• Chinese Optics Letters
  • Vol. 20, Issue 3, 031405 (2022)
Zexing Zhao1, Hao Chen1, Ziming Zhang1, Jiatong Li1, Fangxiang Zhu1, Wei Wan2, Fei He2, Huifeng Wei2, Kangkang Chen2, and Peiguang Yan1、*
Author Affiliations
  • 1College of Physics and Optoelectronic Engineering, Shenzhen University, Shenzhen 518060, China
  • 2Wuhan Yangtze Soton Laser Photonics Co., Ltd., Wuhan 430205, China
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    DOI: 10.3788/COL202220.031405 Cite this Article Set citation alerts
    Zexing Zhao, Hao Chen, Ziming Zhang, Jiatong Li, Fangxiang Zhu, Wei Wan, Fei He, Huifeng Wei, Kangkang Chen, Peiguang Yan. High peak power femtosecond cylindrical vector beams generation in a chirped-pulse amplification laser system[J]. Chinese Optics Letters, 2022, 20(3): 031405 Copy Citation Text show less
    Schematic of the generation of radially polarized and azimuthally polarized beams by a typical fiber CPA system. CFBG, chirped fiber Bragg grating; WDM, wavelength division multiplexer; ISO, isolator; AOM, acoustic-optical modulator; M1 and M2, reflective mirrors.
    Fig. 1. Schematic of the generation of radially polarized and azimuthally polarized beams by a typical fiber CPA system. CFBG, chirped fiber Bragg grating; WDM, wavelength division multiplexer; ISO, isolator; AOM, acoustic-optical modulator; M1 and M2, reflective mirrors.
    (a) and (b) are the calculated intensity distribution for the formation of radial and azimuthal vector beams using linear superposition of orthogonally polarized HG modes. (c) and (d) are the measured intensity profiles by a CCD camera at maximum power.
    Fig. 2. (a) and (b) are the calculated intensity distribution for the formation of radial and azimuthal vector beams using linear superposition of orthogonally polarized HG modes. (c) and (d) are the measured intensity profiles by a CCD camera at maximum power.
    Laser performance at maximum output power. (a) The optical spectra of the Gaussian beam and radial and azimuthal vector beams. (b) The autocorrelation trace with sech2 fit.
    Fig. 3. Laser performance at maximum output power. (a) The optical spectra of the Gaussian beam and radial and azimuthal vector beams. (b) The autocorrelation trace with sech2 fit.
    Measured intensity profiles of the output vector beams after passing through a rotated linear polarizer at different output powers. (a) The radially polarized vector beam, with (b) the average output power. (c) The azimuthally polarized vector beam, with (d) the average output power. The white arrows exhibit the transmission axis of the polarizer.
    Fig. 4. Measured intensity profiles of the output vector beams after passing through a rotated linear polarizer at different output powers. (a) The radially polarized vector beam, with (b) the average output power. (c) The azimuthally polarized vector beam, with (d) the average output power. The white arrows exhibit the transmission axis of the polarizer.
    Relationship between incident Gaussian beam power and vector beam power. The dot lines are the linear fitting curves. The insert picture is the intensity profiles of Gaussian beams captured by a CCD camera at maximum output power.
    Fig. 5. Relationship between incident Gaussian beam power and vector beam power. The dot lines are the linear fitting curves. The insert picture is the intensity profiles of Gaussian beams captured by a CCD camera at maximum output power.
    Zexing Zhao, Hao Chen, Ziming Zhang, Jiatong Li, Fangxiang Zhu, Wei Wan, Fei He, Huifeng Wei, Kangkang Chen, Peiguang Yan. High peak power femtosecond cylindrical vector beams generation in a chirped-pulse amplification laser system[J]. Chinese Optics Letters, 2022, 20(3): 031405
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