Back to Search Start Over

Thickness Effect on (La0.26Bi0.74)2Ti4O11 Thin-Film Composition and Electrical Properties.

Authors :
Hui-Zhen Guo
An-Quan Jiang
Source :
Chinese Physics Letters; Feb2018, Vol. 35 Issue 2, p1-1, 1p
Publication Year :
2018

Abstract

Highly oriented (00l) (La<subscript>0</subscript>.26Bi<subscript>0.74</subscript>)2Ti<subscript>4</subscript>O<subscript>11</subscript> thin films are deposited on (100) SrTiO<subscript>3</subscript> substrates using the pulsed laser deposition technique. The grains form a texture of bar-like arrays along SrTiO<subscript>3</subscript> ⟨110⟩ directions for the film thickness above 350 nm, in contrast to spherical grains for the reduced film thickness below 220 nm. X-ray diffraction patterns show that the highly ordered bar-like grains are the ensemble of two lattice-matched monoclinic (La,Bi)<subscript>4</subscript>Ti<subscript>3</subscript>O<subscript>12</subscript> and TiO<subscript>2</subscript> components above a critical film thickness. Otherwise, the phase decomposes into the random mixture of Bi<subscript>2</subscript>Ti<subscript>2</subscript>O<subscript>7</subscript> and Bi<subscript>4</subscript>Ti<subscript>3</subscript>O<subscript>4</subscript> spherical grains in thinner films. The critical thickness can increase up to 440 nm as the films are deposited on LaNiO<subscript>3</subscript>-buffered SrTiO<subscript>3</subscript> substrates. The electrical measurements show the dielectric enhancement of the multi-components, and comprehensive charge injection into interfacial traps between (La,Bi)<subscript>4</subscript>Ti<subscript>3</subscript>O<subscript>12</subscript> and TiO<subscript>2</subscript> components occurs under the application of a threshold voltage for the realization of high-charge storage. [ABSTRACT FROM AUTHOR]

Details

Language :
English
ISSN :
0256307X
Volume :
35
Issue :
2
Database :
Complementary Index
Journal :
Chinese Physics Letters
Publication Type :
Academic Journal
Accession number :
127944411
Full Text :
https://doi.org/10.1088/0256-307X/35/2/026801