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Kim YH, Kim H, Park SC, Kwon Y, Yeom K, Cho W, Kwon T, Yun H, Sung JH, Lee SK, Luu TT, Nam CH, Kim KT. High-harmonic generation from a flat liquid-sheet plasma mirror. Nat Commun 2023; 14:2328. [PMID: 37087465 PMCID: PMC10122666 DOI: 10.1038/s41467-023-38087-3] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Received: 01/04/2023] [Accepted: 04/14/2023] [Indexed: 04/24/2023] Open
Abstract
High-harmonic radiation can be generated when an ultra-intense laser beam is reflected from an over-dense plasma, known as a plasma mirror. It is considered a promising technique for generating intense attosecond pulses in the extreme ultraviolet and X-ray wavelength ranges. However, a solid target used for the formation of the over-dense plasma is completely damaged by the interaction. Thus, it is challenging to use a solid target for applications such as time-resolved studies and attosecond streaking experiments that require a large amount of data. Here we demonstrate that high-harmonic radiation can be continuously generated from a liquid plasma mirror in both the coherent wake emission and relativistic oscillating mirror regimes. These results will pave the way for the development of bright, stable, and high-repetition-rate attosecond light sources, which can greatly benefit the study of ultrafast laser-matter interactions.
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Affiliation(s)
- Yang Hwan Kim
- Center for Relativistic Laser Science, Institute for Basic Science, Gwangju, 61005, Republic of Korea
| | - Hyeon Kim
- Center for Relativistic Laser Science, Institute for Basic Science, Gwangju, 61005, Republic of Korea
- Department of Physics and Photon Science, Gwangju Institute of Science and Technology, Gwangju, 61005, Republic of Korea
| | - Seong Cheol Park
- Center for Relativistic Laser Science, Institute for Basic Science, Gwangju, 61005, Republic of Korea
- Department of Physics and Photon Science, Gwangju Institute of Science and Technology, Gwangju, 61005, Republic of Korea
| | - Yongjin Kwon
- Center for Relativistic Laser Science, Institute for Basic Science, Gwangju, 61005, Republic of Korea
- Department of Physics and Photon Science, Gwangju Institute of Science and Technology, Gwangju, 61005, Republic of Korea
| | - Kyunghoon Yeom
- Center for Relativistic Laser Science, Institute for Basic Science, Gwangju, 61005, Republic of Korea
- Department of Physics and Photon Science, Gwangju Institute of Science and Technology, Gwangju, 61005, Republic of Korea
| | - Wosik Cho
- Center for Relativistic Laser Science, Institute for Basic Science, Gwangju, 61005, Republic of Korea
| | - Taeyong Kwon
- Center for Relativistic Laser Science, Institute for Basic Science, Gwangju, 61005, Republic of Korea
- Department of Physics and Photon Science, Gwangju Institute of Science and Technology, Gwangju, 61005, Republic of Korea
| | - Hyeok Yun
- Advanced Photonics Research Institute, Gwangju Institute of Science and Technology, Gwangju, 61005, Republic of Korea
| | - Jae Hee Sung
- Center for Relativistic Laser Science, Institute for Basic Science, Gwangju, 61005, Republic of Korea
- Advanced Photonics Research Institute, Gwangju Institute of Science and Technology, Gwangju, 61005, Republic of Korea
| | - Seong Ku Lee
- Center for Relativistic Laser Science, Institute for Basic Science, Gwangju, 61005, Republic of Korea
- Advanced Photonics Research Institute, Gwangju Institute of Science and Technology, Gwangju, 61005, Republic of Korea
| | - Tran Trung Luu
- Department of Physics, The University of Hong Kong, SAR Hong Kong, China
| | - Chang Hee Nam
- Center for Relativistic Laser Science, Institute for Basic Science, Gwangju, 61005, Republic of Korea
- Department of Physics and Photon Science, Gwangju Institute of Science and Technology, Gwangju, 61005, Republic of Korea
| | - Kyung Taec Kim
- Center for Relativistic Laser Science, Institute for Basic Science, Gwangju, 61005, Republic of Korea.
