Gigawatt-class, tabletop, isolated-attosecond-pulse light source
Powerful and stable attosecond pulse sources have the potential for wide application in ultrafast science. For this purpose, we have produced a soft X-ray supercontinuum with a pulse energy of 0.24 µJ using high-order harmonics from a multi-terawatt, 10 Hz, three-channel waveform synthesizer [ Sci....
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Published in | Optica Vol. 9; no. 4; p. 360 |
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Main Authors | , , |
Format | Journal Article |
Language | English |
Published |
20.04.2022
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Abstract | Powerful and stable attosecond pulse sources have the potential for wide application in ultrafast science. For this purpose, we have produced a soft X-ray supercontinuum with a pulse energy of 0.24 µJ using high-order harmonics from a multi-terawatt, 10 Hz, three-channel waveform synthesizer [ Sci. Adv. 6 , eaay2802 ( 2020 ) STAMCV 1468-6996 10.1126/sciadv.aay2802 ]. Here, we report an attosecond streaking scheme that is designed to measure this isolated attosecond pulse at a low-repetition rate. We retrieved a pulse duration of 226 attoseconds (as), demonstrating the realization of 1.1 gigawatt isolated as pulses on a tabletop, which compares favorably to an X-ray free-electron laser in a large facility. |
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AbstractList | Powerful and stable attosecond pulse sources have the potential for wide application in ultrafast science. For this purpose, we have produced a soft X-ray supercontinuum with a pulse energy of 0.24 µJ using high-order harmonics from a multi-terawatt, 10 Hz, three-channel waveform synthesizer [ Sci. Adv. 6 , eaay2802 ( 2020 ) STAMCV 1468-6996 10.1126/sciadv.aay2802 ]. Here, we report an attosecond streaking scheme that is designed to measure this isolated attosecond pulse at a low-repetition rate. We retrieved a pulse duration of 226 attoseconds (as), demonstrating the realization of 1.1 gigawatt isolated as pulses on a tabletop, which compares favorably to an X-ray free-electron laser in a large facility. |
Author | Xue, Bing Takahashi, Eiji J. Midorikawa, Katsumi |
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CitedBy_id | crossref_primary_10_1103_PhysRevApplied_18_034048 crossref_primary_10_3788_CJL231535 crossref_primary_10_1063_5_0206718 crossref_primary_10_3390_photonics10030331 crossref_primary_10_1134_S0021364023603883 crossref_primary_10_3367_UFNr_2022_12_039297 crossref_primary_10_31857_S1234567823010020 crossref_primary_10_1088_1361_6455_ac8f01 crossref_primary_10_3367_UFNe_2022_12_039297 crossref_primary_10_1007_s11141_023_10267_7 crossref_primary_10_1088_1674_1056_aca6d2 crossref_primary_10_1134_S0021364023600763 crossref_primary_10_1364_JOSAB_503633 crossref_primary_10_1364_OL_521645 crossref_primary_10_1088_1367_2630_ace8b3 crossref_primary_10_1016_j_optcom_2023_129475 crossref_primary_10_1103_PhysRevA_108_023506 crossref_primary_10_1134_S0021364022602652 crossref_primary_10_31857_S1234567823080037 crossref_primary_10_3390_photonics10101122 crossref_primary_10_1364_JOSAB_512362 |
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