Abstract
Achieving high ion conductivity in glass-based Na-ion conducting materials for their applications as solid electrolytes in batteries is still challenging owing to the vague knowledge on the factors governing Na-ion dynamics. In the present study, an attempt has been made to identify the factors affecting the sodium-ion dynamics through structure and conductivity property correlation for the 37.5Na2O-37.5P2O5-15Al2O3-10NaF (FS-0; mol %) glass system with varied concentrations of Na2SO431P, 27Al, and 23Na MAS NMR (magic-angle spinning nuclear magnetic resonance) and Raman spectroscopy are employed to assess the structural modifications, and impedance spectroscopy is used to measure the variations in ionic conductivity on the addition of Na2SO4 in the FS-0 glass. Raman spectra and MAS NMR analysis indicate that the quantity of P-O-Na bonds and sulfate (SO42-) units surrounded by sodium increase with increasing Na2SO4 concentration. Impedance analysis reveals that the conductivity of FS-0 glass enhances by 1 order with the addition of 6 mol % Na2SO4. We identify from the ac-conductivity spectral analysis that the concentration of charge carriers and the critical hopping length of mobile cations increase with the addition of 6 mol % Na2SO4. Overall, we reveal that the structural modifications, Na-ion concentration, and the shallower potential well that is created for sodium due to its interaction with the nearest neighboring cations affect the Na-ion dynamics. The information obtained from the present study certainly helps to optimize the chemical composition of glasses demonstrating high ionic conductivity.
Original language | English |
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Pages (from-to) | 3276-3288 |
Number of pages | 13 |
Journal | Journal of Physical Chemistry C |
Volume | 126 |
Issue number | 6 |
DOIs | |
State | Published - Feb 17 2022 |
Funding
The authors thank Dr. Suman Kumari Mishra, Director, CSIR-CGCRI, for her continuous support and encouragement. This work was developed under the frame of the project funded by the Science and Engineering Research Board (SERB), DST, Govt. of India, India, through the Early Career Research Award (ECR/2018/000292). I.M. and A.R.A. acknowledge the financial support by DST-SERB (ECR/2018/000292). M.G. acknowledges the financial support of IoE-BHU (grant number R/Dev/D/IoE/Seed Grant-II/2021-22/39944). The authors acknowledge the solid-state NMR facility of the Sophisticated Instrument Center (SIC) of Dr. Harisingh Gour University, India.