Journals Articles Conferences News About CLP
Submit a paper Email Alert
Search
Search
Articles
Journals
News
Advanced Search
Top Searches
2D MaterialsTransformation opticsQuantum PhotonicsSmall lasersSemiconductor UV PhotonicsSupersymmetric microring laser arrays

Chinese Optics Letters, Volume. 20, Issue 2, 021408(2022)

Nanosecond and femtosecond lasers based on black arsenic-phosphorus alloys saturable absorber

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
    • show less
    Full TextGet PDF
    Figures&Tables (4)
    Equations (3)
    References (41)
    Cited By (5)
    Tools
    Paper Information
    Topics
    Figures & Tables(4)
    (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.

    Download full size
    View in Article
    (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.

    Download full size
    View in Article
    (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.

    Download full size
    View in Article
    (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.

    Download full size
    View in Article
    Tools

    Get Citation

    Copy Citation Text

    Shengjun Huang, Yiran Wang, Jingliang He, Xiancui Su, Jie Liu, "Nanosecond and femtosecond lasers based on black arsenic-phosphorus alloys saturable absorber," Chin. Opt. Lett. 20, 021408 (2022)

    Download Citation

    EndNote(RIS)BibTexPlain Text
    Set citation alerts for article
    Save article for my favorites
    Paper Information

    Category: Lasers, Optical Amplifiers, and Laser Optics

    Received: Oct. 28, 2021

    Accepted: Dec. 2, 2021

    Published Online: Dec. 24, 2021

    The Author Email: Xiancui Su (suxiancui@lcu.edu.cn), Jie Liu (jieliu@sdnu.edu.cn)

    DOI:10.3788/COL202220.021408

    Topics

    laser devices and laser physics
    Lasers and Laser Optics
    Laser physics
    laser manufacturing
    Instrumentation, Measurement and Metrology