• Acta Photonica Sinica
  • Vol. 50, Issue 1, 1 (2021)
Hushan WANG1, Huabao CAO1, Liangwen PI1, Pei HUANG1, Xianglin WANG1, Peng XU1, Hao YUAN1、2, Xin LIU1、2, Yishan WANG1、*, Wei ZHAO1, and Yuxi FU1
Author Affiliations
  • 1State Key Laboratory of Transient Optics and Photonics, Xi'an Institute of Optics and Precision Mechanics of CAS, Xi'an709, China
  • 2University of Chinese Academy of Sciences, Beijing100049, China
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    DOI: 10.3788/gzxb20215001.0132001 Cite this Article
    Hushan WANG, Huabao CAO, Liangwen PI, Pei HUANG, Xianglin WANG, Peng XU, Hao YUAN, Xin LIU, Yishan WANG, Wei ZHAO, Yuxi FU. Research Progress of Attosecond Pulse Generation and Characterization (Invited)[J]. Acta Photonica Sinica, 2021, 50(1): 1 Copy Citation Text show less
    Characteristic of HHG spectrum
    Fig. 1. Characteristic of HHG spectrum
    Three step model of HHG
    Fig. 2. Three step model of HHG
    Reported photon energies of HHGs in X ray band
    Fig. 3. Reported photon energies of HHGs in X ray band
    HHGs with pump lasers with different wavelengths[28]
    Fig. 4. HHGs with pump lasers with different wavelengths[28]
    Microscopic mechanisms for solid-state HHG[58]
    Fig. 5. Microscopic mechanisms for solid-state HHG[58]
    Worldwide development of isolated attosecond pulse bandwidth
    Fig. 6. Worldwide development of isolated attosecond pulse bandwidth
    The characteristic properties of the HHG pulses in spectral and temporal domain
    Fig. 7. The characteristic properties of the HHG pulses in spectral and temporal domain
    The contributions of different half cycles to the generated high harmonic spectra with amplitude gating[76]
    Fig. 8. The contributions of different half cycles to the generated high harmonic spectra with amplitude gating[76]
    The scheme of polarization gating[86]
    Fig. 9. The scheme of polarization gating[86]
    The time-dependent ellipticity of the laser pulse formed in the polarization gating[89]
    Fig. 10. The time-dependent ellipticity of the laser pulse formed in the polarization gating[89]
    Control of the generation of HHG in gases based on two color gating[90]
    Fig. 11. Control of the generation of HHG in gases based on two color gating[90]
    Simulated HHG spectrum based on two color gating[95]
    Fig. 12. Simulated HHG spectrum based on two color gating[95]
    13 Scheme of GDOG[101]
    Fig. 13. 13 Scheme of GDOG[101]
    Comparison of DOG and GDOG laser fields[101]
    Fig. 14. Comparison of DOG and GDOG laser fields[101]
    Theory of attosecond lighthouse and the corresponding high harmonic spectrum[76]
    Fig. 15. Theory of attosecond lighthouse and the corresponding high harmonic spectrum[76]
    Principle and experimental setup of noncollinear gating[104]
    Fig. 16. Principle and experimental setup of noncollinear gating[104]
    Transmission spectra and dispersion property of different materials[115]
    Fig. 17. Transmission spectra and dispersion property of different materials[115]
    Si and SiC reflection efficiencies in XUV band at the pump pulse's (800 nn) Brewster angle[116]
    Fig. 18. Si and SiC reflection efficiencies in XUV band at the pump pulse's (800 nn) Brewster angle[116]
    Change of harmonic photon energy with the recombination time[115]
    Fig. 19. Change of harmonic photon energy with the recombination time[115]
    Principle of chirped multilayer mirror[123]
    Fig. 20. Principle of chirped multilayer mirror[123]
    The quantum paths contributing to the photoelectrons in RABITT[132]
    Fig. 21. The quantum paths contributing to the photoelectrons in RABITT[132]
    The experimental setup of RABITT[132]
    Fig. 22. The experimental setup of RABITT[132]
    Effect of a strong laser field on the photoelectrons ionized by attosecond pulses[135], dashed circle-velocity distribution without the laser field, solid circle-distribution with the laser field
    Fig. 23. Effect of a strong laser field on the photoelectrons ionized by attosecond pulses[135], dashed circle-velocity distribution without the laser field, solid circle-distribution with the laser field
    Principle of the all-optical FROG measurement of an isolated attosecond pulse[68]
    Fig. 24. Principle of the all-optical FROG measurement of an isolated attosecond pulse[68]
    Experimental layout of the all-optical FROG for isolated attosecond pulse reconstruction and the retrieved result[68]
    Fig. 25. Experimental layout of the all-optical FROG for isolated attosecond pulse reconstruction and the retrieved result[68]
    Reported results of soft X-ray attosecond pulses with energy up to nJ level[148]
    Fig. 26. Reported results of soft X-ray attosecond pulses with energy up to nJ level[148]
    Electrically neutral mediaSymbols of elementsIonization energyOver barrier ionization intensity
    HeliumHe24.587 eV1.36×1016 W/cm2
    NeonNe20.18 eV4.34×1015 W/cm2
    ArgonAr15.76 eV1.16×1015 W/cm2
    KryptonKr14 eV6.33×1014 W/cm2
    HydrogenH13.6 eV5.47×1014 W/cm2
    XenonXe12.13 eV3.11×1014 W/cm2
    Table 1. Common electrically neutral gaseous media, the corresponding ionization energy and over barrier ionization intensity
    Parameters of driving laserResults of soft X-ray attosecond pulsesReference/Year
    Pulse widthEnergyWavelengthHighest photon energyPhoton flux and energy
    7.8 fs353 μJ1 μm waveband350 eVOver 106 photons/s within the water window

    [141]

    2014

    32 fs2 mJ2.1 μm450 eV

    1.5×106 photons/s/1%bandwidth at 350 eV

    1×106 photons/s/1%bandwidth at 410 eV

    [144]

    2016

    11.7 fs400 μJ1 850 nm550 eV

    (7.3±0.1)×107 photons/s within the water window

    Pulse energy up to 2.9±0.1 pJ

    [145]

    2016

    30 fs10 mJ1.8 μm543 eV2.9×103 photons/s/1%bandwidth at 280 eV

    [146]

    2018

    12 fs550 μJ1.8 μm600 eV

    (1.4±0.4)×109 photons/s within the water window

    Pulse energy up to 71±18 pJ

    [147]

    2018

    Table 2. Research progress of soft X ray attosecond pulses
    Hushan WANG, Huabao CAO, Liangwen PI, Pei HUANG, Xianglin WANG, Peng XU, Hao YUAN, Xin LIU, Yishan WANG, Wei ZHAO, Yuxi FU. Research Progress of Attosecond Pulse Generation and Characterization (Invited)[J]. Acta Photonica Sinica, 2021, 50(1): 1
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