TY - GEN
T1 - Proof-of-Concept Experiment on Quasi-Phase-Matching of High-Order Harmonic Generation Using a Transverse Disruptive Pulse and Selected-Zoning Method
AU - Liu, Yao Li
AU - Kao, Shin Chi
AU - Yang, Yi Yong Ou
AU - Zhang, Zhong Ming
AU - Chu, Hsu Hsin
N1 - Publisher Copyright:
© 2025 IEEE.
PY - 2025
Y1 - 2025
N2 - Quasi-phase-matching of high-order harmonic generation (QPM-HHG) based on the transverse selective-zoning method [1] is demonstrated experimentally. The experimental setup is shown in Fig. 1(a). A driving pulse (810 nm, 42 fs, 1.05 × 1015 W/cm2, S-polarized) is focused onto the Ar gas jet for HHG and a 2-D EUV flat-field spectrometer measures the 31st HHG. The focal spot size is 87 μm (FWHM), corresponding to a Rayleigh range of 39 mm which is much larger than the outlet diameter of the pulsed valve (1.6 mm). The transverse disruptive pulse polarized in the same direction passes through a delay line and then overlaps transversely with the driving pulse on the Ar gas jet. Its pulse duration is stretched to 3.3 ps (2.44 × 1012 W/cm2), ensuring complete spatial-temporal overlap with the driving pulse from the entrance to the end of the Ar gas jet. Two knife edges installed on the moving stages are put in the beamline to control the transverse pulse beam profile, and a lens is inserted to image the beam profile after the knife edges onto the gas jet for interaction length control in tomography or QPM.
AB - Quasi-phase-matching of high-order harmonic generation (QPM-HHG) based on the transverse selective-zoning method [1] is demonstrated experimentally. The experimental setup is shown in Fig. 1(a). A driving pulse (810 nm, 42 fs, 1.05 × 1015 W/cm2, S-polarized) is focused onto the Ar gas jet for HHG and a 2-D EUV flat-field spectrometer measures the 31st HHG. The focal spot size is 87 μm (FWHM), corresponding to a Rayleigh range of 39 mm which is much larger than the outlet diameter of the pulsed valve (1.6 mm). The transverse disruptive pulse polarized in the same direction passes through a delay line and then overlaps transversely with the driving pulse on the Ar gas jet. Its pulse duration is stretched to 3.3 ps (2.44 × 1012 W/cm2), ensuring complete spatial-temporal overlap with the driving pulse from the entrance to the end of the Ar gas jet. Two knife edges installed on the moving stages are put in the beamline to control the transverse pulse beam profile, and a lens is inserted to image the beam profile after the knife edges onto the gas jet for interaction length control in tomography or QPM.
UR - https://www.scopus.com/pages/publications/105016178055
UR - https://www.scopus.com/pages/publications/105016178055#tab=citedBy
U2 - 10.1109/CLEO/EUROPE-EQEC65582.2025.11109649
DO - 10.1109/CLEO/EUROPE-EQEC65582.2025.11109649
M3 - Conference contribution
AN - SCOPUS:105016178055
T3 - 2025 Conference on Lasers and Electro-Optics Europe and European Quantum Electronics Conference, CLEO/Europe-EQEC 2025
BT - 2025 Conference on Lasers and Electro-Optics Europe and European Quantum Electronics Conference, CLEO/Europe-EQEC 2025
PB - Institute of Electrical and Electronics Engineers Inc.
T2 - 2025 Conference on Lasers and Electro-Optics Europe and European Quantum Electronics Conference, CLEO/Europe-EQEC 2025
Y2 - 23 June 2025 through 27 June 2025
ER -