• Chinese Optics Letters
  • Vol. 20, Issue 2, 021408 (2022)
Shengjun Huang1, Yiran Wang2, Jingliang He3, Xiancui Su2、*, and Jie Liu1、**
Author Affiliations
  • 1Shandong Provincial Engineering and Technical Center of Light Manipulations & Shandong Provincial Key Laboratory of Optics and Photonic Device, School of Physics and Electronics, Shandong Normal University, Jinan 250358, China
  • 2Shandong Key Laboratory of Optical Communication Science and Technology, School of Physics Science and Information Technology, Liaocheng University, Liaocheng 252059, China
  • 3State Key Laboratory of Crystal Materials, Institute of Novel Semiconductors, Shandong University, Jinan 250100, China
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    DOI: 10.3788/COL202220.021408 Cite this Article Set citation alerts
    Shengjun Huang, Yiran Wang, Jingliang He, Xiancui Su, Jie Liu. Nanosecond and femtosecond lasers based on black arsenic-phosphorus alloys saturable absorber[J]. Chinese Optics Letters, 2022, 20(2): 021408 Copy Citation Text show less
    (a) Raman spectrum of b-AsP nanosheets. (b) AFM image and representative height profile of b-AsP nanosheets.
    Fig. 1. (a) Raman spectrum of b-AsP nanosheets. (b) AFM image and representative height profile of b-AsP nanosheets.
    (a) Transmittance versus incident optical power intensity of b-AsP SA. (b) Time-resolved response of b-AsP SA.
    Fig. 2. (a) Transmittance versus incident optical power intensity of b-AsP SA. (b) Time-resolved response of b-AsP SA.
    (a) Experimental setup of PQS. (b) The ratio of output powers to absorbed pump powers under the CW and PQS operations. (c) The emission wavelength of the CW and PQS lasers. (d) Pulse durations and repetition rates versus absorbed pump powers. (e) Pulse energy and peak power versus absorbed pump power. (f) The pulse trains and the shortest pulse profiles with different time scales.
    Fig. 3. (a) Experimental setup of PQS. (b) The ratio of output powers to absorbed pump powers under the CW and PQS operations. (c) The emission wavelength of the CW and PQS lasers. (d) Pulse durations and repetition rates versus absorbed pump powers. (e) Pulse energy and peak power versus absorbed pump power. (f) The pulse trains and the shortest pulse profiles with different time scales.
    (a) Experimental setup of CWML laser. (b) CWML laser spectrum. (c) Autocorrelation trace. (d) The frequency spectrum with a wide and narrow span. (e) Pulse trains at the maximum pump power.
    Fig. 4. (a) Experimental setup of CWML laser. (b) CWML laser spectrum. (c) Autocorrelation trace. (d) The frequency spectrum with a wide and narrow span. (e) Pulse trains at the maximum pump power.
    Shengjun Huang, Yiran Wang, Jingliang He, Xiancui Su, Jie Liu. Nanosecond and femtosecond lasers based on black arsenic-phosphorus alloys saturable absorber[J]. Chinese Optics Letters, 2022, 20(2): 021408
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