journal article·2016-05

Isothermal crystallization and effect of soak time on phase evolution, microstructure and ionic conductivity of Li2O–Al2O3–TiO2–P2O5 glass–ceramic

Swati Soman, Dhiren Sonigra, Ajit R. Kulkarni

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Abstract

Glass–ceramics derived from Li 2O–Al 2O 3–TiO 2–P 2O 5 vitreous system were obtained by isothermal heat treatment at 700 °C, for different soak times ranging from 0 to 60 h. Phase analysis revealed mixture of amorphous and crystalline phases for short soak times (< 1 h). By 1 h of soak time, crystallization was complete and phases were ascribed to dominant Li 1 + xAl xTi 2 − x(PO 4) 3 (LATP) along with secondary AlPO 4 and TiO 2 , previously reported. Microstructural evolution with soak time was imaged using high resolution scanning electron microscope (SEM). Crystalline volume fraction in glass–ceramics was estimated from image analysis and it followed Kolmogorov–Johnson–Mehl–Avrami (KJMA) equation. Conductivity of glass–ceramics was derived using impedance spectroscopy data for all soak times and correlated to the crystalline volume content. After attaining a critical volume of crystalline phase/s, conductivity increased significantly and was observed to follow the scaling equation σ dc ~ (V − V c) β, where σ dc is dc conductivity, V is crystalline volume content, V c is threshold value of crystalline volume content above which sudden increase in conductivity was observed and β is scaling exponent. V c ≈ 30% was in accordance with percolation scaling law and is attributed to formation of 3D conducting channel network in the glass–ceramics microstructure.
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Research context

OpenAlex topics: Glass properties and applications · Advanced Battery Materials and Technologies · Recycling and utilization of industrial and municipal waste in materials production

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References (33)

Show source-provided references
1. Superionic conductivity of glass–ceramics in the system Li2O–Al2O3–TiO2–P2O510.1016/S0167-2738(97)00018-0 ↗
2. Ionic conductivity and sinterability of lithium titanium phosphate system10.1016/0167-2738(90)90282-V ↗
3. New solid ionic conductors10.1016/0025-5408(77)90161-1 ↗
4. Phase relationship and electrical conductivity of Li1+xTi2−xGaxP3O12 and Li1+2xTi2−xMgxP3O12 systems10.1016/0167-2738(86)90176-1 ↗
5. Lithium ion conductors based on LiTi2P3O12 compound10.1016/0167-2738(88)90291-3 ↗
6. Lithium ion conductors in the system AB(IV)2(PO4)3 (B=Ti, Zr and Hf)10.1016/0167-2738(86)90179-7 ↗
7. Ionic conductivity and crystal structure of Li1+xTi2−xInxP3O1210.1016/0167-2738(86)90183-9 ↗
8. Dependence of ionic conductivity on composition of fast ionic conductors Li1+xAlxTi2−x(PO4)3, 0≤x≤0.7. A parallel NMR and electric impedance study10.1021/cm010528i ↗
9. Ionic conductivity of solid electrolytes based on lithium titanium phosphate10.1149/1.2086597 ↗
10. Electrical properties of sintered lithium titanium phosphate ceramics (Li1+XMXTi2−X(PO4)3, M3+=Al3+, Sc3+, or Y3+)10.1246/cl.1990.1825 ↗
11. Ionic conductivity of the lithium titanium phosphate (Li1+x MxTi2-x(PO4)3, M=Al, Sc, Y and La) systems10.1149/1.2096693 ↗
12. High lithium ion conductivity glass–ceramics in Li2O–Al2O3–TiO2–P2O5 from nanoscaled glassy powders by mechanical milling10.1016/j.ssi.2006.04.010 ↗
13. Comparative study of lithium ion conductors in the system Li1+xAlxA2−xIV (PO4)3 with AIV=Ti or Ge and 0≤x≤0·7 for use as Li+ sensitive membranes10.1016/S0955-2219(99)00055-2 ↗
14. Conductivity measurements on nasicon and nasicon-modified materials10.1016/S0167-2738(99)00062-4 ↗
15. Fast Li+ ion conduction in Li2O–(Al2O3Ga2O3)–TiO2–P2O5 glass ceramics10.1023/A:1017559619391 ↗
16. Microstructural effects on the superionic conductivity of a lithiated glass–ceramic10.1016/j.ssi.2006.01.027 ↗
17. Microstructure and ionic conductivity of Li1+xAlxTi2−x(PO4) NASICON glass ceramics10.1016/j.ssi.2010.05.010 ↗
18. XPS and ionic conductivity studies on Li2O–Al2O3–(TiO2 or GeO2)–P2O5 glass–ceramics10.1016/S0167-2738(00)00500-2 ↗
19. Kingery · 1975
20. Effect of sintering time on the microstructure, flexural strength and translucency of lithium disilicate glass–ceramics10.1016/j.jnoncrysol.2012.11.010 ↗
21. Effect of heat treatment of the microsctructure and properties of lithium disilicate glass–ceramics10.1016/j.jnoncrysol.2014.05.023 ↗
22. Kinetics of phase formation in jarosite glass–ceramic10.1016/S0955-2219(98)00209-X ↗
23. Evaluation of the degree of crystallization in glass–ceramics by density measurements10.1016/S0955-2219(98)00226-X ↗
24. Grain boundary resistance of fast lithium ion conductors: Comparison between a lithium-ion conductive Li–Al–Ti–P–O type glass ceramic and a Li1.5Al0.5Ge1.5P3O12 ceramic10.1016/j.elecom.2011.10.022 ↗
25. Crystalline phase content and ionic conductivity correlation in LATP glass–ceramic10.1007/s10008-011-1592-4 ↗
26. A threshold selection method from gray level histogram10.1109/TSMC.1979.4310076 ↗
27. Kinetics of phase change. II. Transformation-time relations for random distribution of nuclei10.1063/1.1750631 ↗
28. Quantitative determination of crystal and amorphous phases in glass–ceramics by x-ray diffraction analysis
29. Kinetics of crystallization processes in glass forming melts10.1016/0022-0248(80)90270-5 ↗
30. Treatment of the impedance of mixed conductors — equivalent circuit model and explicit approximate solutions10.1149/1.1392611 ↗
31. Electroceramics: characterization by impedance spectroscopy10.1002/adma.19900020304 ↗
32. Percolation phenomena: a broad-brush introduction with some recent applications to porous media, liquid water and city growth10.1016/S0378-4371(99)00029-1 ↗
33. Electrical properties of glasses