90° Phase-Matching Properties of YCa<sub>4</sub>O(BO<sub>3</sub>)<sub>3</sub> and Gd<sub>x</sub>Y<sub>1-x</sub>Ca<sub>4</sub>O(BO<sub>3</sub>)<sub>3</sub>

  • Umemura Nobuhiro
    Department of Electronic Engineering, Osaka Institute of Technology, 5-16-1, Ohmiya, Asahi-ku, Osaka 535-8585, Japan
  • Nakao Hiroshi
    Department of Electrical Engineering, Osaka University, 2-1 Yamadaoka, Suita, Osaka 560-0871, Japan
  • Furuya Hiroyuki
    Department of Electrical Engineering, Osaka University, 2-1 Yamadaoka, Suita, Osaka 560-0871, Japan
  • Yoshimura Masashi
    Department of Electrical Engineering, Osaka University, 2-1 Yamadaoka, Suita, Osaka 560-0871, Japan
  • Mori Yusuke
    Department of Electrical Engineering, Osaka University, 2-1 Yamadaoka, Suita, Osaka 560-0871, Japan
  • Sasaki Takatomo
    Department of Electrical Engineering, Osaka University, 2-1 Yamadaoka, Suita, Osaka 560-0871, Japan
  • Yoshida Kunio
    Department of Electronic Engineering, Osaka Institute of Technology, 5-16-1, Ohmiya, Asahi-ku, Osaka 535-8585, Japan
  • Kato Kiyoshi
    Faculty of Photonics Science, Chitose Institute of Science and Technology, Bibi 758-65, Chitose, Hokkaido 066-0027, Japan

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タイトル別名
  • 90.DEG. Phase-Matching Properties of YCa4O(BO3)3 and GdxY1-xCa4O(BO3)3.

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説明

YCa4O(BO3)3 has been found to be 90º phase-matchable for type-1 second-harmonic generation at 0.4168 μm along the z-axis at 20°C. The improved Sellmeier equations of YCa4O(BO3)3 that correctly reproduce our new experimental data for second-harmonic and sum-frequency generation in the 0.3547-1.9079 μm range are reported. In addition, the 90º phase-matching properties of GdxY1-xCa4O(BO3)3 as a function of the Gd molar concentration X are presented together with the empirical index formula.

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