• Chinese Optics Letters
  • Vol. 15, Issue 3, 030009 (2017)
Han Li1、3, Xin Huang1、7, Qian Cao1、4、6, Yun Zhao1, Peiyun Li1, Chenchen Wan1、5, and Andy Chong1、2、*
Author Affiliations
  • 1Department of Electro-Optics and Photonics, University of Dayton, Dayton, OH, 45469, USA
  • 2Department of Physics, University of Dayton, Dayton, OH 45469, USA
  • 3Image Sensor Group, ON Semiconductor, San Jose, CA 95134, USA
  • 4Center for Free-Electron Laser Science, Hamburg 22607, Germany
  • 5Deutsches-Elektronen Synchrotron (DESY), Hamburg 22607, Germany
  • 6Department of Physics, University of Hamburg, Hamburg 22761, Germany
  • 7Intelligent Robot System Department, SIASUN Robot & Automation Co., Ltd., Shenyang 110168, China
  • show less
    DOI: 10.3788/COL201715.030009 Cite this Article Set citation alerts
    Han Li, Xin Huang, Qian Cao, Yun Zhao, Peiyun Li, Chenchen Wan, Andy Chong. Generation of three-dimensional versatile vortex linear light bullets (Invited Paper)[J]. Chinese Optics Letters, 2017, 15(3): 030009 Copy Citation Text show less
    Formation of the vortex Airy–Bessel wave packet.
    Fig. 1. Formation of the vortex Airy–Bessel wave packet.
    Experimental setup to generate and measure the vortex Airy–Bessel wave packet. AC, Auto-correlation; XC, Cross-correlation.
    Fig. 2. Experimental setup to generate and measure the vortex Airy–Bessel wave packet. AC, Auto-correlation; XC, Cross-correlation.
    Dispersion and diffraction effects of the glass rod on (a) a Gaussian pulse and (b) and (c) a ring beam. The duration of the Gaussian beam is the same as the main lobe duration of the Airy pulse. The size of the ring is the same as the first ring of the first-order Bessel beam. The initial ring beam (b) expands ∼2 after the glass rod (c).
    Fig. 3. Dispersion and diffraction effects of the glass rod on (a) a Gaussian pulse and (b) and (c) a ring beam. The duration of the Gaussian beam is the same as the main lobe duration of the Airy pulse. The size of the ring is the same as the first ring of the first-order Bessel beam. The initial ring beam (b) expands 2 after the glass rod (c).
    3D measurements of the vortex Airy–Bessel wave pocket. The iso-intensity profiles (a) without and (d) with the glass rod. The sagittal intensity profiles (b) without and (e) with the glass. The transverse phase in the range of (−π,π) profiles (c) without and (f) with the glass rod.
    Fig. 4. 3D measurements of the vortex Airy–Bessel wave pocket. The iso-intensity profiles (a) without and (d) with the glass rod. The sagittal intensity profiles (b) without and (e) with the glass. The transverse phase in the range of (π,π) profiles (c) without and (f) with the glass rod.
    Han Li, Xin Huang, Qian Cao, Yun Zhao, Peiyun Li, Chenchen Wan, Andy Chong. Generation of three-dimensional versatile vortex linear light bullets (Invited Paper)[J]. Chinese Optics Letters, 2017, 15(3): 030009
    Download Citation