(a) Schematic diagram of the experimental set-up for the spatio-temporal measurement of the IAP generated in a tow-color driving field. BS, beam splitter; DM, dichroic mirror; DL, delay line; HWP, half-wave plate; WGP, wire grid polarizer. (b) Spatially-resolved harmonic spectrum driven by the 1300 nm fundamental field alone. (c) Same as (b), but for the two-color driving field synthesized by the 1300 nm fundamental and 800 nm assistant laser fields. (d) On-axis harmonic spectra driven by the one-color (red line) and two-color (blue line) laser field, respectively.

(a) Schematic diagram of the experimental set-up for the spatio-temporal measurement of the IAP generated in a tow-color driving field. BS, beam splitter; DM, dichroic mirror; DL, delay line; HWP, half-wave plate; WGP, wire grid polarizer. (b) Spatially-resolved harmonic spectrum driven by the 1300 nm fundamental field alone. (c) Same as (b), but for the two-color driving field synthesized by the 1300 nm fundamental and 800 nm assistant laser fields. (d) On-axis harmonic spectra driven by the one-color (red line) and two-color (blue line) laser field, respectively.

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Article
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Characterizing an isolated attosecond pulse (IAP) is essential for its potential applications. A complete characterization of an IAP ultimately requires the determination of its electric field in both time and space domains. However, previous methods, like the widely-used RABBITT and attosecond streaking, only measure the temporal profile of the atto...

Citations

... The HHG process can be well explained by the semiclassical three-step model: electronic ionization, acceleration, and recombination in intense fields [2]. In recent decades, HHG is attracting intense interest worldwide because of its potential applications in the production of a coherent XUV source and attosecond pulses (APs) [3][4][5]. This allows tracing and controlling ultrafast processes in many disciplines with high spatio-temporal resolution [6,7]. ...
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... backed with a phosphor screen [53]. The spectrally resolved images are recorded using a charge-coupled device (CCD) camera. ...
Preprint
High-energy, few-cycle laser pulses are essential for numerous applications in the fields of ultrafast optics and strong-field physics, due to their ultrafast temporal resolution and high peak intensity. In this work, different from the traditional hollow-core fibers and multiple thin solid plates, we represent the first demonstration of the octave-spanning supercontinuum broadening by utilizing multiple ultrathin liquid films (MTLFs) as the nonlinear media. The continuum covers a range from 380 to 1050 nm, corresponding to a Fourier transform limit pulse width of 2.5 fs, when 35 fs Ti:sapphire laser pulse is applied on the MTLFs. The output pulses are compressed to 3.9 fs by employing chirped mirrors. Furthermore, a continuous high-order harmonic spectrum up to the 33rd order is realized by subjecting the compressed laser pulses to interact with Kr gas. The utilization of flowing water films eliminates permanent optical damage and enables wider and stronger spectrum broadening. Therefore, this MTLFs scheme provides new solutions for the generation of highly efficient femtosecond supercontinuum and nonlinear pulse compression, with potential applications in the fields of strong-field physics and attosecond science.
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