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Structural Study of (1-x) (Bi0.5Na0.5) TiO3 -xLiNbO3 Solid-Ceramics


 

Bismuth sodium titante Lithium Niobate (1-x)(Bi0.5Na0.5)TiO3-xLiNbO3where (x=0.01,0.02,0.03)[BNTLN] which is a lead free antimony are prepared by conventional method of solid state reaction method. BNTLN samples are selected such that density about 95% of theoretical values. The phase formation was confirmed by X-ray diffraction (XRD). Bi0.5Na0.5TiO3 was investigated by XRD and Raman spectroscopy for phase formation and local structure. The density and grain size depend upon Li,Nb concentration and found propsanal to LiNbO3 concentration. In X-ray diffraction patterns the peak decreases with increase in LiNbO3. In Preliminary crystal-structure analysis shows the existence of phase transition from rhombhedral to a hexagonal structure.

A splitting of (TO3) mode at x=0.03. With increase in x change in peak position, width and intensity respectively has been noticed in Raman spectrum with increase in LiNbO3 concentration piezoelectric properties increase and found optimum at x=0.03.This optimum value is due to co-existence of two ferroelectric phases. Thus it is conducted that morphotropic phase boundary in (1-x )(Bi0.5Na0.5)TiO3-xLiNbO3  lies for composition x=0.03.


Keywords

Ceramics, X-ray diffraction, Raman spectroscopy
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  • Structural Study of (1-x) (Bi0.5Na0.5) TiO3 -xLiNbO3 Solid-Ceramics

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Abstract


Bismuth sodium titante Lithium Niobate (1-x)(Bi0.5Na0.5)TiO3-xLiNbO3where (x=0.01,0.02,0.03)[BNTLN] which is a lead free antimony are prepared by conventional method of solid state reaction method. BNTLN samples are selected such that density about 95% of theoretical values. The phase formation was confirmed by X-ray diffraction (XRD). Bi0.5Na0.5TiO3 was investigated by XRD and Raman spectroscopy for phase formation and local structure. The density and grain size depend upon Li,Nb concentration and found propsanal to LiNbO3 concentration. In X-ray diffraction patterns the peak decreases with increase in LiNbO3. In Preliminary crystal-structure analysis shows the existence of phase transition from rhombhedral to a hexagonal structure.

A splitting of (TO3) mode at x=0.03. With increase in x change in peak position, width and intensity respectively has been noticed in Raman spectrum with increase in LiNbO3 concentration piezoelectric properties increase and found optimum at x=0.03.This optimum value is due to co-existence of two ferroelectric phases. Thus it is conducted that morphotropic phase boundary in (1-x )(Bi0.5Na0.5)TiO3-xLiNbO3  lies for composition x=0.03.


Keywords


Ceramics, X-ray diffraction, Raman spectroscopy