- Department of Physics and Photon Science, Gwangju Institute of Science and Technology, Gwangju, 61005, Republic of Korea.
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Condamine FP, Jourdain N, Hernandez JC, Taylor M, Bohlin H, Fajstavr A, Jeong TM, Kumar D, Laštovička T, Renner O, Weber S. High-repetition rate solid target delivery system for PW-class laser-matter interaction at ELI Beamlines. THE REVIEW OF SCIENTIFIC INSTRUMENTS 2021; 92:063504. [PMID: 34243562 DOI: 10.1063/5.0053281] [Citation(s) in RCA: 2] [Impact Index Per Article: 0.7] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 04/06/2021] [Accepted: 05/11/2021] [Indexed: 06/13/2023]
Abstract
L3-HAPLS (High-repetition-rate Advanced Petawatt Laser System) at ELI (Extreme Light Infrastructure) Beamlines currently delivers 0.45 PW pulses (12 J in 27 fs) at 3.3 Hz repetition rate. A fresh target surface for every shot was placed at the laser focus using an in-house tape target system designed to withstand large laser intensities and energies. It has been tested for different material thicknesses (25 and 7.6 µm), while L3-HAPLS delivered laser shots for energies ranging from 1 to 12 J. A technical description of the tape target system is given. The device can be used in diverse geometries needed for laser-matter interaction studies by providing an ≈300° free angle of view on the target in the equatorial plane. We show experimental data demonstrating the shot-to-shot stability of the device. An x-ray crystal spherical spectrometer was set up to measure the Kα yield stability, while a GHz H-field probe was used to check the shot-to-shot electromagnetic pulse generation. Finally, we discuss short and mid-term future improvements of the tape target system for efficient user operation.
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Affiliation(s)
- F P Condamine
- ELI-Beamlines Center, Institute of Physics, Czech Academy of Sciences, 25241 Dolní Brežany, Czech Republic
| | - N Jourdain
- ELI-Beamlines Center, Institute of Physics, Czech Academy of Sciences, 25241 Dolní Brežany, Czech Republic
| | - J-C Hernandez
- ELI-Beamlines Center, Institute of Physics, Czech Academy of Sciences, 25241 Dolní Brežany, Czech Republic
| | - M Taylor
- ELI-Beamlines Center, Institute of Physics, Czech Academy of Sciences, 25241 Dolní Brežany, Czech Republic
| | - H Bohlin
- ELI-Beamlines Center, Institute of Physics, Czech Academy of Sciences, 25241 Dolní Brežany, Czech Republic
| | - A Fajstavr
- ELI-Beamlines Center, Institute of Physics, Czech Academy of Sciences, 25241 Dolní Brežany, Czech Republic
| | - T M Jeong
- ELI-Beamlines Center, Institute of Physics, Czech Academy of Sciences, 25241 Dolní Brežany, Czech Republic
| | - D Kumar
- Department of Radiation and Chemical Physics, Institute of Physics of the Czech Academy of Sciences, 18200 Prague, Czech Republic
| | - T Laštovička
- ELI-Beamlines Center, Institute of Physics, Czech Academy of Sciences, 25241 Dolní Brežany, Czech Republic
| | - O Renner
- ELI-Beamlines Center, Institute of Physics, Czech Academy of Sciences, 25241 Dolní Brežany, Czech Republic
| | - S Weber
- ELI-Beamlines Center, Institute of Physics, Czech Academy of Sciences, 25241 Dolní Brežany, Czech Republic
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Ishino M, Dinh TH, Hosaka Y, Hasegawa N, Yoshimura K, Yamamoto H, Hatano T, Higashiguchi T, Sakaue K, Ichimaru S, Hatayama M, Sasaki A, Washio M, Nishikino M, Maekawa Y. Soft x-ray laser beamline for surface processing and damage studies. APPLIED OPTICS 2020; 59:3692-3698. [PMID: 32400492 DOI: 10.1364/ao.387792] [Citation(s) in RCA: 1] [Impact Index Per Article: 0.3] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 01/15/2020] [Accepted: 03/23/2020] [Indexed: 06/11/2023]
Abstract
