TY - JOUR
T1 - Effect of point defects on Curie temperature of lithium niobate
AU - Koyama, Chihiro
AU - Nozawa, Jun
AU - Fujiwara, Kozo
AU - Uda, Satoshi
N1 - Funding Information:
This work was supported in part by JSPS KAKENHI grant no. 24360002 and by the Global COE Program “Materials Integration (International Center of Education 392 and Research), Tohoku University,” of the Ministry of Education, Culture, Sports, Science and Technology (MEXT) of Japan.
Publisher Copyright:
© 2016 The American Ceramic Society
PY - 2017/3/1
Y1 - 2017/3/1
N2 - The effect of point defects on the Curie temperature (Tc) of LiNbO3 (LN) was investigated by combining Tc measurements with an analysis of the defect structures of LN doped with impurities having various valences. The data show that Tc of congruent LN increases with the impurity concentration up to around 3 and 2 mol% for divalent and trivalent impurities, respectively, whereas it decreases continuously with increased concentrations of tetravalent impurities. These Tc variations were examined with respect to the defect structures of impurity-doped LN, which are expressed in the form chemical formulae using Kröger-Vink notation. The defect structures of divalent and trivalent impurity-doped LN are (Formula presented.) and (Formula presented.), respectively (NbLi: Nb at Li sites; VL i: vacancies at Li sites, ML i: impurities at Li sites, and Li/Nb = the congruent ratio). The defect structure in the case of tetravalent impurities is (Formula presented.). Analyses of the defect structures indicated that the NbLi concentration decreases with divalent or trivalent impurity doping, which increases Tc. In contrast, the NbLi concentration increases with tetravalent impurity doping, which decreases Tc. In addition, the divalent or trivalent impurity concentrations at which the NbLi concentration becomes zero were found to correspond to the concentrations at which Tc is maximized, suggesting that Tc of LN depends on the NbLi concentration.
AB - The effect of point defects on the Curie temperature (Tc) of LiNbO3 (LN) was investigated by combining Tc measurements with an analysis of the defect structures of LN doped with impurities having various valences. The data show that Tc of congruent LN increases with the impurity concentration up to around 3 and 2 mol% for divalent and trivalent impurities, respectively, whereas it decreases continuously with increased concentrations of tetravalent impurities. These Tc variations were examined with respect to the defect structures of impurity-doped LN, which are expressed in the form chemical formulae using Kröger-Vink notation. The defect structures of divalent and trivalent impurity-doped LN are (Formula presented.) and (Formula presented.), respectively (NbLi: Nb at Li sites; VL i: vacancies at Li sites, ML i: impurities at Li sites, and Li/Nb = the congruent ratio). The defect structure in the case of tetravalent impurities is (Formula presented.). Analyses of the defect structures indicated that the NbLi concentration decreases with divalent or trivalent impurity doping, which increases Tc. In contrast, the NbLi concentration increases with tetravalent impurity doping, which decreases Tc. In addition, the divalent or trivalent impurity concentrations at which the NbLi concentration becomes zero were found to correspond to the concentrations at which Tc is maximized, suggesting that Tc of LN depends on the NbLi concentration.
KW - Curie temperature
KW - defects
KW - ferroelectricity/ferroelectric materials
KW - lithium niobate
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U2 - 10.1111/jace.14701
DO - 10.1111/jace.14701
M3 - Article
AN - SCOPUS:85007623448
SN - 0002-7820
VL - 100
SP - 1118
EP - 1124
JO - Journal of the American Ceramic Society
JF - Journal of the American Ceramic Society
IS - 3
ER -