• Chinese Optics Letters
  • Vol. 15, Issue 12, 120202 (2017)
Meng Li1、2, Guizhong Zhang1、*, Tianqi Zhao1, Xin Ding1, and Jianquan Yao1
Author Affiliations
  • 1College of Precision Instrument and Optoelectronics Engineering, Tianjin University, Tianjin 300072, China
  • 2Civil Aviation Meteorological Institute, Key Laboratory of Operation Programming & Safety Technology of Air Traffic Management, Civil Aviation University of China, Tianjin 300300, China
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    DOI: 10.3788/COL201715.120202 Cite this Article Set citation alerts
    Meng Li, Guizhong Zhang, Tianqi Zhao, Xin Ding, Jianquan Yao. Electron vortices in photoionization by a pair of elliptically polarized attosecond pulses[J]. Chinese Optics Letters, 2017, 15(12): 120202 Copy Citation Text show less
    Photoelectron momentum distributions in the polarization plane for ionization of hydrogen by right–left circularly polarized attosecond pulses with the ellipitcity (a) η1=1, η2=−1, (b) η1=0.75,η2=−0.75, (c) η1=0.5, η2=−0.5, (d) η1=0.25, η2=−0.25, (e) η1=0, η2=0, which are delayed in time by 2478 as.
    Fig. 1. Photoelectron momentum distributions in the polarization plane for ionization of hydrogen by right–left circularly polarized attosecond pulses with the ellipitcity (a) η1=1, η2=1, (b) η1=0.75,η2=0.75, (c) η1=0.5, η2=0.5, (d) η1=0.25, η2=0.25, (e) η1=0, η2=0, which are delayed in time by 2478 as.
    Photoelectron momentum distributions in the polarization plane for ionization of H by right–left circularly polarized attosecond pulses with the ellipitcity (a) η1=1, η2=−1, (b) η1=1, η2=−0.5, (c) η1=0.5, η2=−0.5, (d) η1=0.25, η2=−0.25, (e) η1=0.25, η2=−0.25, which are delayed in time by 2478 as.
    Fig. 2. Photoelectron momentum distributions in the polarization plane for ionization of H by right–left circularly polarized attosecond pulses with the ellipitcity (a) η1=1, η2=1, (b) η1=1, η2=0.5, (c) η1=0.5, η2=0.5, (d) η1=0.25, η2=0.25, (e) η1=0.25, η2=0.25, which are delayed in time by 2478 as.
    Photoelectron momentum distributions in the polarization plane for ionization of H by right–right circularly polarized attosecond pulses with the ellipitcity (a) η1=η2=1, (b) η1=η2=0.5, (c) η1=0.5, η2=0.25, (d) η1=η2=0.25, which are delayed in time by 2478 as.
    Fig. 3. Photoelectron momentum distributions in the polarization plane for ionization of H by right–right circularly polarized attosecond pulses with the ellipitcity (a) η1=η2=1, (b) η1=η2=0.5, (c) η1=0.5, η2=0.25, (d) η1=η2=0.25, which are delayed in time by 2478 as.
    Photoelectron momentum distributions in the polarization plane for ionization of H by a linearly polarized attosecond pulse and a circularly polarized attosecond pulse with the ellipitcity (a) η1=0.5, and (b) η1=1, which are delayed in time by 2478 as.
    Fig. 4. Photoelectron momentum distributions in the polarization plane for ionization of H by a linearly polarized attosecond pulse and a circularly polarized attosecond pulse with the ellipitcity (a) η1=0.5, and (b) η1=1, which are delayed in time by 2478 as.
    Photoelectron momentum distributions in the polarization plane for ionization of H by a right–left elliptically polarized attosecond pulse with the ellipitcity (a)–(c) η1=0.5, η2=−0.5, and (d)–(f) η1=1, η2=−1, delayed in time by (a) and (d) 826 as, (b) and (e) 1652 as, and (c) and (f) 2478 as.
    Fig. 5. Photoelectron momentum distributions in the polarization plane for ionization of H by a right–left elliptically polarized attosecond pulse with the ellipitcity (a)–(c) η1=0.5, η2=0.5, and (d)–(f) η1=1, η2=1, delayed in time by (a) and (d) 826 as, (b) and (e) 1652 as, and (c) and (f) 2478 as.
    Meng Li, Guizhong Zhang, Tianqi Zhao, Xin Ding, Jianquan Yao. Electron vortices in photoionization by a pair of elliptically polarized attosecond pulses[J]. Chinese Optics Letters, 2017, 15(12): 120202
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