We have developed a soft x-ray laser (SXRL) beamline equipped with an intensity monitor dedicated to ablation study such as surface processing and damage formation. The SXRL beam having a wavelength of 13.9 nm, pulse width of 7 ps, and pulse energy of around 200 nJ is generated from Ag plasma mediums using an oscillator-amplifier configuration. The SXRL beam is focused onto the sample surface by the Mo/Si multilayer coated spherical mirror. To get the correct irradiation energy/fluence, an intensity monitor composed of a Mo/Si multilayer beam splitter and an x-ray charge-coupled device camera has been installed in the beamline. The Mo/Si multilayer beam splitter has a large polarization dependence in the reflectivity around the incident angle of 45°. However, by evaluating the relationship between reflectivity and transmittance of the beam splitter appropriately, the irradiation energy onto the sample surface can be derived from the energy acquired by the intensity monitor. This SXRL beamline is available to not only the ablation phenomena but also the performance evaluation of soft x-ray optics and resists.
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Reagan BA, Li W, Urbanski L, Wernsing KA, Salsbury C, Baumgarten C, Marconi MC, Menoni CS, Rocca JJ. Hour-long continuous operation of a tabletop soft x-ray laser at 50-100 Hz repetition rate. OPTICS EXPRESS 2013; 21:28380-28386. [PMID: 24514347 DOI: 10.1364/oe.21.028380] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Indexed: 06/03/2023]
Abstract
We report the uninterrupted operation of an 18.9 nm wavelength tabletop soft x-ray laser at 100 Hz repetition rate for extended periods of time. An average power of about 0.1 mW was obtained by irradiating a Mo target with pulses from a compact diode-pumped chirped pulse amplification Yb:YAG laser. Series of up to 1.8 x 10(5) consecutive laser pulses of ~1 µJ energy were generated by displacing the surface of a high shot-capacity rotating molybdenum target by ~2 µm between laser shots. As a proof-of-principle demonstration of the use of this compact ultrashort wavelength laser in applications requiring a high average power coherent beam, we lithographically printed an array of nanometer-scale features using coherent Talbot self-imaging.
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Magnitskiy S, Nagorskiy N, Faenov A, Pikuz T, Tanaka M, Ishino M, Nishikino M, Fukuda Y, Kando M, Kawachi T, Kato Y. Observation and theory of X-ray mirages. Nat Commun 2013; 4:1936. [PMID: 23733009 PMCID: PMC3709498 DOI: 10.1038/ncomms2923] [Citation(s) in RCA: 8] [Impact Index Per Article: 0.7] [Reference Citation Analysis] [Abstract] [Track Full Text] [Download PDF] [Figures] [Journal Information] [Subscribe] [Scholar Register] [Received: 11/15/2012] [Accepted: 04/25/2013] [Indexed: 11/09/2022] Open
Abstract
The advent of X-ray lasers allowed the realization of compact coherent soft X-ray sources, thus opening the way to a wide range of applications. Here we report the observation of unexpected concentric rings in the far-field beam profile at the output of a two-stage plasma-based X-ray laser, which can be considered as the first manifestation of a mirage phenomenon in X-rays. We have developed a method of solving the Maxwell–Bloch equations for this problem, and find that the experimentally observed phenomenon is due to the emergence of X-ray mirages in the plasma amplifier, appearing as phase-matched coherent virtual point sources. The obtained results bring a new insight into the physical nature of amplification of X-ray radiation in laser-induced plasma amplifiers and open additional opportunities for X-ray plasma diagnostics and extreme ultraviolet lithography. X-ray lasers are of interest to study various properties of materials down to the atomic scale. The discovery by Magnitskiy et al. of a mirage interference effect in X-ray plasma lasers could lead to new possibilities to control the output of such lasers.
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