patterns of vortex beams; third and fourth rows, corresponding clockwise and anticlockwise spiral interferograms; and fifth row, the output spectra.
    Jinqiu Zheng, Ao Yang, Teng Wang, Xianglong Zeng, Ning Cao, Mei Liu, Fufei Pang, Tingyun Wang. Wavelength-switchable vortex beams based on a polarization-dependent microknot resonator[J]. Photonics Research, 2018, 6(5): 396
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