TY - JOUR
T1 - Combined effect of rattling and compression on the microwave dielectric properties of B-site 1:3 ordered Li6A7Ti11O32 (A = Zn, Mg) spinels
AU - Li, Mu
AU - Tang, Ying
AU - Xiang, Huaicheng
AU - Li, Jie
AU - Zhou, Di
AU - Fang, Liang
N1 - Publisher Copyright:
© 2022 Elsevier Ltd and Techna Group S.r.l.
PY - 2023/3/15
Y1 - 2023/3/15
N2 - Dense ceramics of two B-site 1:3 ordering spinels Li6A7Ti11O32 (A = Zn, Mg) with space group P4332 were prepared by solid-state reaction. Raman spectroscopy and XRD analysis revealed why the lattice parameters and volume of Li6Mg7Ti11O32 are abnormally greater than those of Li6Zn7Ti11O32. Li6Zn7Ti11O32 exhibits outstanding microwave dielectric properties (Q × f = 129,600 GHz (8.9 GHz), εr = 20.7, τf = −45 ppm/°C) and a low thermal expansion coefficient (αL) of 5.5 ppm/°C. While Mg-analogue displayed a lower Q × f ∼108,600 GHz (9.1 GHz), a lower αL ∼ 4.9 ppm/°C, a higher εr ∼ 21.9, and a slightly positive offset τf ∼ −21 ppm/°C relative to Li6Zn7Ti11O32. A significant positive deviation of 91.6% was observed between the corrected εr(corr) by the porosity and the calculated εr(C-M) by the Clausius-Mosotti (C-M) equation in the Li1.33xA2-2xTi1+0.67xO4 solid solution. The variation in εr and τf values of Li6A7Ti11O32 (x = 0.5625) compared to Li2ATi3O8 (x = 0.75) might be attributed to the combined effect of rattling and compression cations at A-site and B-site. Moreover, the negative τf of Li6A7Ti11O32 (A = Zn, Mg) ceramics was balanced to near zero by adding CaTiO3.
AB - Dense ceramics of two B-site 1:3 ordering spinels Li6A7Ti11O32 (A = Zn, Mg) with space group P4332 were prepared by solid-state reaction. Raman spectroscopy and XRD analysis revealed why the lattice parameters and volume of Li6Mg7Ti11O32 are abnormally greater than those of Li6Zn7Ti11O32. Li6Zn7Ti11O32 exhibits outstanding microwave dielectric properties (Q × f = 129,600 GHz (8.9 GHz), εr = 20.7, τf = −45 ppm/°C) and a low thermal expansion coefficient (αL) of 5.5 ppm/°C. While Mg-analogue displayed a lower Q × f ∼108,600 GHz (9.1 GHz), a lower αL ∼ 4.9 ppm/°C, a higher εr ∼ 21.9, and a slightly positive offset τf ∼ −21 ppm/°C relative to Li6Zn7Ti11O32. A significant positive deviation of 91.6% was observed between the corrected εr(corr) by the porosity and the calculated εr(C-M) by the Clausius-Mosotti (C-M) equation in the Li1.33xA2-2xTi1+0.67xO4 solid solution. The variation in εr and τf values of Li6A7Ti11O32 (x = 0.5625) compared to Li2ATi3O8 (x = 0.75) might be attributed to the combined effect of rattling and compression cations at A-site and B-site. Moreover, the negative τf of Li6A7Ti11O32 (A = Zn, Mg) ceramics was balanced to near zero by adding CaTiO3.
KW - Cation ordering
KW - Microwave dielectric properties
KW - Rattling and compressed effects
KW - Spinel structure
UR - https://www.scopus.com/pages/publications/85142004675
U2 - 10.1016/j.ceramint.2022.11.021
DO - 10.1016/j.ceramint.2022.11.021
M3 - 文章
AN - SCOPUS:85142004675
SN - 0272-8842
VL - 49
SP - 8754
EP - 8761
JO - Ceramics International
JF - Ceramics International
IS - 6
ER -