Liqiong An
Tohoku University
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Publication
Featured researches published by Liqiong An.
Optical Materials Express | 2014
Liqiong An; Akihiko Ito; Jian Zhang; Dingyuan Tang; Takashi Goto
Laser oscillation was demonstrated using a 1 at.% Nd3+-doped Lu2O3 (Nd3+:Lu2O3) transparent ceramic produced by spark plasma sintering. Nd2O3, Lu2O3, and LiF commercial powders were mixed by ball milling and were sintered at 1723 K using a two-step sintering profile. After the transparent Nd3+:Lu2O3 ceramic was annealed in air, its transmittance at 1076 nm reached 81.8%, which was close to the theoretical value for Lu2O3 (82.2%). The absorption cross-section at 806 nm was 1.29 × 10−20 cm2, and the fluorescence decay time at 1076 nm was 229 μs. The laser oscillation of Nd3+:Lu2O3 ceramic for the transition from 4F3/2 to 4I11/2—specifically, at 1076.7 and 1080.8 nm—was simultaneously obtained, with a laser output of 0.21 W and slope efficiency of 14%.
Journal of Asian Ceramic Societies | 2014
Liqiong An; Akihiko Ito; Takashi Goto
Abstract Transparent Nd-doped Lu2O3 bodies were fabricated by spark plasma sintering, and the effect of LiF addition on sintering, microstructure and transparency of Nd-doped Lu2O3 bodies were investigated. LiF promoted the densification at an early stage of sintering, resulted in high transparency of the Nd-doped Lu2O3 body. The optimal content of LiF was 0.2 wt% and that Nd-doped Lu2O3 body showed a transmittance of 81.8% (99.5% of theoretical) at 1080 nm after annealing in air for 21.6 ks.
IEEE Transactions on Nuclear Science | 2014
Shunsuke Kurosawa; Liqiong An; Akihiro Yamaji; Akira Suzuki; Yuui Yokota; Kenji Shirasaki; Tomoo Yamamura; Akihiko Ito; Takashi Goto; G. Boulon; Akira Yoshikawa
Nd<sup>3+</sup>-doped Lu<sub>2</sub>O<sub>3</sub> (Nd: Lu<sub>2</sub>O<sub>3</sub>) is a candidate for an infrared scintillator because (i) Lu<sub>2</sub>O<sub>3</sub> has a high density of 9.5 g/cm<sup>3</sup> and a high atomic number of 67 and (ii) Nd<sup>3+</sup>-doped materials emit in the infrared range and the emission lines from Nd<sup>3+</sup> can be used in medical applications since human body has a transparency window between 600 and 1,100 nm. However, it is extremely difficult to fabricate Lu<sub>2</sub>O<sub>3</sub> single crystals using conventional crystal growth methods because of the high melting point (2,510 <sup>°</sup> C). Using solid-state reactions, it is much easier to fabricate Lu<sub>2</sub>O<sub>3</sub> into a ceramic structure. Therefore, Nd: Lu<sub>2</sub>O<sub>3</sub> transparent ceramics were fabricated using a spark plasma sintering method. This technique is comparatively simple and consumes less time than other methods such as vacuum hot pressing. The scintillation properties and transmittance spectra of the as-produced ceramics were studied in both the visible and infrared regions. Radioluminescence spectra were measured in the range 800-1,200 nm. Nd<sup>3+</sup> emission lines were observed in the transparency window of human body. Thus, these ceramic materials could be a candidate for medical imaging applications.
IEEE Transactions on Nuclear Science | 2012
Akihiro Fukabori; Liqiong An; Akihiko Ito; Valery Chani; Kei Kamada; Takashi Goto; Akira Yoshikawa
Detailed scintillation properties of Sc<sub>2</sub>O<sub>3</sub>, especially γ-ray response, are not well studied because of low density and low effective atomic number of this compound. They are reported in this paper. Sc<sub>2</sub>O<sub>3</sub> single crystals grown by the micro-pulling-down method and Sc<sub>2</sub>O<sub>3</sub> translucent ceramics produced by the spark plasma sintering are analyzed. Optical, luminescence, and scintillation properties of these single- and poly-crystalline solids are discussed and compared based on examination of their optical transmittance, radio-luminescence spectra, light yields under γ-ray excitation, non-proportionality, energy resolution, and scintillation decay profiles. Spectrally corrected light yields of the Sc<sub>2</sub>O<sub>3</sub> single crystals and Sc<sub>2</sub>O<sub>3</sub> ceramics were approximately 7,700 and 19,200 photons/MeV, respectively.
Journal of the American Ceramic Society | 2011
Liqiong An; Akihiko Ito; Takashi Goto
Journal of The European Ceramic Society | 2012
Liqiong An; Akihiko Ito; Takashi Goto
Journal of The European Ceramic Society | 2011
Liqiong An; Akihiko Ito; Takashi Goto
Journal of The European Ceramic Society | 2011
Liqiong An; Akihiko Ito; Takashi Goto
Ceramics International | 2011
Liqiong An; Akihiko Ito; Takashi Goto
Journal of The European Ceramic Society | 2012
Liqiong An; Akihiko Ito; Takashi Goto