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. 14, Issue 11, 111401(2016)

1.88  μm, Ba(NO3)2-based Raman laser pumped by a potassium-titanyl-phosphate-based optical parametric oscillator laser

Junchi Chen1,2,3, Xiao Zou2,3, Yujie Peng2、*, Hongpeng Su2,3, and Yuxin Leng2、**
Author Affiliations
  • 1School of Physics Science and Engineering, Tongji University, Shanghai 200092, China
  • 2State Key Laboratory of High Field Laser Physics, Shanghai Institute of Optics and Fine Mechanics, Chinese Academy of Sciences, Shanghai 201800, China
  • 3University of Chinese Academy of Science, Beijing 100190, China
    • show less
    Full TextGet PDF
    Figures&Tables (6)
    Equations (0)
    References (21)
    Cited By (2)
    Tools
    Paper Information
    Topics
    Figures & Tables(6)
    Schematic layout of the Ba(NO3)2 SRS laser pumped by the KTP OPO laser.

    Fig. 1. Schematic layout of the Ba(NO3)2 SRS laser pumped by the KTP OPO laser.

    Download full size
    View in Article
    Spectra of the monitored OPO and Raman lasers.

    Fig. 2. Spectra of the monitored OPO and Raman lasers.

    Download full size
    View in Article
    (a) Output energy of the 1.57 μm laser in terms of the energy of the 1064 nm laser; (b) output energy of the 1.88 μm laser in terms of the energy of the 1.57 μm laser.

    Fig. 3. (a) Output energy of the 1.57 μm laser in terms of the energy of the 1064 nm laser; (b) output energy of the 1.88 μm laser in terms of the energy of the 1.57 μm laser.

    Download full size
    View in Article
    Laser output energy stability in terms of time of up to 600 s. (a) Energy fluctuation of the 1064 nm laser versus time; (b) energy fluctuation of the 1.57 μm laser versus time; (c) energy fluctuation of the 1.88 μm laser versus time.

    Fig. 4. Laser output energy stability in terms of time of up to 600 s. (a) Energy fluctuation of the 1064 nm laser versus time; (b) energy fluctuation of the 1.57 μm laser versus time; (c) energy fluctuation of the 1.88 μm laser versus time.

    Download full size
    View in Article
    Temporal pulse shape of lasers. (a) 1064 nm laser with a pulse width of 7.7 ns; (b) 1.57 μm laser with a pulse width of 6.3 ns; (c) 1.88 μm with a pulse width of 5.4 ns with the maximum output energy.

    Fig. 5. Temporal pulse shape of lasers. (a) 1064 nm laser with a pulse width of 7.7 ns; (b) 1.57 μm laser with a pulse width of 6.3 ns; (c) 1.88 μm with a pulse width of 5.4 ns with the maximum output energy.

    Download full size
    View in Article
    Beam profiles of the lasers under the maximum SRS output energy. (a) 1064 nm; (b) 1.57 μm; (c) 1.88 μm.

    Fig. 6. Beam profiles of the lasers under the maximum SRS output energy. (a) 1064 nm; (b) 1.57 μm; (c) 1.88 μm.

    Download full size
    View in Article
    Tools

    Get Citation

    Copy Citation Text

    Junchi Chen, Xiao Zou, Yujie Peng, Hongpeng Su, Yuxin Leng, "1.88  μm, Ba(NO3)2-based Raman laser pumped by a potassium-titanyl-phosphate-based optical parametric oscillator laser," Chin.Opt.Lett. 14, 111401 (2016)

    Download Citation

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

    Category: Lasers and Laser Optics

    Received: May. 16, 2016

    Accepted: Sep. 23, 2016

    Published Online: Aug. 2, 2018

    The Author Email: Yujie Peng (yjpeng@siom.ac.cn), Yuxin Leng (lengyuxin@mail.siom.ac.cn)

    DOI:10.3788/COL201614.111401

    Topics

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