Please use this identifier to cite or link to this item: https://dspace.iiti.ac.in/handle/123456789/8277
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dc.contributor.authorPareek, Tanvien_US
dc.contributor.authorSen, Somadityaen_US
dc.contributor.authorKumar, Sunilen_US
dc.date.accessioned2022-03-17T01:00:00Z-
dc.date.accessioned2022-03-21T11:15:58Z-
dc.date.available2022-03-17T01:00:00Z-
dc.date.available2022-03-21T11:15:58Z-
dc.date.issued2018-
dc.identifier.citationPareek, T., Singh, B., Dwivedi, S., Yadav, A. K., Anita, Sen, S., . . . Kumar, S. (2018). Ionic conduction and vibrational characteristics of Al3+ modified monoclinic LiZr2(PO4)3. Electrochimica Acta, 263, 533-543. doi:10.1016/j.electacta.2018.01.087en_US
dc.identifier.issn0013-4686-
dc.identifier.otherEID(2-s2.0-85040745025)-
dc.identifier.urihttps://doi.org/10.1016/j.electacta.2018.01.087-
dc.identifier.urihttps://dspace.iiti.ac.in/handle/123456789/8277-
dc.description.abstractEffects of Al3+ substitution for Zr4+ in LiZr2(PO4)3 on its structure and lithium ion conduction are investigated. Li1+xZr2-xAlx(PO4)3 samples prepared via a sol-gel route and calcined at 900 °C crystallize in monoclinic structure with P21/n space group and show a reduction in cell volume with an increase in x. Raman spectra showed an increase in broadening of higher frequency v1 & v3 vibrational modes and a spectral weight transfer between v2 & v4 bending modes of PO4 tetrahedra with the increase in Al3+ doping. Analysis of Raman spectra further suggested that the renormalization of the mode frequencies in doped samples is controlled by Li-ion motion via strongly interacting with internal bending modes of PO4 tetrahedra. A significant improvement in ionic conductivity was observed in Al-doped samples, and the highest conductivity of 1.83 × 10−4 Ω−1m−1 and lithium diffusion coefficient of about 5.7 × 10−19 m2s−1 was observed for Li1.25Zr1.75Al0.25(PO4)3 at room temperature. Li transference number suggested that the conductivity in Li1.25Zr1.75Al0.25(PO4)3 is predominantly ionic. Activation energy was found to decrease from 0.58 eV for LiZr2(PO4)3 to 0.47 eV for Li1.25Zr1.75Al0.25(PO4)3. © 2018 Elsevier Ltden_US
dc.language.isoenen_US
dc.publisherElsevier Ltden_US
dc.sourceElectrochimica Actaen_US
dc.subjectActivation energyen_US
dc.subjectAluminumen_US
dc.subjectAluminum compoundsen_US
dc.subjectGeometryen_US
dc.subjectLithiumen_US
dc.subjectRaman scatteringen_US
dc.subjectRaman spectroscopyen_US
dc.subjectSol-gel processen_US
dc.subjectSol-gelsen_US
dc.subjectSolid electrolytesen_US
dc.subjectHigher frequenciesen_US
dc.subjectImpedance spectroscopyen_US
dc.subjectLithium ion conductionen_US
dc.subjectLiZr2(PO4)3en_US
dc.subjectMonoclinic structuresen_US
dc.subjectSol - Gel synthesisen_US
dc.subjectSpectral weight transferen_US
dc.subjectTransference numberen_US
dc.subjectZirconium compoundsen_US
dc.titleIonic conduction and vibrational characteristics of Al3+ modified monoclinic LiZr2(PO4)3en_US
dc.typeJournal Articleen_US
Appears in Collections:Department of Physics

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