Atomic structure of undoped Σ = 5 symmetrical tilt grain boundary in strontium titanate

1993 ◽  
Vol 52 (3-4) ◽  
pp. 557-563 ◽  
Author(s):  
V. Ravikumar ◽  
Vinayak P. Dravid
Author(s):  
V. Ravikumar

Strontium titanate is an important electroceramic material which, under appropriate processing and dopant additions exhibits both varistor and Grain Boundary Layer Capacitor (GBLC) behavior. The presence of electrically active grain boundaries is essential for obtaining these properties. The first step towards correlating the grain boundary structure to properties is to determine the detailed atomic structure of the boundary, which includes its geometric structure, chemistry and electronic structure. We present here our TEM investigation of the atomic structure of an undoped (“pristine”) symmetrical tilt grain boundary in SrTiO3. This provides the basic reference structure, changes to which can be studied as a function of doping and/or processing parameters, and correlated to electrical and dielectric properties.Self-supported TEM samples were made from bicrystals of SrTiO3 through the conventional sample preparation route. Fig. 1 shows a high resolution electron micrograph (Hitachi H9000) of a representative grain boundary region in the sample.


Author(s):  
V. Ravikumar ◽  
Vinayak. P. Dravid ◽  
D. Wolf

Strontium Titanate is a prototypical perovskite oxide whose macroscopic electroceramic properties, like varistor and grain boundary barrier layer capacitor (GBBLC) behavior, are controlled by grain boundary (GB) phenomena. In this paper, we present a comparative analysis of the results of both experimental and theoretical investigations of the atomic structure of a (310) symmetrical tilt GB (a Σ=5 (310) [001] GB in the CSL notation) in SrTiO3. Bicrystals of SrTiO3 were procured from Shinkosha Ltd., and electron backscatter kikuchi pattern analysis as well as transmission electron diffraction studies confirm that the GB conforms to the Σ =5 misorientation. The atomic structure of this GB has been investigated using high resolution transmission electron microscopy (HRTEM) and associated image simulations, as well as by atomistic simulations using static iterative energy minimization schemes (“lattice-statics”).2


2011 ◽  
Vol 46 (12) ◽  
pp. 4162-4168 ◽  
Author(s):  
T. Mitsuma ◽  
T. Tohei ◽  
N. Shibata ◽  
T. Mizoguchi ◽  
T. Yamamoto ◽  
...  

2013 ◽  
Vol 97 (2) ◽  
pp. 617-621 ◽  
Author(s):  
Ji-Young Roh ◽  
Yukio Sato ◽  
Yuichi Ikuhara

2013 ◽  
Vol 48 (16) ◽  
pp. 5470-5474 ◽  
Author(s):  
Mitsuhiro Saito ◽  
Zhongchang Wang ◽  
Susumu Tsukimoto ◽  
Yuichi Ikuhara

2004 ◽  
Vol 10 (S02) ◽  
pp. 282-283
Author(s):  
Gunther Richter ◽  
Steffen Schmidt ◽  
Wilfried Sigle ◽  
Manfred Rühle

Extended abstract of a paper presented at Microscopy and Microanalysis 2004 in Savannah, Georgia, USA, August 1–5, 2004.


1990 ◽  
Vol 5 (11) ◽  
pp. 2658-2662 ◽  
Author(s):  
William Krakow

An electron microscope structure image of a σ = 21/[111] tilt grain boundary in Au was obtained and atomic column positions identified to yield a structural unit model of the interface consisting of repeating polyhedron shapes. This result represents the smallest projected spacings at a grain boundary containing defect structures imaged by an electron microscope and interpreted atomistically.


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