Fig. 1. Proposed scheme of two-color HHG driven by Ho-CPA as front-end.

Fig. 2. (a) The schematic layout of the Ho-CPA based on Ho:fiber oscillator, amplifier, and chirp volume Bragg grating (CVBG)-based stretcher and compressor with half-wave plate (λ/2), quarter-wave plate (λ/4), and thin-film polarizer (TFP). (b) The principle of intracavity gain shaping using an etalon in the amplifier: the etalon transmission (blue) aligned with the gain spectrum (black) that yields effectively broader net gain spectrum (red).

Fig. 3. Measured spectral evolution at the output of the Ar-gas filled 19-cell Kagome fiber at a pressure of 3 bar with an increasing input energy at a pulse duration of 3.3 ps (left) and 1.8 ps (right).

Fig. 4. Experimental layout of the two-stage compression in 7-cell Kagome fiber: the first stage comprises spectral broadening in the fiber of length 3 m and a prism compressor whose tip-to-tip separation is 1.1 m. The output of the first stage is launched in the second piece of Kagome fiber and self-compressed with the outer end placed in the gas cell. The GDD of the thin window of the gas cell is used to compensate for the small positive chirp remaining in the fiber.

Fig. 5. (a) Measured spectral evolution obtained at the output of the second stage with increasing input pulse energy for three different gas conditions in the fiber: air at 1 atm pressure; Kr gas filled in the fiber at a pressure of 3, 4, and 5 bar. (b) Measured autocorrelation trace at the input of the first stage (red), input of the second stage (blue), output of the second stage (highlighted background) with different amount of negative GDD added to optimize the remaining chirp from the second stage fiber compressor.

Fig. 6. FROG results of output pulse from the second stage based on 7-cell Kagome fiber of length 2 m filled with air. (a) Measured FROG trace shown on the full time scale; (b) FROG trace after filtering out the compressed part using a super-Gaussian filter in the time domain; (c) reconstructed FROG trace retrieved from the filtered trace; (d) measured (red) and retrieved (black) spectrum with the retrieved spectral phase in blue; (e) retrieved temporal profile (black) and retrieved temporal phase (blue) overlaid with the simulated profile in the green dotted line.

Fig. 7. (a) Measured pulse-to-pulse fluctuations for 70 min at the output of the Ho-CPA (black) and after the second stage compression (red); (b) measured output spectra from the amplifier (black), after compression from the first stage Kagome fiber (red) and from the second stage Kagome fiber (blue).

Fig. 8. Simulation results after the second stage with a fiber length of 2 m and input pulse parameters obtained from the output of the first stage. (a) Spectral evolution along the fiber length; (b) temporal evolution along the fiber length, the white dashed line indicates the pulse exit point from the fiber; (c) simulated spectrum (red); (d) simulated temporal profile (red) obtained at the end of the fiber length, overlaid with the experimental profile (black).

Fig. 9. White light generation in a thin YAG plate with pulses derived from the two-stage Kagome compressor for different input energies. The top panel shows the schematic of white light generation setup.

Table 1. Calculated Dispersion Length^a, Nonlinear Length^b, Soliton Order^c, at Different Pulse Duration for Air, Ar, and Kr Gas