• Chinese Optics Letters
  • Vol. 15, Issue 11, 110201 (2017)
Meng Li1、2, Guizhong Zhang1、*, Tianqi Zhao1, Xin Ding1, and Jian Yao1
Author Affiliations
  • 1College of Precision Instrument and Optoelectronics Engineering, Tianjin University, Tianjin 300072, China
  • 2Civil Aviation Meteorological Institute, Key Laboratory of Operation Programming and Safety Technology of Air Traffic Management, Civil Aviation University of China, Tianjin 300300, China
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    DOI: 10.3788/COL201715.110201 Cite this Article Set citation alerts
    Meng Li, Guizhong Zhang, Tianqi Zhao, Xin Ding, Jian Yao. Characterizing carrier envelope phase of an isolated attosecond pulse with annular photoionization momentum spectra[J]. Chinese Optics Letters, 2017, 15(11): 110201 Copy Citation Text show less
    (Color online) (a) Schematic illustration of the overlapping of an IAP (red line) with an IR pulse: time instants t1 and t2 determine the IAP, while t3 and t4 determine the IR pulse. (b) A typical electric field pattern of the overlapped IAP and the IR pulse, for which three categories of circles are defined: the inner circle, the intermediate circles, and the outer circle. IIR=2×1014 W/cm2, IIAP=8×1011 W/cm2.
    Fig. 1. (Color online) (a) Schematic illustration of the overlapping of an IAP (red line) with an IR pulse: time instants t1 and t2 determine the IAP, while t3 and t4 determine the IR pulse. (b) A typical electric field pattern of the overlapped IAP and the IR pulse, for which three categories of circles are defined: the inner circle, the intermediate circles, and the outer circle. IIR=2×1014W/cm2, IIAP=8×1011W/cm2.
    (Color online) Electric field patterns of the superimposed IAP and IR pulse in the laser polarization plane for different overlapping parameters. The red curves indicate the superimposed segments. IIR=2×1014 W/cm2, IIAP=2×1011 W/cm2, and θ=θIR=0.
    Fig. 2. (Color online) Electric field patterns of the superimposed IAP and IR pulse in the laser polarization plane for different overlapping parameters. The red curves indicate the superimposed segments. IIR=2×1014W/cm2, IIAP=2×1011W/cm2, and θ=θIR=0.
    (Color online) Photoelectron momentum spectra for different overlapping parameters. IIR=2×1014 W/cm2, IIAP=2×1011 W/cm2, θ=θIR=0.
    Fig. 3. (Color online) Photoelectron momentum spectra for different overlapping parameters. IIR=2×1014W/cm2, IIAP=2×1011W/cm2, θ=θIR=0.
    (Color online) Photoelectron momentum spectra for different initial phases of the IAP: (a) θ=0, (b) θ=π/4, (c) θ=π/2, (d) θ=3π/4, (e) θ=π, (f) θ=5π/4, (g) θ=3π/2, (h) θ=7π/4, and (i) θ=2π. The overlapping parameter η is set to be 0.8. IIR=2×1014 W/cm2, IIAP=2×1011 W/cm2, and θIR=0.
    Fig. 4. (Color online) Photoelectron momentum spectra for different initial phases of the IAP: (a) θ=0, (b) θ=π/4, (c) θ=π/2, (d) θ=3π/4, (e) θ=π, (f) θ=5π/4, (g) θ=3π/2, (h) θ=7π/4, and (i) θ=2π. The overlapping parameter η is set to be 0.8. IIR=2×1014W/cm2, IIAP=2×1011W/cm2, and θIR=0.
    (a) Rotation angle of the annular photoelectron momentum spectra versus the IAP CEP. (b) Schematic of the rotation angle of the annular photoelectron momentum spectra. The overlapping parameter η is 0.8. IIR=2×1014 W/cm2, IIAP=2×1011 W/cm2, and θIR=0.
    Fig. 5. (a) Rotation angle of the annular photoelectron momentum spectra versus the IAP CEP. (b) Schematic of the rotation angle of the annular photoelectron momentum spectra. The overlapping parameter η is 0.8. IIR=2×1014W/cm2, IIAP=2×1011W/cm2, and θIR=0.
    Photoelectron momentum spectra with (a) θIR=0, (b) θIR=π/4, (c) θIR=π/2, (d) θIR=3π/4, (e) θIR=π, (f) θIR=5π/4, (g) θIR=3π/2, (h) θIR=7π/4, and (i) θIR=2π. IIR=2×1014 W/cm2, IIAP=2×1011 W/cm2, η=0.8, and θ=0.
    Fig. 6. Photoelectron momentum spectra with (a) θIR=0, (b) θIR=π/4, (c) θIR=π/2, (d) θIR=3π/4, (e) θIR=π, (f) θIR=5π/4, (g) θIR=3π/2, (h) θIR=7π/4, and (i) θIR=2π. IIR=2×1014W/cm2, IIAP=2×1011W/cm2, η=0.8, and θ=0.
    Photoelectron momentum spectra with (a) θ=1.2π and (b) θ=0.2π. η=0 and θIR=0. IIR=2×1014 W/cm2, and IIAP=2×1011 W/cm2.
    Fig. 7. Photoelectron momentum spectra with (a) θ=1.2π and (b) θ=0.2π. η=0 and θIR=0. IIR=2×1014W/cm2, and IIAP=2×1011W/cm2.
    Photoelectron momentum spectra for different overlapping parameters. (a) η=0.92, (b) η=0.88, (c) η=0.84, (d) η=0.8, (e) η=0.76, and (f) η=0.72. IIR=2×1014 W/cm2, IIAP=2×1011 W/cm2, and θ=θIR=0.
    Fig. 8. Photoelectron momentum spectra for different overlapping parameters. (a) η=0.92, (b) η=0.88, (c) η=0.84, (d) η=0.8, (e) η=0.76, and (f) η=0.72. IIR=2×1014W/cm2, IIAP=2×1011W/cm2, and θ=θIR=0.
    Photoelectron momentum spectra for different initial phases of the IR pulse. (a) θ=0, (b) θ=π/4, (c) θ=π/2, (d) θ=3π/4, (e) θ=π, (f) θ=5π/4, (g) θ=3π/2, (h) θ=7π/4, and (i) θ=2π. η=0.72, IIR=2×1014 W/cm2, IIAP=2×1011 W/cm2, and θIR=0.
    Fig. 9. Photoelectron momentum spectra for different initial phases of the IR pulse. (a) θ=0, (b) θ=π/4, (c) θ=π/2, (d) θ=3π/4, (e) θ=π, (f) θ=5π/4, (g) θ=3π/2, (h) θ=7π/4, and (i) θ=2π. η=0.72, IIR=2×1014W/cm2, IIAP=2×1011W/cm2, and θIR=0.
    Meng Li, Guizhong Zhang, Tianqi Zhao, Xin Ding, Jian Yao. Characterizing carrier envelope phase of an isolated attosecond pulse with annular photoionization momentum spectra[J]. Chinese Optics Letters, 2017, 15(11): 110201
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