• Chinese Optics Letters
  • Vol. 17, Issue 5, 051406 (2019)
Zhigang Zhao1、2、*, Kenta Kuroda1, Ayumi Harasawa1, Takeshi Kondo1, Shik Shin1, and Yohei Kobayashi1
Author Affiliations
  • 1The Institute for Solid State Physics, The University of Tokyo, Kashiwa, Chiba 277-8581, Japan
  • 2Current affiliation: School of Information Science and Engineering, Shandong University, Qingdao 266237, China
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    DOI: 10.3788/COL201917.051406 Cite this Article Set citation alerts
    Zhigang Zhao, Kenta Kuroda, Ayumi Harasawa, Takeshi Kondo, Shik Shin, Yohei Kobayashi. Monolithic LiF or MgF2 lens-window-prism device for coherent 10.7  eV beam source with 1 MHz repetition rate[J]. Chinese Optics Letters, 2019, 17(5): 051406 Copy Citation Text show less
    Schematic diagram of the “wedge-crystal”-like gas cell (lower part), integrated with the monolithic lens-window-prism (LPW) device. (a) A photograph of the custom-made LiF-LPW device. (b) The integrated flange that can be fixed onto the other end of the gas cell.
    Fig. 1. Schematic diagram of the “wedge-crystal”-like gas cell (lower part), integrated with the monolithic lens-window-prism (LPW) device. (a) A photograph of the custom-made LiF-LPW device. (b) The integrated flange that can be fixed onto the other end of the gas cell.
    Schematic diagram of the experimental setup for the generation of a 10.7 eV beam source. The input laser is from a homemade 347 nm femtosecond laser with a repetition rate of 1 MHz. (a) The previously obtained beam profile. (b) The beam profile obtained with the LWP device. Phototube: Hamamatsu Photonics R1187.
    Fig. 2. Schematic diagram of the experimental setup for the generation of a 10.7 eV beam source. The input laser is from a homemade 347 nm femtosecond laser with a repetition rate of 1 MHz. (a) The previously obtained beam profile. (b) The beam profile obtained with the LWP device. Phototube: Hamamatsu Photonics R1187.
    Beam profiles on the fluorescence plate taken with a CCD camera when different UV powers were used.
    Fig. 3. Beam profiles on the fluorescence plate taken with a CCD camera when different UV powers were used.
    Experimentally measured decay of the average powers using LiF-LWP and MgF2-LWP in vacuum conditions. The black lines are fitted results using exponential decay. For both cases, the normalized intensity 1.0 corresponds to a real power of 8 μW.
    Fig. 4. Experimentally measured decay of the average powers using LiF-LWP and MgF2-LWP in vacuum conditions. The black lines are fitted results using exponential decay. For both cases, the normalized intensity 1.0 corresponds to a real power of 8 μW.
    Average power of the 10.7 eV beam with the chamber filled with nitrogen. LiF-LWP was used here.
    Fig. 5. Average power of the 10.7 eV beam with the chamber filled with nitrogen. LiF-LWP was used here.
    Zhigang Zhao, Kenta Kuroda, Ayumi Harasawa, Takeshi Kondo, Shik Shin, Yohei Kobayashi. Monolithic LiF or MgF2 lens-window-prism device for coherent 10.7  eV beam source with 1 MHz repetition rate[J]. Chinese Optics Letters, 2019, 17(5): 051406
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