TY - JOUR
T1 - Control of the solid-liquid interface during growth of a Ce-doped Gd2Si2O7 crystal by the traveling solvent floating zone method
AU - Watauchi, Satoshi
AU - Matsuya, Kohei
AU - Nagao, Masanori
AU - Tanaka, Isao
AU - Kurosawa, Shunsuke
AU - Yokota, Yuui
AU - Yoshikawa, Akira
N1 - Funding Information:
This work was partly performed under the Inter-University Cooperative Research Program of the Institute for Materials Research, Tohoku University (Proposal No. 15K0034) and Grant-in-Aid for Scientific Research(C) by JSPS (Grant Number JP26410236).
Publisher Copyright:
© 2016
PY - 2017/6/15
Y1 - 2017/6/15
N2 - The growth conditions of Ce-doped Gd2Si2O7 crystals, using the infrared convergent heating floating zone method, were optimized to make the shape of the crystal-melt interface flat or convex. The shape of the crystal-melt interface, meaning the interface between the molten zone and the grown crystal, was evaluated quantitatively using the convexity (h/r) as a parameter. The h/r value was found to be systematically dependent on the crystal diameter, the focus position of the ellipsoidal mirror for infrared convergent heating, and the lamp power used during crystal growth. For an 8.2-mm-diameter crystal grown using conventional conditions, the h/r value was −0.8, which indicates that the crystal-melt interface had a concave shape. The h/r value increased with the position of the ellipsoidal mirror, going from −0.8 for the −8 mm mirror position, to −0.5 for the +6 mm mirror position. Lastly, when the lamp power increased from 5.8 to 7.0 kW, the h/r value increased from −0.6 to −0.3, which was the maximum value observed, indicating that a flat or convex crystal-melt interface was not obtained.
AB - The growth conditions of Ce-doped Gd2Si2O7 crystals, using the infrared convergent heating floating zone method, were optimized to make the shape of the crystal-melt interface flat or convex. The shape of the crystal-melt interface, meaning the interface between the molten zone and the grown crystal, was evaluated quantitatively using the convexity (h/r) as a parameter. The h/r value was found to be systematically dependent on the crystal diameter, the focus position of the ellipsoidal mirror for infrared convergent heating, and the lamp power used during crystal growth. For an 8.2-mm-diameter crystal grown using conventional conditions, the h/r value was −0.8, which indicates that the crystal-melt interface had a concave shape. The h/r value increased with the position of the ellipsoidal mirror, going from −0.8 for the −8 mm mirror position, to −0.5 for the +6 mm mirror position. Lastly, when the lamp power increased from 5.8 to 7.0 kW, the h/r value increased from −0.6 to −0.3, which was the maximum value observed, indicating that a flat or convex crystal-melt interface was not obtained.
KW - A1. Interfaces
KW - A2. Floating zone technique
KW - A2. Growth from melt
KW - B2. Oxides
KW - B2. Scintillator materials
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U2 - 10.1016/j.jcrysgro.2016.11.018
DO - 10.1016/j.jcrysgro.2016.11.018
M3 - Article
AN - SCOPUS:85006994712
VL - 468
SP - 465
EP - 468
JO - Journal of Crystal Growth
JF - Journal of Crystal Growth
SN - 0022-0248
ER -