• Acta Optica Sinica
  • Vol. 39, Issue 6, 0602001 (2019)
Xuelian Kong, Guizhong Zhang*, Tianqing Wang, Xin Ding, and Jianquan Yao
Author Affiliations
  • Key Laboratory of Optoelectronics Information Technology, Ministry of Education, School of Precision Instruments and Optoelectronics Engineering, Tianjin University, Tianjin 300072, China
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    DOI: 10.3788/AOS201939.0602001 Cite this Article Set citation alerts
    Xuelian Kong, Guizhong Zhang, Tianqing Wang, Xin Ding, Jianquan Yao. Dynamic-Stark-Effect Induced Distortion of Vortex Momentum Distributions of Hydrogen Atoms[J]. Acta Optica Sinica, 2019, 39(6): 0602001 Copy Citation Text show less
    Schematic illustration of ionization process of hydrogen atom
    Fig. 1. Schematic illustration of ionization process of hydrogen atom
    Vortex-shaped momentum distributions of hydrogen atom. (a)-(c) ‘Right/left’ polarization for two time-delayed pulses (first is right circularly polarized and second is left circularly polarized); (d)-(f) ‘left/right’ polarization for two time-delayed pulses
    Fig. 2. Vortex-shaped momentum distributions of hydrogen atom. (a)-(c) ‘Right/left’ polarization for two time-delayed pulses (first is right circularly polarized and second is left circularly polarized); (d)-(f) ‘left/right’ polarization for two time-delayed pulses
    Vortex-shaped momentum distributions of hydrogen atom when dynamic Stark effect is considered. (a)-(c) ‘Right/left’ polarization for two time-delayed pulses; (d)-(f) ‘left/right’ polarization for two time-delayed pulses. Laser pulses parameters are same as in Fig. 2
    Fig. 3. Vortex-shaped momentum distributions of hydrogen atom when dynamic Stark effect is considered. (a)-(c) ‘Right/left’ polarization for two time-delayed pulses; (d)-(f) ‘left/right’ polarization for two time-delayed pulses. Laser pulses parameters are same as in Fig. 2
    Transition of vortex-shaped momentum distributions from α=0 to α=0.04. (a) α=0 (vortex arms numbered as 1, 2, 3, 4); (b) α=0.04 (arrow illustrating corresponding shift of peak position of second vortex arm); (c) variation of peak intensity of each arm; (d) variation of polar angle of each arm
    Fig. 4. Transition of vortex-shaped momentum distributions from α=0 to α=0.04. (a) α=0 (vortex arms numbered as 1, 2, 3, 4); (b) α=0.04 (arrow illustrating corresponding shift of peak position of second vortex arm); (c) variation of peak intensity of each arm; (d) variation of polar angle of each arm
    Time evolution of different kinds of phases. (a)-(d) Stark phases for α=0.01, 0.02, 0.03, 0.04; (e)-(h) total phase (semiclassical phase+Stark phase) for each vortex arm; (i) comparison of total phases with (solid line) and without (dashed line) Stark effect for each vortex arm
    Fig. 5. Time evolution of different kinds of phases. (a)-(d) Stark phases for α=0.01, 0.02, 0.03, 0.04; (e)-(h) total phase (semiclassical phase+Stark phase) for each vortex arm; (i) comparison of total phases with (solid line) and without (dashed line) Stark effect for each vortex arm
    Vortex-shaped momentum distributions reproduced by integrating between 2 o.c and 8 o.c. (a) α=0.04; (b) pulse envelope function F(t) is unit constant
    Fig. 6. Vortex-shaped momentum distributions reproduced by integrating between 2 o.c and 8 o.c. (a) α=0.04; (b) pulse envelope function F(t) is unit constant
    Xuelian Kong, Guizhong Zhang, Tianqing Wang, Xin Ding, Jianquan Yao. Dynamic-Stark-Effect Induced Distortion of Vortex Momentum Distributions of Hydrogen Atoms[J]. Acta Optica Sinica, 2019, 39(6): 0602001
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